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ORSAY
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THE8E
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DOCTORAT
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SS-SCIENCES
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PAlSENTII A L'UNIVERSITE DE
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POUR
08TENIR
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GRAJ)B
DE
DOCTEUR
ES-SCIENCES
SYSTEMATIQUE DE LA PHOTOIONISATION ET DE LA
RECOMBINAISON RADIATIYE DANS LES SEQUtNCES
ISOELECTROHIQUES OU POTASSIU"
DU RUBIDIUM,
i
.1
DU CUIVRE ET DE L'ARGENT.
i1,
1
1
l
1
,
SOUTENue LE 15 ~tel' , . DEYANT LA COMMISSION D'eXAMEN
M• .
S. llBERMAN
PT4.ideaC
M_e
". AYMAR
MH.
3. BAUCHE
A. BES.ICK
.',
H_e
A. CIUSTI
"H.
A. HAQUET
s. NIANC
TITLE
SYSTEMATIC TRENDS Of PHOTO IONISATION AND RADIATIVE
RECOMBINATION fOR THE POTASSIUM, RUBIDIUM, COPPER
AND SIL VER ISOELECTRONIC SEQUENCES
ABSTRACT
In
the
framework
of a
non-relativistic
single elec-
tron
model,
photoionisation
cross
sections
from
ground
and
excited nR. states
have
been computed
for
the K,
Rb,
Cu and
Ag
isoelectronic sequences,
by the use of a parametric cen-
tral potential.
The evolution of the non-hydrogenic behaviour of pho-
toionisation cross sections near
threshold is studied along
Rydberg
series
and
along
the
isoelectronic
sequences,
and
emphasis
is
put
on
the
occurrence
of minima
and
maxima
in
the photoionisation cross section curves.
5ystematic trends
along
an
isoelectronic
sequence
and
in
addition
along
the
sequence of neutral alkali atoms Li through Cs, and the com-
parison
of the
behaviour
along the different K,
Rb,
Cu and
Ag
isoelectornic
sequences
are
analysed
in
terms
of
the
quantum defect theory.
Through the principle of the detailed balance radia-
tive
recombination
rate
coefficients
have
been
obtained
along the isoelectronic sequences,
rather for relatively low
temperatures.
Markedly
and
peculiar non-hydrogenic features
are outlined and the systematics of recombination along the
isoelectronic sequences are analysed.
Comparisons
for
both
photoionisation
and
recombina-
tion
results
are
made
with
mainly
those
of
the
hydrogenic
model,
and with other available theoretical or experimental
results.
LAB1E DES MATIERES
INTRODUCT ION
.
CHAPITRE 1 : RAPPELS THEORIQUES CONCERNANT LA PHOTOIONI-
SATION ATOMIQUE ET LA RECOMBINAISON RADIA-
lIVE.... ..
.. .. .. .. . .. . .
. .
. ..
6
A. PHOTOIONISATION DES ATOMES ET DES IONS ...........•.....
7
1. Définitions. Formules générales . . . . . . • . . . . . . . . . . . . . .
7
1)
Grandeurs caractéristiques de la photoionisation.
8
2)
Expression de la section efficace
de photoioni-
sation
10
2.1)
Formule générale
11
2.2)
2.3)
II. Modèle
1)
1 .1)
Hypothèsesde
1.2) Expression de la sectio~ efficace dans le
mo d è 1 e à un
1 e c t r
é
0 n . . . . . . . . . . . . . . . . . . . . . ..
19
1.3) Expression générale de la section efficace.
21
2)
Différents modèles à particules indépendantes
non relativistes...............
22
2.1) Modèles à champ central . . . . . . . . . . . . . . . . • . . •
22
2 . 1 . 1) Mo d 1e h yd r
è
0 gé n 0 Ide. . . • . . . . . . . . . . . ..
23
a) Comportement hydrogénolde et lois
d'échelle
24
b) Validité et limites . . . . • . . . . . . . . . . . .
24
c) Modèle de Kramers et approximation
de Kramers-Gaunt . . . . . . . . . . . . . . . • . • . .
26
2.1.2) Méthode
du défaut quantique
26
1$
2 . 1 . 3) Pot en t i e l s ce n t ra u x par a mé tri que s • ..
29
2.1.4) Potentiels semi-empiriques avec
effets de polarisation du coeur .....
31
2.1. 5) Potentiels centraux ab-initio.......
32
2.2) Le modèle Hartree-Fock •.••••..•......••••..
33
3) Modèles à particules indépendantes incluant des
e f f e t s rel a t i vis tes. . • • • . • • . • . . • . . • . . . . • . • . • • • •.
34
3.1) Traitement approché des effets relativis-
tes : m0 dè le" sem i - rel a t i vis te" . . . . . • . . • . •.
34
3.2) Modèle relativiste à champ centraL •••.••..
35
3.3) Méthode de Dirac-Fock .•.•..•.•..•••.••.•..•
35
III. Modèles au-delà du modèle à particules indépen-
dantes
36
IV. Résultats antérieurs concernant les études systéma-
tiques de9 caractères non hydrogénoldes de la
photoionisation • . . . . . . . . . • . . • • . • . . . . . . . . . . . . . • . . . . .
37
B. RECOMBINAISON RADIATIVE DES ATOMES ET DES IONS ......•..
41
1. Définitions -
Formules générales ...•......•...•.....
41
1)
Définitions
41
2) Exp r e s s ion s 9 n r ale s . . . . . . • • . . . • . . . • . • . . . • . • . . ..
43
é
é
II. Modèles théoriques.. . . . . • .. .. . . . .• . . . . . .. . . . . . .. . . . ..
44
1) M0 dè l e h ydr 0 g n
é
0 ï de. • . . . • . • • . • . • • • . . • • • . . . • • . . •.
44
1 • 1) Cal cul e xa ct. Loi s hYd r 0 9 n
é
0 r des. . • . • . • . . •.
44
1.2) Modèle de Kramers et approximation de
Kramers-Gaunt.. .... ........ .. ...... .. .. .. ...... .. .. .. .. ...... .. .. .. ......
45
2) Autres modèles théoriques ••..•....•.•.••..•••...
46
III. Résultats antérieurs obtenus pour la recombinaison
radiative des atomes et des ions ..••••••.••....•••
47
CHAPITRE II : PHOTOIONISATION ET RECOMBINAISON RADIATIVE
DANS LES SEQUENCES ISOELECTRONIQUES OU
POTASSIUM, OU RUBIDIUM, DU CUIVRE ET DE
l'ARGENT.. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. .. ....
49
A. PHOTOIONISATION DANS LES SEQUENCES ISOELECTRONIQUES DU
POTASSIUM, DU RUBIDIUM, DU CUIVRE ET DE L'ARGENT. ...•.•
51
1. Modèle théorique utilisé pour le calcul des sections
efficaces de photoionisation .••.•.•....•••..•.••.•..
52
II. Analyse de la photoionisation des états excités par
la théorie du défaut quantique
54
1) Comportement non hydrogénolde des courbes de
sec t ion s e f fic ace s . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..
54
1. 1) C0 mpar ais 0 n s a ve c l ' h Yd r 0 g è ne. . . . . . . . . . . . . . . ..
54
1.2) Evolution le long d'une série de Rydberg......
56
1.3) Variation le long d'une séquence
56
2)
Analyse du comportement non hydrogénolde des
sections efficaces
60
III. Présentation globale des résultats . . . . . . . . • . . . . . . . .
63
1) Evolution avec n le long d'une série de Rydberg
d'un élément donné . • . . . . . . . . . . . . . . . . . . . . . . . . . . . .
64
2) Séquence des alcalins Li-Cs
66
3) Evolution le long d'une séquence isoélectronique
Comparaison des séquences de K, Rb,
Cu et Ag....
69
3.1) Variation isoélectronique des défauts
quantiques asymptotiques et de leurs
d i f f é r e n ces. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..
69
3.2) Systématique de la photoionisation
.
73
3.2.1) Etats n s ••••••••••••••••••••••••••••
73
3.2.2) Etats n d ••••.•••••••••..••••••••••••
73
3.2.3) Etats n f ................•...........
76
3.3) Discussion
78
IV. Discussion critique des résultats obtenus
.
79
v. Calculs relativistes
.
85
1) Modèle relativiste à champ central . . . . . . . . . . . . • • . .
85
2)
Sections efficaces
87
3) Méthode de calculs et résultats
88
B. RECOMBINAISON RADIATIVE DANS LES SEQUENCES ISOELECTRO-
NIQUES DU POTASSIUM, DU RUBIDIUM, DU CUIVRE ET DE
LIA RGENT. • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • ••
90
1. Modèle théorique utilisé pour le calcul des sec-
tions efficaces de capture et des coefficients de
r e c 0 mb i nais 0 n rad i a t ive • . . . . . . . . . . • . . . . . . • . . . . . . . . ..
90
II.
Résultats . . . • . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
91
1) Variation de a~l(T') en fonction de n , l e t T'
étant
fixés
92
a) a~l < a~l···············.···················· 92
,
b)
Evolution avec n présentant un maximum
96
c ) Evolution avec n présentant un minimum
96
d ) Cl. ~ fl, > Cl. ~ fl, • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • ••
96
2)
Variation de Cl.~fl,(TI) en fonction de T', n et fl,
étant
fixés
97
3) Var i a t ion de Cl. ~ fl, ( T ,) a ve c fl"
net T'
tan t
f i x
é
é s 100
CONCLUSION . . . . . . . . . . . . • . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 104
REfERENCES . . . . . . . . . . . . . . • . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 110
ART ICLES PRESENTES . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . • 118
ANNEXE 1
Aymar M., Robaux O. and Wane S. 1984 J. Phys. 8:
At. Mol.
Phys.
17 993-1007
"Central-field calculations of photoionisation
cross-sections of excited states of Rb and sr+
and analysis of photoionisation cross-sections
of excited alkali atoms using quantum defect
the 0 r y l' • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •
ANNEXE II
Wane S. 1985 J. Phys. 8 : At. Mol. Phys. 18
3881-93
"Radiative recombination in Rubidium"
.
ANNEXE III
Wane S. and Aymar M. 1987 J. Phys. B A t .
Mol.
Phys. lQ 2657-75
"Excited-state photoionisation and radiative
recombination for ions of the potassium iso-
electronic sequence"
.
ANNEXE IV
Wane S. and Aymar M. 1987 J.
Phys. B : At.
Mol. Phys. 1Q 4425-40
"Photoionisation and radiative recombination
for the Rubidium,
Copper and Sil ver isoelec-
tronic sequences"
.
APPENDICE (fascicule séparé) .....•..........•.•...•.••••.•
Tables
donnant
les
défauts
quantiques,
les
Lémerrt s
de
ma-
é
tri ce
di pol ai res et
les
sect ions
e f fi caces
de
photo ioni sa-
tion,
partielles
et
totales,
pour
les
divers
éléments
des
séquences isoélectroniques de K,
Rb,
Cu et Ag.
Ce t~ava~l a été ~éal~~é au Labo~ato~~e A~mé Cotton.
Je do~~ a Mon~~eu~ S. FENEUILLE, anc~en d~~ecteu~, d'y avo~~
été
accue~ll~ et à. .6on .6ucce~.6eu~,
Mon~~eu~
S.
LIBERMAN,
d av oL« pu y pou~~u~v~e
le t~ava~l déj a ent~ep~~.6. Qu
ï
1 ~1.6
t~ouvent ~c~ l'e~p~e.6~~on de me.6 v~6~ ~eme~c~ement.6.
Je ~u~~ pa~t~cul~è~ement heu~eux. d' ex.p~~me~ ma pno-
6onde ~econna~.6.6ance a Mon.6~eu~ S. LI BERMAN pou~ l' ~nté~ê.t
con~tant qu'~l a po~té a ce t~ava~l, pou~ .6a d~.6pon~b~l~té
et le~ nomb~eu.6e.6 d~~cu.6.6~on.6 .6t~mulante~ que j'a~ eue~ avec
lu~. Se.6 encou~agement.6,
.6on .6out~en et .6on a~de p~éc~eu~e
m'ont pe~m~.6 de mene~ a b~en cette étude dan.6 le.6 me~lleu~e.6
cond~t~on.6 pO~.6~ble~.
Je
t~en~ tout
~péc~alement a ex.p~~me~
ma.
p~o6onde
g~at~tude
a Madame M. AYMAR qu~ m'a con6~é le .6ujet de ce
t~ava~l,
et m'a d~~~gé tout au long avec beaucoup d'atten-
t~on. J'a~ béné6~c~é de .6on ex.pé~~ence et de .6a p~o6onde
conna~.6~ance
de la phY.6~que, de .6on e.6p~~t de d~.6ce~nement
et de
.6a g~ande
~~gueu~.
Je la ~eme~c~e t~è.6 .6~ncè~ement
pou~ .6on a.Lâe ,
.6e~
encou~agement.6,
.6e~ .6ugge.6t~on.6 et .6e.6
c~~t~que.6,
et pou~ tout ce qu'elle m'a app~~~.
J' a~ beaucoup app~éc~é l' acâe. géné~eu.6e et e6 6~cace
de Madame E. LUC et de Madame O. ROBAUX. Le~ nomb~eu.6e~ d~.6­
cU.6.6~on.6 que j'a~ eue.6 avec elle.6 m'ont été ex.t~èmement p~o­
6~table.6. Je le~ ~eme~c~e t~è.6 .6~ncè~ement de leu~ d~~pon~­
b~l~té et de la pa~t déte~m~nante qu'elle.6 ont p~~.6e dan.6
cette étude.
L'attent~on pa~t~cul~è~e
acco~dée
a ce t~ava~l pa~
Mon~~eu~ J. BAUCHE m'a p~o6ondément touché. Je lu~ .6U~.6 t~è.6
~econna~.6.6ant de .6on ~out~en,
de ~e.6 con~e~l~ et de ~e.6 ~ug­
ge~t~on~.
J~ ~~m~~e~~ Mon~~~u~ "A. BESWICK, Madam~ A. GIUSTI ~t
Mon~~~u~ A.
MAQUET d~ l'~nté~êt
qu'~l~ man~6~~t~nt
pou~ e~
t~ava~l ~n aee~ptant d~ 6a~~~ pa~t~~ du ju~y.
J~ ~~m~~e~~ Mon~~~u~ Y.
GUEVENEY ~t tout l~ S~~v~e~
In6o~mdt~qu~ pou~ l~u~ géné~~u~~ a~~~~tane~. J~ n'oubl~~ pa~
M~~~~~u~~ H. CALVIGNAC ~t B. VEMARETS pou~ l~u~ t~ava~l ~a­
p~d~
~t ~o~gné,
et: la t~è~ g~and~ qual~té du d~~~~n d~~
eou~b~~.
J'a~~oe~~ a la p~é~~ntat~on d~ e~ t~ava~l tou~ e~ux
qu~,
~n~~~gnant~, eh~~eh~u~~, p~~~onn~l t~ehn~qu~ ~t adm~­
n~~t~at~6, ont pa~t~e~pé a ~a ~éal~~at~on. J~ ~~m~~e~~ tou~
pou~ l'aeeu~~l ~ympath~qu~ ~t dét~ndu qu~ m'a été ~é~~~vé au
Labo~ato~~~.
Pou~ t~~m~n~~,
j~ voud~a~~ d~~~ eomb~~n j~ ~u~~ h~u­
~~ux d~ la pa~t~e~pat~on au ju~y d~ Mon~~~u~ S. NIANG, R~e­
t~u~ d~ l'Un~v~~~~té
d~ Vaka~,
~t dont j'a~ été l'étud~ant.
A t~av~~~ lu~, j~ ~~m~~e~~ la Faeulté d~~ Se~~ne~~ d~ Vaka~
d~ m'avo~~ p~~m~~ d'~nt~~p~~nd~~ ~t d~ m~n~~ a b~~n e~ t~a­
va~l. Jla~ un~ p~n~é~ am~eal~ pou~ m~~ eollègu~~ du Vépa~t~­
m~nt d~ Phy~~qu~ qu~ ont ~u a ~uppo~t~~ l~ po~d~ d~ mon ab-
~~ne~.
INTRODUCTION
Les
processus
de
photoionisation
à
partir des
états
fondamentaux ou excités des atomes et des ions ainsi que les
processus
inverses
de
recombinaison
radiative
jouent
un
grand
rôle
dans
les
transferts
radiatifs
intervenant
dans
les
plasmas
de
laboratoire,
d'astrophysique
et
de
fusion
thermonucléaire contrôlée.
L'interprétation des spectres de
recombinaison,
l'étude de
l'équilibre entre l'ionisation et
la recombinaison,
les diagnostics de plasmas par émission et
l'évaluation des pertes par rayonnement dû es à des impuretés
nécessitent la détermination des sections efficaces de pho-
toionisation
et
de
capture et
des
coefficients ~e recombi-
naison radiative.
Les
progrès
dans
la
technologie
des
lasers
et
dans
les techniques des jets atomiques ont conduit récemment à un
développement
considérable
des
expériences
mettant
en
jeu
des atomes excités. En particulier l'utilisation de lasers à
colorant
permet
de
préparer
sélectivement
les
atomes
dans
des
niveaux
excités.
Parmi
ces nouvelles expériences,
cer-
taines
ont
pour
but
l'étude
de
la photo ionisation à partir
des
états
exci tés
et
d'autres
sont
destinées
à
comprendre
des mécanismes plus compliqués, comme par exemple ceux d'io-
nisation collisionnelle d'atomes très excités. Les expérien-
ces
du
premier
type
permettent
de
mesurer
des
sections
efficaces de
photoionisation.
La plupart de ces expériences
ont
été
réalisées
dans
les
alcalins
(Duong
et
al.
1978,
Kollath
1980,
Smith
et
al.
1980).
Les
valeurs
de
sections
efficaces
ainsi
obtenues
sont
très
peu
nombreuses,
les expériences n'étant souvent
réalisées que pour quelques
longueurs
d'onde
bien
définies.
Notons
aussi
le développe-
ment récent de mesures de sections efficaces de photo ionisa-
tion
obtenues
par
utilisation
simultanée
d'un
rayonnement
A-
2
synchrotron
et
d'une
excitation
laser
(Koch 1982,
Wuilleu-
mier
1982).
La
seconde
classe
d'expériences
mettant
en
jeu
des
processus d'ionisation
à
partir d'états atomiques exci-
tés
ne
donnent
en
général
pas
un
accès
direct
aux
sections
efficaces
de
photoionisation.
Par
contre
l'interprétation
des
expériences
nécessi te
la
connaissance
préalable
de
ces
grandeurs atomiques radiatives.
Citons par exemple les expé-
riences
d'ionisation
collisionnelle
d'atomes
de
.rubidium
excités (Cheret et al.
1982a,b).
En ce qui concerne la photoionisation des états exci-
tés
des
ions,
les
résultats expérimentaux sont
très rares à
cause des difficultés
expérimentales
encore
non surmontées.
De même
les
résultats
expérimentaux
relatifs
à
la
recombi-
naison
radiative
sur
des
états
excités
sont
peu
nombreux
;
ils
se
rapportent
pour
la
plupart
à
des
plasmas d'alcalins
(Agnew and Summers 1965,-Rothe 1969,
1971).
Parallèlement
à
l'essor des
méthodes expérimentales,
i l
y
a
un
regain
d'intérêt
considérable
pour
les
études
théoriques de photoionisation des états excités et de recom-
binaison
radiative
des
atomes
et
des
ions.
Et
ceci
pour
répondre
à
la demande
des expérimentateurs mais aussi,
d'un
point
de
vue
plus
fondamental,
pour
mieux
comprendre
les
phénomènes physiques mis en jeu.
En effet si les caractéris-
tiques
générales
de
la
photoionisation
des
atomes
et
des
ions
dans
leur
état
fondamemntal
sont
bien connues
grâce
à
de
nombreuses
études
expérimentales
et
théoriques
(Manson
1977,
Starace
1982)
il
n'en
est
pas
de
même pour
la
photo-
ionisation
à
partir
de
niveaux
atomiques
excités.
Lorsque
nous
avons
abordé
ce
travail,
les
seules
études
globales
visant
à
analyser
la
systématique
de
la
photoionisation
à
partir
de
niveaux
excités
étaient celles réalisées au labo-
rat 0 ire
dan s I e s a I cal i n s
lé g ers
Li,
Na et
K (Ayma r
et
al.
1976,
Aymar
1978).
Ces
études
ainsi
que
celles
plus
ponc-
tuelles
réalisées dans
Cs par Msezane and Manson (1975)
ont
mis
en
évidence
des
caractères
non
hydrogénoldes
nouveaux
..
3
par rapport
à
ceux apparaissant pour la photoionisation des
états
fondamentaux
d'atomes
ou
ions
apparition
de
plu-
sieurs minima dans les sections efficaces partielles corres-
pondant aux transitions n~ ..
e: (~+1)
et apparition d'un mi-
nimum dans
certaines sections efficaces associées aux tran-
sitions
n~
..
e: (~ -1).
De nombreuses
questions
se
posaient
alors. Les caractéristiques nouvelles mises en évidence pour
la
photoionisation
de
certains
états
excités
des
alcalins
étaient-elles générales et
les retrouvait-on pour la photo-
ionisation des états excités des ions? Dans ce domaine,
il
n'existait aucune étude globale de
systématique.
Pouvait-on
prévoir
l'existence
et
le
nombre
de
minima
apparaissant
dans
les
courbes
de
sections
efficaces
?
Enfin
quelles
étaient les conséquences de ces caractères non hydrogénoldes
sur
les
coefficients
de
recombinaison
radiative
sur
des
états excités ? Concernant ce processus inverse de celui de
photoionisation aucune étude globale de systématique n'avait
été réalisée.
Notre but est d'éte~dre et de généraliser les études
théoriques
antérieures
en
considérant
un
grand
nombre
de
systèmes
simples,
atomes
ou
ions à
un électron de
valence.
Notre étude porte sur la photoionisation, au voisina-
ge
du
seuil,
des
états
exci tés
de
nombreux
éléments
des
séquences
isoélectroniques de
K et Rb et des séquences iso-
électroniques
de
leurs
éléments
homologues
Cu
et
Ag.
Notre travail concerne aussi l'étude de la recombinaison ra-
diative dans ces mêmes éléments.
Rappelons que les alcalins
K et
Rb ont
pour
état
fondamental
m s
(m
= 4 pour K et
o
0
m
= 5 pour Rb).
Les
éléments
de
transition
Cu et
Ag
ont
o
10
pour
état
fondamental
(m -1)d
m s
(m
= 4 pour Cu et
0 0 0
m
=
o
5 pour Ag) et sont donc tout à fait semblables aux al-
calins puisque notre étude ne porte que sur la photo ionisa-
tion de l'électron de valence. Les études réalisées pour les
atomes
neutres ont été étendues à de nombreux ions de
leurs
séquences
isoélectroniques
un
grand
nombre
de
ces
ions
4
apparaissent dans
les plasmas de
laboratoire,
d'astrophysi-
que ou dans ceux de
fusion thermonucléaire contrôlée (Hinnov
1976, Shull and Steenberg 1982).
Nous
avons
calculé
les
sections
efficaces de
photo-
ionisation
au
voisinage
des
seuils
d'ionisation
où
les
caractères
non
hydrogénoldes
apparaissent
le
plus
marqués.
Nous
nous
sommes
placés
dans
le cadre d'un modèle à
poten-
tiel
central,
à
l'approximation
dipolaire
non
relativiste,
en
utilisant
la
méthode
du
potentiel
central
paramétrique.
Ce modèle convient bien aux systèmes à un électron de valen-
ce et sa simplicité permet des études intensives de systéma-
tique.
Les
coefficients
de
recombinaison
radiative
sont
déduits des sections efficaces de
photoionisation calculées
uniquement au voisinage des seuils par le ~rincipe de micro-
réversibilité.
Ils sont en
conséquence évalués à des tempé-
ratures relativement peu élevées.
Le
but
de
ces
calculs
très
extensifs est de
dégager
les caractères non hydrogénoldes spécifiques à la photoioni-
sation
des
états
excités
et
à
la
recombinaison
radiative
sur des états excités. Notre objectif est aussi d'étudier de
manière systématique l'évolution des caractères non hydrogé-
nOldes le
long d'une série de
Rydberg d'un élément donné et
le long des diverses séquences isoélectroniques et de compa-
rer le comportement le long des diverses séries et séquences
étudiées.
Ces
études
de
systématique
ont
pu
être
menées
à
bien en analysant les caractères non hydrogénoldes apparais-
sant dans les sections efficaces partielles de photo ionisa-
tian par une méthode nouvelle basée sur la théorie du défaut
quantique.
Dans le chapitre 1 nous rappelons des généralités sur
la
photoionisation
atomique
et
la
recombinaison
radiative.
Puis
nous
décrivons
les
divers
modèles
théoriques
permettant
de
calculer
les
grandeurs
atomiques
caractéris-
5
tiques
de
ces
processus.
Nous
donnons
aussi
les
résul tats
des
études
antérieures
obtenus
à
l'aide
de
ces
modèles
en
insistant
sur
la
systématique
des
caractères
non
hydrogé-
nOldes pour les systèmes à un électron de valence.
Les modèles théoriques de calcul des grandeurs atomi-
ques
que
nous
avons utilisés
et
celui
permettant
l'analyse
de
la
systématique
des
caractères
non
hydrogénoldes
sont
présentés
dans
le chapi t re
II.
Dans ce même chapi t re,
nous
présentons
et
discutons
l'ensemble
de
nos
résultats.
Ce
chapitre
a
pour
but
de
synthétiser
les
résultats
déjà
pu-
bliés dans quatre articles présentés en annexes.
Des tables
donnant
les
valeurs des défauts quantiques, des éléments de
matrice dipolaires et des sections efficaces de photoionisa-
tion pour
les
éléments
étudiés
sont
regroupés en appendice
dans un fascicule séparé.
7
CHAPITRU
BAeffLS THEORIQUES CONCE]NANT LA PHOTOIONISATION
ATOP1l.WE-f:T LA RECOMBINAISON RADIATIVE
Dans le cadre de ce travail nous étudions la systéma-
tique
de
la
photoionisation
des
états
excités
et
de
la
recombinaison radiative à l'intérieur des séquences isoélec-
troniques des alcalins K et Rb,
et des séquences isoélectro-
niques
de
leurs
éléments
homologues
Cu et Ag.
Les sections
efficaces de photoionisation sont calculées au voisinage des
seuils d'ionisation, et l'énergie des photoélectrons n'excè-
de
pas 20 Rydbergs.
Les énergies de photons incidents mises
en
jeu
couvrent
un
domaine
spectral
relativement
large
en
raison
de
la
diversité
des
degrés
d'ionisation
et
des
seuils
d'ionisation,
mais
elles
restent
inférieures
à
100
Rydbergs.
Les
coefficients
de
recombinaison
radiative
sont
déduits
des sections efficaces de
photoionisation calculées
uniquement
au
voisinage
des
seuils.
Ces
coefficients
sont
en
conséquence
évalués
à
des
températures
relativement
peu
4
élevées, n'excédant pas 8 x 10
K.
Dans
le
chapitre
L,
nous
rappelons
des
généralités
sur la
théorie de
la photoionisation aux basses énergies et
à
l'approximation dipolaire non
relativiste et sur la théo-
rie de
la recombinaison radiative,
puis des généralités sur
les
divers
modèles
théoriques
utilisés
pour
le
calcul
des
grandeurs caractéristiques de
ces deux
processus physiques.
Nous
les
complétons
en
donnant
quelques
résul tats, obtenus
antérieurement à l'aide de ces divers modèles,pour la photo-
ionisation
et la recombinaison radiative d'atomes et d'ions,
et
plus
particulièrement
de
systèmes
à
un seul électron de
valence.
Les
rappels
relatifs
à
la
photoionisation et
à
la
,
8
recombinaison
radiative
sont
regroupés
respectivement
dans
les parties A et B de ce chapitre.
Ces rappels vont permet-
tre de bien situer notre étude et de mieux cerner les objec-
ti fs que nous nous assignons dans ce travail.
A. PHOTOIONISATION DES ATOMES ET DES IONS
Nous
rappelons
dans
la
section
l
de
cette
partie
A
les
définitions
et
la signification
physique des grandeurs
fondamentales
qui
caractérisent
la
photoionisation.
Nous
donnons
ainsi
l'expression
générale
de
la section
efficace
de
photoionisation
et
les
formes
particulières
auxquelles
elle se ramène moyennant
quelques approximations.
Les modè-
les
théoriques
atomiques
utilisés
pour
le
calcul
des
sec-
tions efficaces de
photoionisation et
leur importance rela-
tive sont décrits dans les sections II et III.
Nous présen-
tons enfin dans la section IV les résultats généraux obtenus
antérieurement sur la photoionisation des états fondamentaux
et
exci tés
d'atomes
et
d'ions,
surtout
des
alcalins
et
de
leurs séquences isoélectroniques et d'autres systèmes élec-
troniques
qui
leur
sont
homologues.
Nous
insistons
plus
particulièrement
sur
la
systématique
des
caractères
non
hydrogénoldes de la photoionisation.
1. DEFINITIONS - FORMULES GENERALES
Considérons
l'interaction
d'un
rayonnement
incident
monochromatique avec une cible atomique.
Lorsqu'un
faisceau
de
photons
d'énergie
hv
d'un
tel
rayonnement
traverse
la
cible,
son intensité l
subit un affaiblissement qui est dû
o
à
diverses
interactions
élémentaires
entre
les
atomes
ou
ions
de
la
cible
et
les
photons
diffusion
élastique
et
inélastique,
création
de
paires,
effet
photoélectrique,
etc ... Après avoir traversé l'épaisseur x de cible, l'inten-
9
sité du faisceau passe de l
à l selon la relation (Ditchburn
o
and Opik 1962, Samson 1982)
l = l
exp(-Tx)
(1.1)
o
où
T
est
le coefficient d'absorption linéaire de
la cible.
Pour atteindre à partir de là les grandeurs caractéristiques
à
l'échelle atomique,
il faut avoir une connaissance précise
de
la cible atomique et savoir quels processus élémentaires
sont en jeu.
1)
Grandeurs caractéristiques de la photoionisation
Pour des énergies de photons inférieures à 10 keV, ce
qui
est
largement
le
cas de
notre étude,
le processus pré-
dominant
est
l'effet
photoélectrique
ou
photoionisation
(Pratt et
al.
1973).
Sous
l'action 'des photons,
les atomes
ou
ions
de
la
cible
perdent
un ou
plusieurs électrons
qui
passent des états liés dans le continuum.
Dans le cas où un
seul
électron
est
éjecté
après
absorption
d'un
photon,
le
processus de photoionisation est le suivant
X ( z - 1 ) +
h
(xz+
-)
i
+
V ~
j
+
e
f
( 1. 2)
L'atome
ou' ion
X(z-1)+
de
charge
(z-1)e
initialement
dans
l'état
i
passe
à
l'état
final
f
composé
de
l'ion
XZ+
de
charge ze dans l'état j et de l'électron éjecté. Pour que le
processus se produise il faut que l'énergie hv soit égale ou
supérieure
à
l'énergie
seuil
ou potentiel
d'ionisation
1 ..
.
~
l'électron est éjecté avec l'énergie cinétique €
telle que:
€
= hv - 1.
( 1. 3)
l
Nous
considérons
dans
la
suite
que
le
phénomène
global
observé en
photoionisation
est dû à l'effet purement addi-
tif des phénomènes élémentaires du type (1.2), et que chaque
photon
incident
ne
rencontre
dans
son
parcours
qu'un
seul
atome ou ion à l'état libre.
10
De
la
mesure
du
coefficient
d'absorption
linéaire
du
matériau
de
la
cible
à
l'aide
de
l'expression
(1.1)
on
déduit
la
section efficace de
photoionisation
que
nous
dé-
finissons maintenant.
Considérons une cible homogène de
section de surface
S,
d'épaisseur
dx
soumise
par unité de
temps à un rayonne-
- ment monochromatique
formé d'un
flux homogène de N
photons
p
par unité de surface.
Soient
T.
f
la probabilité pour qu'un
1-+
photon soit absorbé
par parcours unité,
N. le nombre d'ato-
1
mes
ou
d'ions
par
unité
de
volume
de
cible dans
leur état
initial,
et
w. f
la
probabilité
par
unité
de
temps
pour
1-+
qu'un atome ou ion soit ionisé.
Le nombre dN
de photons ab-
p
sorbés par unité de temps est :
( 1. 4)
en
con
du
flux
de
photons.
Ce
en
considérant les atomes
ou ions
i sont ionisés
dN
= N.S
w. fdx
( 1. 5)
p
1
1-+
Des deux expressions (1.4) et (1.5) on déduit N T.
f=
P 1-+
N.w.
f
et
les
deux
définitions
équivalentes
de
la
section
1
1-+
efficace de photoionisation cr. f
1-+
( 1. 6)
La première définition indique très clairement la si-
gnification physique de
la section efficace.
Elle a les di-
mensions
d'une
surface
et
représente
la
probabilité
d' ab-
sorption,
rapportée
à
un
parcours
unité,
de
chaque
photon
incident
dans
le
cas
où
le
milieu
cible
ne
lui
offrirait
qu'un atome ou ion par unité de volume.
La section efficace
24
est d'ordinaire exprimée en c~, en barns (1 b = 10-
c~) ou
11
1 8
mégabarns
(1
Mb = 10-
c~).
Il
est
rare
que
les
photons
ne provoquent qu'un seul
processus
élémentaire
(I. 2)
pour
une
cible
non
polarisée
il
y a donc
lieu de sommer sur les états initiaux et
finals
possibles pour obtenir la section efficace
(I. 7)
cr =
L: cr i-+ f
i, f
C'est
cette
grandeur
qui
est
directement
reliée
au
coeffi-
cient
linéaire dl absorption
l'
= L: 1'i-+f défini par la rela-
tion ( L n
i , f
l'
A
l'
cr = r
= Np
( I. 8)
l
a
où
A est
la
masse
atomique
de
l'absorbant
et
p
sa
masse
volumique,
et
Na le
nombre d'Avogradro.
Les mesures expéri-
mentales
du
coefficient
d'absorption
ne
peuvent
donc
con-
duire
à
des
valeurs
absolues de la section efficace que
si
la
cible
est
connue
parfaitement,
c'est-à-dire
principale-
ment pour les gaz
(Marr 1967).
La
deuxième
définition
de
la
section efficace donnée
par
la
relation
(I.6)
en
rapport
avec
la
probabilité
par
unité
de
temps
w -+
permet
d.'établir
l'expression
générale
i
f
de
la
section
efficace,
à
partir
de
laquelle
les
calculs
théoriques peuvent être effectués.
2)
Expression de la section efficace de photoionisation
L'établissement
détaillé
de
cette
expression
est
exposé
dans
de
nombreux
ouvrages
(Heitler
1954,
Bethe
and
Salpeter 1957,
Sobel'man 1972)
ou articles de
revue
(Stewart
1967,
Burke
1976,
St ar ace
1982),
et
nous
n'en
donnons
ici
que les grandes lignes.
F
1.2
2.1) Formule générale
La probabilité par unité de
temps w. f p-st
la pro ba-
1-+
bilité pour que x(z-1)+ passe de l'état initial discret i
à
l'état final f du continuum composé de
Z
X + dans l'état
dis-
cret
j
et
d'un
électron
éjecté,
suite
à
l'absorption
d'un
photon
suivant
le
schéma
CI. 2).
Les
principes
de
base
de
l'électrodynamique quantique
permettent
d'obtenir
l'expres-
sion
de
la
probabilité
de
transition
par
unité
de
temps
Wi-+f.
è
.
X(z-1)+
t
l
'
Le syst me électron1que
e
e champ electro-
magnétique
des
photons
sont
couplés
par
l'intermédiaire du
Hamiltonien
d'interaction
Hint.
En considérant
l'action
de
Hint comme faible
la probabilité de transition par unité de
temps est obtenue au premier ordre de la théorie des pertur-
bations
dépendantes
du
temps
à
l' aid e
de
la
règle d'or
de
Fermi (Messiah 1962, Cohen-Tannoudji et al. 1973)
( 1. 9)
Dans la relation (1.9),
les vecteurs d'états initial
I~.> et
1
final
I~f> sont les états propres de l'équation de Schrëdin-
ger de X (z-1)+
HI~> = EI~>
(1.10)
avec les énergies E
et Er telles que la relation
i
(1.11)
exprime
la
conservation
de
l'énergie.
L'état
initial
I~i>
est
normalisé
à
l'unité et
l'état
final
I~r> est normalisé
par
unité
d'énergie
suivant
(Bethe
and
Salpeter
1957)
(1.12)
La
densi té
d'états
correspondant
à
l'énergie
E
de
l'état
f
13
final
P
(équation
1.9)
s'identifie
avec
la
densité
des
Ef
états dans le continuum. La relation de normalisation (1.12)
1
donne PE
=
f
7T
Al' approximation
non
relativiste
qui
convient
bien
aux
basses
énergies
des
électrons
et
en
négligeant
les
effets de
spin,
le
Hamiltonien H (équation 1.10) du système
.
(z-1)+
électronlque
X
de
numéro
atomique
Z
et
de
nombre
d'électrons
N
a
pour
expression
(Heitler
1954,
Sobel'man
1972)
N
~2
!:..!..2
H = ~ (~
J+ ~ ~
(1.13)
r.
L r' k
j =1
J
j>k:1
J
Dans
la
relation
(1.13),
e
est
la
charge
élémentaire
de
~
l'électron,
m sa
masse,
p.
l'impulsion
de
l'électron
j ,
J
11
~
r.
=
j 1 le
module
de
son
rayon
vecteur
r.
rapporté
au
J
J~
noyau considéré comme immobile, et r
-
j k = 1
1j
r k 1 •
~
En considérant qu'un seul photon de vecteur d'onde k,
de
polarisation
1 et d'énergie h v est absorbé, on a pour
H.
t
(équation
1.9)
dans
l'approximation
non
relativiste
ln
N
Hint = ~ ~Pj.Aj
(1.14)
j=1
où c est la vitesse de la lumière et A. le potentiel vecteur
J
du
champ
électromagnétique
agissant
sur
l'électron
j.
En
développant
A
en
ondes
planes
polarisées
(Messiah
1962,
j
Sobel'man 1972)
et en utilisant les relations (1.6),
(1.7),
(1.9)
et
(1.14)
on
trouve
l'expression
générale de
la sec-
tion efficace de photoionisation :
2
N
(1.15)
c Chv ) = +- ~ I<wfl ~ 1. P j e xpOk.1 j ) /wi>1 2
m cv . f
. 1
r ,
J =
14
Cette
formule générale dépend explicitement de la direction
k des photons incidents, mais se simplifie dans le cas d'ap-
proximations particulières.
2.2) L'approximation dipolaire
Lorsqu'il
s'agi t
de
photons
de
faibles
énergies,
on
utilise
l'approximation
dipolaire
ou
"approximation
des
grandes
longueurs
d'onde"
(Bethe
and
Salpeter
1957).
Elle
correspond
au
cas
où
les
dimensions
atomiques
sont
petites
par rapport à
la longueur d'onde du rayonnement monochroma-
t i que
in c id e nt,
e t
s ' ex p r i me
pa r I a
con dit i on
k. r. << 1
J
(j
= 1, ••• , N). Toutes les exponentielles de la formule
(1.15) sont alors assimilables à l'unité et la section effi-
cace de photoionisation s'écrit:
(1.16)
et
ne
dépend
plus
de
la direction k des photons incidents.
La for mu l e
(1. 16)
est dit e for mu le" vit e s s e du di Pô le" deI a
section
efficace
puisqu'elle
fait
intervenir
l'opérateur
N
N
P = LP = -i~ L9 qui est proportionnel à l'opérateur som-
j
j
j=1
j=1
me
des
vecteurs
vitesses
des
électrons.
On
peut
utiliser
une
autre
expression,
dite
formule
"longueur
du
dipôle"
en
tenant compte des propriétés de commutation
du
Hamiltonien
H (équation
1.13).
Pour
un
opérateur
A ne
dépendant
pas
explicitement du
temps t,
la dérivée totale par rapport à t
est telle que (Sobel'man 1972)
."dA
[A,H]
IVldt
=
(1.17)
-+
Pour l'opérateur r =
on obtient
15
(1.18)
et puis, d'après l'équation (1.10)
N
N
<~fle. LPjl~i> = -4r(E i - Ef)<~fl€. L1jl~i>· (1.19)
j=1
j=1
En
utilisant
la
relation
(1.11)
la
formule
"longueur
du
dipôle"
de
la section efficace de photoionisation s'écrit:
2
2
N
v e
cr = cr L( hv)
= 81T c
i > 1 2
0.20)
L
~
1 <~ f 1€.
L1 j 1
i,f
j=1
Il est à noter que la formule "accélération du dipôle" de la
section efficace
peut
être aussi
obtenue
à
l'aide des pro-
priétés
de
commutation
de
H
(Stewart
1967,
Manson
1976),
mais
elle
est
beaucoup
moins
utilisée
que
les
deux
autres
formules
"vitesse" et
"longueur" du dipôle.
Des
expressions
(1.16)
et
(1.20)
on
déduit
pour
une
cible non polarisée l'expression générale de la section ef-
ficace
de
photoionisation,
en
moyennant
sur
tous
les
états
initiaux de même énergie E.
et en sommant sur tous les états
1
finals de même énergie E
(Burgess
and Seaton 1960,
Stewart
f
1967)
:
(1.21)
En considérant
la
relation
(1.21)
on
a en
particulier pour
crL(hV)
:
N
S~i = L I<~fl L1jl~i>12
(1.22)
i,f
j=1
et pour crV(hv)
:
V
Sfi =
(1.23)
16
Dans
l'équation
(1.21),
a.
est
la
constante
de
structure
fin e,
a l e
r a yon
de
B0 h r ,
hv
l' é n erg i e
du
p hot on
i ne ide n t
o
exprimée en Rydbergs,
g.
la dégénérescence du niveau d'éner-
l
gie
initial.
La
grandeur
Sfi
est
exprimée
en
unités
atomi-
ques
(Bethe
and
Salpeter 1957).
Le
facteur
1/3 dans
(l.21)
provient
de
la
sommation
sur
la
polarisation
€
du
photon
incident.
La détermination de
la section efficace de photoioni-
sat i on
suppose
la
conna issance
des
ét a ts
11JJ i >
et
11JJ f>
de
l'élément
X(z-l)+ de
numéro atomique
Z et de nombre d'élec-
trons
N.
Pour
un
système
à
plus
d'un
électron,
le Hamilto-
nien
H
(équation
1.13)
n'est
pas
séparable
en
variables
2
monoélectroniques à cause des termes biélectroniques _e__ .
Il
r j k
n'y a pas alors de solutions exactes
l1JJ > et
l1JJ
> à l'équa-
i
f
tion
de
Sc h r o d Lnqe r
(l.10).
Il
y a
lieu
de
recourir
à
des
solutions
approchées,
moyennant
certaines
hypothèses
typi-
ques
des
différents
modèles
atomiques
théoriques
utilisés.
La
relation
(1.19)
n ' est
en
général
plus
véri fiée
et
les
formules
"longueur"
et
"vitesse"
du
dipôle
de
la
section
efficace donnent
des
résultats
différents.
Selon la
formule
retenue différentes régions de l'espace de configuration ont
une
importance
relative
plus
grande
que
d' autres
dans
les
calculs.
Ainsi
la
formule
"longueur"
du
dipôle
est
plus
appropriée aux rayons moyens,
et la formule "vitesse" du di-
pôle
plutôt
aux
rayons
petits.
Les différences de
résultats
entre
ces
deux
formules
mesurent
le
degré
d'approximation
des solutions approchées dans tout
l'espace de configuration.
2.3.) Forces d'oscillateur
et autres grandeurs
caractéristiques
La
section
efficace
de
photoionisation
est
liée
à
d'autres grandeurs fondamentales.
17
.
df(h\\l)
La densité de forces d t o s c f I Lat eu r
d(h\\l)
qu'on défi-
nit
dans
le
spectre
du
continuum
(Bethe and
Salpeter 1957,
5tarace 1982) lui est directement proportionnelle:
df(h\\l)
2
2-1
d(h\\l)
= (4'11' ('tao)
o Cnv) .
(1. 24)
Cette
notion de densité de forces d'oscillateur complète la
notion
habituelle
de
forces
d'oscillateur
des
transitions
dans
le
spectre
discret
(Bethe
and
Salpeter
1957,
Stewart
1976).
La distribution des forces d'oscillateur dans tout le
spectre,
discret et continu,
est importante (Fano and Cooper
1968)
du
fait
des
règles
de
somme
très
utiles
auxquelles
elles obéissent
(Shore and Henzel
1968).
La
section
efficace
de
photo ionisation
est
directe-
ment
reliée
à
la
distribution
angulaire
des
photoélectrons
émis,
qui
est
si
importante
en
spectroscopie
d'électrons
(Cooper and
lare 1968,
Hanson 1976,
Starace 1982). De
fait,
si on considère l'état final
I~f> comme étant constitué d'un
ion et d'un électron émis dans une direction bien définie la
même
expression
(1.16)
ou
(1.20)
désigne
aussi
la
section
efficace
différentielle
de
photoionisation
~~, dn étant
l'élément
d'angle
solide
d' éjection
du
photoélectron.
La
section
efficace
différentielle *IT permet d'obtenir la dis-
tribution
angulaire
des
photoélectrons
(Cooper 1976),
et
la
section
efficace
de
photoionisation cr s'en déduit par inté-
gration
sur
tous
les
angles
d'éjection
(Sobel'.an
1972,
Burke
1976).
A l'approximation
dipolaire,
on
obtient
pour
une
polarisation
linéaire
des
photons
incidents
et
un
élé-
men t
c i b l e
non
pol a ris é , l a
rel a t ion
g é n é r ale
(C 0 op e r
and
lare 1968)
(1.25)
Dans la relation
(1.25), B(h\\l) est le paramètre d'asymmétrie,
P2(cos8)
le
polynôme
de
Legendre
d'ordre
2,
et
8
l'angle
18
ent re
le
vecteur
polarisation
€
des
photons et
le
vecteur
d'onde ~
du photoélectron émis.
e
Signalons enfin que la section efficace de photoioni-
sation
est
reliée
à
la
section
efficace
de
recombinaison
radiative par le principe de microréversibilité (Hassey 1969),
la
recombinaison
radiative
étant
le
processus
inverse
du
processus de photoionisation, ainsi que nous le verrons dans
la partie B de ce chapitre.
Nous
avons
rappelé dans
cette
section 1 les défini-
tions
et
formules
générales
des
grandeurs
caractéristiques
du
processus
de
photoionisation.
La
détermination
de
la
section
efficace
de
photoionisation
pour
l'élément
X(z-1)+
ayant
plus
dl un
électron
ni est
possible
qu'avec
les
solu-
tions appr.ochées de l'équation de
Schrodinger.
Nous présen-
tons dans
la suite les différents modèles atomiques théori-
ques utilisés dans les calculs de photoionisation, en préci-
sant
leur
domaine
de
validité,
leurs
limites et les
résul-
tats qu'ils ont permis d'obtenir.
Ces différents modèles se
répartissent
en deux
grandes
catégories
le modèle à par-
ticules
indépendantes
et
les
modèles
au-delà
du
modèle
à
particules indépendantes.
II. MODELE A PARTICULES INDEPENDANTES
Les méthodes théoriques les plus simples utilisent le
modèle
à
particules
indépendantes
(fana
and
Cooper
1968).
Nous
rappelons
des
générali tés
sur ce modèle,
l'expression
particulière
de
la
section
efficace
de
photoionisation
et
les
différents
types
de modèle
à
particules
indépendantes
utilisés dans les calculs de photoionisation.
19
1) Généralités sur le modèle à particules indépendantes
1.1) Hypothèses de base
La principale hypothèse de
base est que chaque élec-
.
(z-1>+
tron du système électronlque X
se meut sur une orbitale
bien
définie,
à
laquelle
correspond
une
fonction
d'onde
monoélectronique
cp appelée
spin-orbitale.
La spin-orbitale
a la forme pour un électron lié
(1.26)
et pour l'électron libre éjecté
Pe:R..,(r)
cp n,
(-;)
::
<-; 1 c R.. ' mn , ms' > =
r
y n , m
( e , cp ) ô ( a , ms' )
e:~ mR..,m s'
~
~
R..'
(1.27)
où
;t = (r,a) représente les variables d'espace et de spin.
Les coordonnées sphériques d'un électron sont (r,e,cp), R..(R..')
et
m R..(m R..')
les
moments
angulaires
orbital
et
magnétique,
Yn (e,cp) et Y n,
(e,cp)
les harmoniques sphériques normali-
z m
~ mR..'
sées,
ô(a ,ms)
et
ô(a ,ms')
les
fonctions
de
spin
normali-
sées; n est le nombre quantique principal d'un électron lié
de
fonction
d'onde
radiale
PnR.. (r ) et e:
l'énergie cinétique
de
l'électron
libre
de
fonction
d'onde
radiale
P e:R.. ,(r).
L'attribution
d'une
orbitale
bien
précise
à
chaque
électron
conduit
à
considérer
que
dans
le
processus
de
photoionisation
de
X(z-1)+
(1.2),
le
Nième
électron
passe
d'une
orbitale
discrète
à
une
orbitale
du
continuum tandis
que
la
répartition des
(N-1) électrons du coeur qui ne par-
ticipent pas à la photoionisation reste inchangée. La déter-
mination des fonctions d'onde radiales PnR..(r) et Pe:R..,(r) dé-
pend
du
type
de
modèle
à
particules
indépendantes
choisi.
Leur obtention à
l'aide
par exemple
d'un
potentiel
central
V(r) sera discutée plus loin (§ 2). Auparavant, nous donnons
20
l'expression
de
la
section efficace
en
considérant
d'abord
le cas le plus simple du modèle à un électron,
puis le cas
plus général.
1.2) Expression de la section efficace dans le modèle
à
un électron
Le modèle à un électron est caractérisé par l'emploi
d'un
Hamiltonien
monoélectronique
h
en
lieu
et
place
du
Hamiltonien
H de
X(z-1)+
(équation
I,13).
Au
cours
du
(I,2),
l'électron
passe
d'un
un état
telle que (équation 1.11)
:
(I,28)
L'expression longueur du dipôle de la section effica-
de
photoionisation
(équations
1.21,
1.22 et I,28)
s'écrit
+,q,
+,q,'
4
2
1
\\'
\\'
crn,q,(€)
= 3wa a o ( €- €n ,q, ) 2,q, +1 L
L
En
passant
aux
composantes
sphér iques
(Shore
and
Henzel
+1
1968) de r = \\'
(-1) qrC(1);
et en utilisant le théorème
de
L
q - q
q=-1
Wigner-Eckart
(Sobel'man 1972)
cr n,q, (e:) = ina a ~ ( € - € n,q, ) 2,q,1+ 1 L1<€,q, 1 Il r C( 1) Il n,q, >12, 0 u en cor e
,q,'
21
4
2
1
\\'
2
l '
(1)
]2
an R. (e;)
= JlTa a 0 ( c - c nR. )~ L RnR. , R. ' ( €)
<R. 1/ C
Il R. >
R.'
L'élément de mat r ice rédui t
<R.' Il c (1) Il R.> condui t aux règles
de sélection
des transitions dipolaires électriques bien
connues
R.' = t
:t 1
(1.29)
En
remplaçant
les
éléments
de
matrice
réduits
par
leurs
valeurs on trouve
:
a nt(€)
= O.855X10-1~€-€nR.) (2t:1R~R.,t_1(€)+2tt+\\R~t,t+1(€))
( crrf)
( 1. JO)
00
où
(1.31)
RnR.,R.,(E:)
= f Pnt(r)rPEt,(r)dr
o
est
l'élément
de
matrice
de
transition -d Lp o Lai r e
en
unités
atomiques.
Les
fonctions
d'onde
radiales
Pnt(r)
et
P€tr(r)
sont
normalisées
respectivement
à
l'unité
et
par intervalle
d'énergie en Rydbergs
(équation 1.12)
:
00
f P€t,(r)P€,t,(r)dr
=
lTô(€-€').
(1. 32)
o
Le
facteur
numérique
dans
l'équation
(1.30)
dépend du
choix
de
la
normalisation
(1.32),
qui
implique
que
la
fonction
radiale du continuum a pour forme asymptotique
Les grandeurs
e( r ) et
ô
(e;)
seront définies ultérieurement,
t'
dans la section 2.1.2.
La
section
efficace
totale de
photoionisation a nt(€)
est la somme des sections efficaces partielles de photoioni-
sation an R., R.-1 (€)
et a nt ,t+1 (c ) correspondant aux deux con-
tinua
(t -1)
et
(t+1)
du
photoélectron
pour
t
-j.
0,
et
se
22
rédui t
à la seule O'n~, ~+1 (e:) pour ~ = O.
1.3) Expression générale de la section efficace
(z-1)+
Pour
un
système
X
avec
un
nombre
N élevé
d' é-
lectrons,
les solutions approchées l'!I
> et l'!I > de H (équa-
i
f
tion
1.13)
caractérisant
les
états
initial
et
final
du
processus
de
photoionisation
(1.2)
sont
dans
un
modèle
à
particules
indépendantes
des
déterminants
de
Slater
(Slater
1960)
ou
des
combinaisons
linéaires
de
ces
déterminants,
construits
à
partir
des
N spin-orbitales
monoélectroniques.
Dans l'hypothèse des particules indépendantes où
une orbita-
le
bien
précise
est
attribuée
à chaque électron,
l'interac-
tion
de
configurations
est
négligée.
En
ce
qui
concerne
la
photoionisation
il
suffit
de
ne
considérer
que
les
transi-
.
ième
t i oris
dans
lesquelles
le
N
électron
dit
Le c t r o n
actif
é
est
éjecté
d'une
des
sous-couches
(n ~)
vers
le
continuum
(e:~'), passant d'une orbitale discrète à une orbitale libre.
Dans
le
même
temps,
la
distribution
des
(N-1)
autres
élec-
trons
dits
électrons
passifs
entre
les
différentes
sous-
couches
reste
inchangée.
Donc
l'approximation
l'!I. > ne cam-
l
porte
que des orbitales discrètes
et celle
l'!I > en comporte
f
une seule de libre.
La
section
efficace
de
photo ionisation
de
la
sous-
couche
(n~) de potentiel d'ionisation 1 n peut s'écrire sous
n~
_
la
forme
très
générale
(Bates
1946,
Burgess
and
Seaton
1960)
:
0.34)
O'n~(e:) = j~aa~(e:+ln~)Cp
~ C~,R~~,~,(e:)
~'=~±1
Dans l'équation
(1.34),
hv = e:+ln~ d'après l'équation (1.3).
Les
deux continua du photoélectron sont
~'
= ~± 1 comme dans
le
cas
simple
du
modèle
à
un
électron
(1.29).
Les
coeffi-
cients
C~,
sont
purement
angulaires
et
dépendent
des
états
23
initial
et
final.
La
distribution
des
électrons
passifs
reste inchangée dans l'hypothèse des particules indépendan-
tes,
mais
leurs
fonctions
d'onde
peuvent
être
di fférentes
dans les états initial et final.
Le coefficient
N-1
0.35)
fClD i
f
2
Cp:
IT 1
P(n1)t (r)P(n1)t (r)drl
t=1 0
est
lié
à
cette distorsion,
et sa différence par rapport à
l'unité
évalue
l'importance
de
la
relaxation
du
coeur
du
systèm~ électronique formé des (N-1) électrons passifs.
Les
éléments
de
matrice
de
transitions
dipolaires
R
(g)
sont calculés
n1,1'
à
partir des fonctions d'onde liée
P
et libre P
n1(r)
g1,(r) de l'électron actif; ces fonctions
peuvent
éventuellement
dépendre des termes spectroscopiques
caractérisant les états initial
I~i> et final I~f>.
2) Différents modèles à particules indépendantes, non
relativistes
Le
calcul
de
la section efficace
de
photoionisation
(1.30 et 1.34) se ramène donc à celui des co~fficients angu-
laires, et des fonctions d'onde radiales Pn 1(r)
et Pg1' (r) •
Les
coefficients
angulaires
sont
facilement
calculables
en
utilisant l'algèbre de Racah (Armstrong 1959). La détermina-
tion de
Pn1(r)
et Pg1,(r) dépend du type de modèle à parti-
cules
indépendantes
considéré.
Nous
mentionnons
les
types
de
modèles
non
relativistes
les
plus
couramment
utilisés
dans les calculs de photoionisation.
2.1) Modèles à champ central
Dans
l'approximation
du
champ
central
(Slater
1929,
1960)
le
Hamiltonien approché H
du système X(z-1)+ s'écrit
o
en unités atomiques (les énergies sont exprimées en Rydbergs)
24
N
( 1.
Ho = L[-6
36)
j
+ v(r j )]
j=1
où
V(r .)
est
le
potentiel
central
moyen
exercé
sur
chaque
J
électron
j
par
le noyau et les autres électrons.
Les orbi-
tales monoélectroniques int~oduites par les équations (1.26)
et (1.27) sont fonctions propres du hamiltonien monoélectro-
nique
h . = -6. + V(r .)
(1.37)
J
J
J
où V(r ) est défini pour tout r,
et est choisi de manière à
j
être
une
bonne
approximation
des
effets
du
coeur
(noyau,
(N-n
électrons)
sur
l'électron
actif.
Le
modèle
à
champ
central
est
un
modèle
à
un
électron.
Le
potentiel
central
Ver)
est
caractérisé
par
les
conditions
aux
limites
2Z
2z
Ver) r~O -r' V(r) -+
(1.38)
r-+oo
r
où Z est la charge nucléaire de X(z-1)+,
z
et
z
= Z-N+1
est
la
charge
résiduelle
de
l'ion
final
X+
après ionisation.
Le modèle à champ central le plus simple est le modè-
le
hydrogénoide
pour
lequel
chaque
électron
du
système
électronique
de
numéro
atomique
Z est
soumis au
champ cen-
tral coulombien du noyau
v(r ) =
2Z
--
( 1. 39 )
r
quelque soit r.
C'est le seul modèle qui soit soluble exac-
tement (Bethe and Salpeter 1957). Nous rappelons son domaine
d'utilisation,
le comportement hydrogénaI de bien connu (Hall
1936,
fano and Cooper 1968)
et les formules d'approximation
pour la section efficace de photoionisation (Sobel'man 1972).
2S
Pour
le
système
hydrogénolde
on
obtient
des expres-
sions analytiques pour les éléments de matrice de transition
Rn~,~'(€)
(équation 1.31)
et la section efficace
an~(€)
(~quation 1.30) (Gordon 1929, Menzel
and Pekeris 1935, Bur-
gess 1964). La section efficace a~~(€) d'un ion hydrogénolde
de charge z = Z est reliée à la section efficace de l'hydro-
gène H par la relation :
( I. 40)
Nous
rappelons quelques points
importants du compor-
tement
hydrogénolde.
Les
éléments
de
matrice
de
transition
R~~,~,'(€) sont toujours des fonctions monotones, positives
et
décroissantes
de
e .
Les
sections
efficaces
partielles
a~~,~,(€) et totale a~~(€) ont alors un maximum au seuil de
photoionisation €
=0, d'où elles décroissent de façon mono-
tone et tendent vers zéro quand €
croit. Pour ~ i 0, la con-
tribution de a~~,t+1(€) est toujours dominante et le rapport
a~.Q".Q,_1 (€)/a~.Q".Q,+1(E) est toujours inférieur à 1 et croit
avec n. Pour une série de Rydberg nt donnée, les valeurs des
sections efficaces au seuil a~.Q"t,(O) et a~.Q,(O)
croissent
avec n. Pour un n donné, a~t(O) croit avec t jusqu'à attein-
dre un maximum puis décroit. Pour t
~ 3, la section efficace
a~.Q, (E) décroi t avec € d'autant plus rapidement que n est
grand.
b) Validité et limites
Le modèle hydrogénolde constitue une bonne approxima-
tion
pour
la
photoionisation
d'électrons
de
couches
assez
internes de systèmes électroniques complexes,
et correspon-
dant au domaine spectral des rayons X durs (Hall 1936). Ces
électrons internes sont en effet soumis à un potentiel moyen
coulombien du fait que les effets d'écran sur le noyau sont
faibles,
et donc que l'interaction coulombienne du noyau de-
vient prépondérante.
26
Le
modèle hydrogénolde constitue aussi
un cas limite
pour
les
atomes
très
Lo n i s s
é
à
l'intérieur
des
séquences
isoélectroniques lorsque
le
degré
d'ionisation
augmente.
En
effet
d'après
l'équation
(1.13),
l'interaction coulombienne
du
noyau
devient
de plus en plus prépondérante sur l'inter-
action répulsive des électrons lorsque la charge Z augmente,
le nombre d'électrons N restant constant.
Lem 0 dè l e
h y d ro g é n 0 1den ' est
cep end a n t
g uère
a ppro -
prié
au
voisinage
du
premier
seuil
de
photoionisation
des
atomes
peu
ionisés
et
pour
de
faibles
énergies
de
photons
incidents,
correspondant
plutôt
aux
rayons
X
mous
et
à
l'ultraviolet
lointain
(Fano and
Cooper 1968).
En effet des
caractères
non
hydrogénoldes
marqués
apparaissent
alors
tels
par
exemple
les
minima
et
maxima
des
courbes
de
sec-
tions
efficaces
de
photoionisation
mis
en
évidence
expéri-
mentalement (Ederer 1964, Harr and Creek 1968), dont l'exis-
tence
ne
peut
être
prévue .p e r
le
modèle
hydrogénolde.
De
fait
les
électrons
des
couches
peu
profondes
et
externes
se
meuvent
dans
un
potentiel moyen sensiblement non coulom-
bien.
Il
y a
lieu
dans
ces
conditions d'utiliser
un
modèle
plus
réaliste
et
plus
élaboré
que
le
modèle
hydrogénolde,
pour
rendre
compte
et
prévoir
le
comportement
non
hydrogé-
no Lde
des
sections
efficaces
de
photoionisation.
Ceci
fera
l'objet des sections qui suivent.
Auparavant,
nous
considérons
les
formules
d' approxi-
mation
déduites
du
modèle
hydrogénolde
qui
nous
serviront
dans la suite (section B.II). Le modèle hydrogénolde consti-
tue
une
bonne
approximation
pour
la
photoionisation
et
la
recombinaison radiative des états très excités de systèmes à
plusieurs
électrons,
en
particulier
de
systèmes
à
un
seul
électron
de
valence.
Pour
ces
processus il
y a
souvent
be-
soin
de
calculer
un
grand
nombre
de
sections
efficaces
de
27
photoionisation.
Les expressions analytiques de
a~1(e) de-
viennent de
plus en plus compliquées et difficiles à calcu-
ler
directement
lorsque
n
croit
(Burgess
1964).
On
peut
alors utiliser des expressions approchées plus simples.
Gaunt
La section efficace de photoionisation à partir de la
couche n définie par
est
approximée
dans
le
modèle
de
Kramers
par
l'expression
semi-classique (Kra.ers 1~23t Sobel'man 1972) :
2
64'ITaa o
(1.41)
Cette expression donne des
résultats corrects près du seuil
e = 0 quelque soit nt mais n'est pas satisfaisante dès qu'on
s'éloigne du seuil.
Une importante amélioration est obtenue
à
l'aide du
facteur g (z,e) de Kramers-Gaunt
(Gaunt
1930,
n
Sobel'man 1972) défini par
(1.42)
dont
le
développement
asymptotique est
bien connu
(Henzel
and
Pekeris 1935,
Burgess 1958 t Seaton 1959). Les diverses
corrections
apportées
au
modèle
de
Kramers
qui
correspond
lui-même à gn(z,e) = 1 améliorent le comportement au-delà du
seuil de la section efficace de photoionisation.
La méthode du défaut quantique (Seaton 1955,
1958) a
permis à Burgess et Seaton (1960) de généraliser la méthode
de calcul des probabilités de transitions discrètes de Bates
28
et
Damgaard
(1949)
ou
approximation
de
Coulomb,
en
l'éten-
dant
aux
calculs
de
sections
efficaces
de
photoionisation.
De fai t,
la contribution
la
plus
importante à
l'élément
de
matrice
de
transition
Rn R.,R.' Cc )
(équation
1.31)
provient
presque entièrement de régions où les valeurs de la variable
radiale r sont grandes, et où l'électron se meut principale-
ment
dans
le champ
asymptotique
coulombien
du
coeur
(équa-
tion
1.38).
Dans la méthode du défaut quantique,
l'électron
actif
est
donc
soumis
au
potentiel
central
v Cr ) tel
que
2z
pour r > r
V(r)
= - -
(1. 43)
o'
r
Les fonctions d'onde radiales de cet électron dans la
transition nR. ~ e:R.' sont déterminées uniquement pour r
> r •
o
La fonction PnR. (r) s'exprime à partir des fonctions réguliè-
res
et
irrégulières
de
Coulomb
et
du
défaut
quantique
]..InR.
relié à l'énergie monoélectronique e:nR. par:
2
z
o .44)
2
(n-]..InR.)
La
fonction
Pe:R.,(r)
a
pour
forme
asymptotique
0.33)
où
1/2
R.''IT
Z
( 1 / 2
(
iZ)
0(r) = e:
r--Z-I
1/21n 2e:
r)+argr R.'+1-~
e:
e:
représente
la
phase
asymptotique
d' une
fonction
radiale
du
continuum pour un
électron soumis partout au seul potentiel
coulombien
V(r)
= _l!. (équation 1.39). Pour un électron
r
sou mis
à
un
pot e n t i e l
V( r )
tel
que
V( r )
= -g uni que men t
r
lorsqu'il
est
loin
du
coeur
(équations
1.38
et
1.43),
il
s'introduit
un déphasage supplémentaire
ôR.,(e:)
dû à la par-
tie non coulombienne du potentiel aux
faibles valeurs de r.
Dans
la
méthode
du
défaut
quantique
le
déphasage
ôR.,(e:)
peut être obtenu par extrapolation dans le continuum
des défauts quantiques de la série
nR.'
(1.45)
29
Cette extrapolation n'a de sens que si exp(-2nz/l€)
« 1. Le
défaut quantique ~n~ et le déphasage Ô~I(€) mesurent l'écart
par rapport au modèle hydrogénolde.
Burgess et
Seston
(1960)
ont établi une formule très
générale pour le calcul des sections efficaces de photoioni-
sation.
Cette
formule a été revue par Pesch (1967),
étendue
à
des
états
plus
exci tés
et
à
un
domaine
d'énergie c
plus
grand. L'élément de matrice de transition Rn~,~'(€) est pré-
senté sous la forme oscillatoire :
) - 2
c '
x
( 1. 46 )
où n* = n-~n~' €'
= €/z2
et ~~(€) est obtenu
par extrapola-
tion
des
défauts
quantiques
~nt
de
la
série n~.
Les fonc-
tions G et X sont tabulées par Pesch (1967).
La méthode
du
défaut
quantique
a été
largement
uti-.
lisée
pour
la
photoionisation
à
partir
des
états
fondamen-
taux
des
atomes
neutres
et
des
ions
(Burgess
and
Seston
1960,
Pesch
1967),
à
partir
des
états
excités
surtout
des
alcalins
(Moskvin 1963,
Norcross and Stone 1966, Devdsriani
and
Klyucharev
1977)
et des
gaz
rares
(Harquist 1981).
Les
résul tats
obtenus
sont
en
assez
bon
accord
avec
ceux
des
autres
méthodes
théoriques,
surtout
si
les éléments
de
ma-
trice
de
transition
(1.46)
sont
peu sensibles au
comporte-
ment des fonctions d'onde aux petites valeurs de r < r
et
o'
s'ils ne s'annulent pas,
aux grandes valeurs de r > r . Au-
o
trement
il
y a lieu de
recourir à d'autres types de
modèle
introduisant un potentiel central défini pour tout r.
Nous nous servirons de la méthode du défaut quantique
pour une analyse systématique de nos résultats de photoioni-
sa t i on dans le chapitre II.
30
Dans
le cas du
modèle
à
champ central les fonctions
d'onde
radiales
dans
les
états
initial
et
final,
respecti-
vement
Pn R. (r )
et
P ER. ' (r),
sont
sa lut ions
de
l' équat ion
de
Schrodinger radiale :
(1.47)
dans
l'hypothèse où
l'électron dans l'état final est soumis
au
même
potentiel
central
que
l'électron
dans
l'état
ini-
tial.
Notons que l'utilisation de deux potentiels différents
pour
décrire
le
mouvement
de
l'électron
lié
et
celui
de
l'électron libre permet de
tenir compte parfois de certains
effets de relaxation.
Les
potentiels
centraux
paramétriques
dépendent
de
paramètres.
Ceux-ci sont souvent déterminés par comparaison
de
grandeurs
calculées
aux
valeurs
expérimentales
en
général il s'agit des énergies,
et on parle alors de
poten-
tiels
semi-empiriques.
Les
paramètres
peuvent
aussi
être
déterminés par minimisation de l'énergie de l'état fondamen-
tal
de
l'atome ou de
l'ion considéré,
et il s'agit alors de
potentiels
ab-initia.
Nous
ne
citerons
ici
que
quelques
types
de
potentiels
utilisés
pour
calculer
les
sections
efficaces de photoionisation des états excités des alcalins.
a)
Des
calculs de
sections efficaces de photoionisa-
tian
à
partir
des
états
fondamentaux
de Cs
(Norcross 1973)
et des états peu excités des alcalins Li-Cs (Hofsaess 1977)
ont été effectu~ à l'aide du potentiel de Thomas-Fermi avec
facteur d'échelle (Stewart and Rotenberg 1965)
:
l-.?f(cp(x)+Îx:)
Ver)
=
2z
( 1. 48)
r
31
où
x = r/~, ~ = 0.8853 Z-1/3. La fonction ~(x) est la fonc-
tion
Thomas-Fermi
de
l'ion
de
rayon
ionique
X
dédui te
de
o
l'équation:
d2p ( x ) _
()3/2 -1/2
2
- cp x
x
dx
avec les conditions aux limites
:
( )
dP(X)1
z
~(O) = 1, cp X
= a et
dx
o
= -XZ
x=x
o
o
Le
potentiel
de
Thomas-Fermi
(1.48)
peut
être
modifié
en
introduisant
le
facteur
d'échelle
À
,
paramètre
ajustable
n t
r
avec alors x = ---x--.
~ nt
b )
L'étude
de
la
photoionisation
à
partir
de
l'état
fondamental
et
à
l'intérieur
de
la séquence isoélectronique
de Li a été
faite
(Tiwari et al.
1975) à l'aide du
potentiel
analytique
(Green et al.
1969)
:
Ver)
= -;[(Z-1H"2(d+1]
( 1. 49)
r
d
avec
n(r)
= [H(e / _ 1 )+1J-1
où le paramètre de forme H et le paramètre facteur
d'échelle
d sont ajustables.
c)
Le
potentiel paramétrique de Klapisch (1971)
a été
employé
par
Aymar
et
al.
(1976)
dans
la
photoionisation
le
long
de
séries
de
Rydberg
des
alcalins
légers
Li,
Na et
K.
C'est
ce
potentiel
que
nous
utilisons
dans
notre
étude
et
nous en rappellerons les caractéristiques dans
le chapitre
II.
32
2.1.4) ~~~~~~~~!~_~~~~:~~e~E~g~~~_~~~~_~!!~~~_~~_e~!~E~~~~~~~
du coeur
Allant au-delà du simple modèle à particules indépen-
dantes
qui
ne
tient
pas
compte
explicitement
des
corréla-
tions entre les électrons du système électronique et consi-
dère le coeur comme statique, l'interaction entre l'électron
de
valence
et
les
moments
induits
des
électrons
du
coeur
peut
être
prise
en
considération
de
manière
effective.
La
théorie
des
perturbations
stationnaires
au
premier
ordre
introduit
un
terme
de
potentiel
de
polarisation
du
coeur
V
l(r)
(Weisheit
and
Dalgarno
1971,
Caves
and
Dalgarno
po
1972, Weisheit 1972a,b) comme correction qui s'ajoute au poten-
tiel central V (r)
de l'ion coeur.
La forme asymptotique de
o
V
l( r ) est :
po
a -68a
g
0
+
•• ,.
(I,SO)
6
2r
où
on
introduit
les
polarisabilités
statiques
dipolaire
(ad) et quadrupolaire (a ) du coeur,
ainsi que la polarisa-
q
bilité dipolaire
dynamique
(8).
De plus pour éviter
la di-
vergence
lorsque
r
-+
0,
les
termes
de
polarisation
sont
multipliés
par
des
fonctions
de
coupure.
Des
formes
très
diverses de V
l(r)
ont
été
choisies
(Beigman
et
al.
1970,
po
Weisheit 1972a,b,
Black
and
al.
1972, Chichkov
and Shevelko
1981).
Ces
potentiels
sont
associés
à
divers
potentiels
V (r),
souvent
du
type
Thomas-Fermi
avec
facteur
d'échelle
o
(Norcross 1973, Hofsaess 1977).
La théorie des perturbations stationnaires au premier
ordre
permet
également
de
tenir
compte
des
effets
de
la
polarisation du coeur sur l'élément de matrice de transition
dipolaire
(Hameed et
al.
1968,
Weisheit and Dalgarno 1971,
Weisheit
1972a,b)
sous
diverses
formes
(Norcross
1973).
Dans la
formulation longueur du dipôle,
Rn~,~'(€) (équation
(1.31) est modifié et devient (Weisheit 1972a,b) :
33
Rn R, , R, 1(e ) = fOl PnR, ( r ) [r{1- :~ f c ( r c )}] PER,' ( r ) dr
(1.51)
o
où
r
est
le
rayon
de
coupure
effectif du
coeur et
fc(r
c
c)
une fonction de coupure.
Nous
avons tenu compte des effets de polarisation du
coeur
dans
nos
calculs
de
photoionisation,
ainsi
que
nous
le verrons dans le chapitre II.
2.1.5) Potentiels centraux ab-initio
Les potentiels centraux ab-initio les plus couramment
employés dans les calculs de photoionisation sont dérivés du
formalisme Hartree-Fock
(Hartree 1957,
slater 1960,
Froese-
Fischer
1977).
Le
plus
largement
utilisé
de
tous
est
le
potentiel Hartree-Slater (Herman and skillman 1963, Fano and
Cooper
1968).
L' introduction
de
l'approximation
des
effets
d'échange
par le potentiel central
(slater 1951)
déduit
du
modèle de gaz dtélectrons libres
( 1.52)
dans
les
équations
self-consistantes
Hartree-Fock
(Herman
and
Ski lIman
1963,
Cohen and
Mc Each r an
1980)
condui taux
équations Hartree-Slater.
Dans
(1.52),
p(r) désigne la den-
sité électronique totale du système électronique. La résolu-
tion
des équations
de
Hartree-Slater permet d'obtenir
à
la
fois
le
potentiel
central
Hartree-Slater
VHS(r),
les
fonc-
tions d'onde fadiales PnR,(r) et les énergies monoélectroni-
ques En! (Herman and skillman 1963). Le potentiel VHS(r) n'a
un
bon
comportement
asymptotique
que
si
on
introdui t
la
correction de Latter (1955).
Le potentiel
VHS(r)
a été employé dans de
très nom-
breuses études de
photoionisation,
surtout à partir de l'é-
tat
fondamental des atomes neutres (Manson and Cooper 1968,
34
Combet farnoux
1969,
Manson
1977) ,
des
ions
(Reilman
and
Manson
1979),
à
l' intér ieur
de
séquences
isonucléaires
(Missavage et al.
1977,
Reilman and Manson 1978) ou
isoélec-
troniques
(Combet farnoux
and
Lamoureux
1976,
Msezane
and
al.
1977),
et
pour
un
grand
nombre
d'orbi tales
de
sous-
couches surtout internes.
Il a également été utilisé dans la
photoionisation
des
états
excités,
surtout
des
alcalins
(Msezane
and
Manson
1975,
1982,
Lahiri
and
Manson
1982).
2.2) Le modèle Hartree-Fock
Le
modèle
Hartree-Fock
est
le
plus
élaboré
de
tous
les
types
de
modèle
à
particules
indépendantes.
Il
tient
compte,
de manière
self-consistante,
des
interactions
élec-
trostatiques
(directes
et
d'échange)
entre
tous
les
élec-
trons.
La
fonction
d'onde
radiale
initiale
discrète
Pnl(r)
est
solution
du
système
d'équations
intégra-différentielles
Hartree-Fock,
obtenu
par
application
du
principe
variation-
nel
à
la
fonctionnelle
de
l'énergie
(Hartree
1957,
Slater
1960,
Cohen
and
Mc
Eachran
1980).
Lorsqu'un
électron
est
dans
le
continuum,
la
méthode
Hartree-Fock
(HF)
n'est
pas
valab le.
On
procède
alors
en
deux
ét apes
(Seaton
1951 t
Chang and Mc Dowell 1968, Kennedy and Manson 1972)
en calculant
d'abord les (N-1)
fonctions radiales correspondant aux élec-
trons
liés
de
l'ion
positif
XZ+
restant
après
ionisation,
par
la
méthode
HF
précédente.
Puis
on
résoud
pour
P Et' (r )
une
équation
du
type
HF
obtenue
pour
le
système
initial
X(z-1)+
dans
laquelle
les
termes
de
potentiels
direct
et
d'échange
sont
estimés
à
l'aide des
fonctions
radiales cal-
Z+
culées
pour
X
et
donc
où
PEt,(r)
est
la
seule
inconnue.
Lorsque
les
fonctions
radiales
de
XZ+ sont
différentes
de
ce Il es des
(N -1) é l e ct r ons pas s ifs de X( Z -1 ) + ce mad è lep r end
en compte la relaxation du
coeur.
Le
modèle
HF
a
été utilisé pour
la photoionisation à
partir
des
états
fondamentaux
des
alcalins
(Seaton
1951,
Mc Dowell
1969)
et
des gaz
rares
(Kennedy and Manson 1972),
35
de quelques états excités des alcalins (Msezane 1983, Mseza-
ne and
Manson 1984) et des éléments de
transition Cu et Ag
(Msezane and Lee 1985).
3) Modèles à particules indépendantes incluant des effets
relativistes
Jusque
là
nous
avons
traité
la
photoionisation
dans
l'approximation
non
relativiste.
Les
effets
relativistes
peuvent avoir de l'importance dans bien des cas, en particu-
lier pour le calcul des minima non nuls des sections effica-
ces
de
photoionisation à
partir
des
états
fondamentaux
des
alcalins
(Seston
1951,
Marr
and
Creek
1968),
minima
qu'on
trouve
nuls
à
l'approximation
non
relativiste.
La prise en
compte
des
effets
relativistes
se
fait
souvent
dans
le
cadre du modèle à particules indépendantes.
3.1) Traitement approché des effets relativistes
modèle »semi-relativiste»
Le modèle
»semi-relativiste"
tient compte uniquement
des corrections relativistes d'ordre ~2 (~ étant la constan-
te
de
structure
fine)
introduites
dans
l'approximation
de
Pauli.
Dans
l'approximation du champ central, des orbitales
radiales
prenant
en
compte
la
plus
grande
partie
de
ces
effets
relativistes
sont
obtenues
en
ajoutant
le
terme
de
spin-orbite V
(r) = ~ l d~(r) t.~ au potentiel central
s.a
L
r
r
Ver) = V (r) + V
1er) de l'équation non relativiste (1.47).
a
po
On obtient ainsi des
fonctions radiales
P 1 0
et P l' 0'
où
-+
-:t'
-+..,.
-:t'
-+
n
J
e
J
j
= ) ( .
+
S
(J'
= )(., + s'). Ce modèle a été utilisé pour étu-
dier
la
photoionisation
à
partir
des
états
fondamentaux
(Weisheit 1972a,
Norcross 1973)
et excités (Weisheit 1972b,
Hofsaess 1977) des alcalins.
Il permet de reproduire les mi-
nima non nuls observés pour les sections efficaces des alca-
lins plus lourds.
36
3.2) Modèle relativiste à champ central
La
manière
la
plus
correcte
pour
prendre
en
compte
les effets relativistes consiste à déterminer les fonctions
propres
relativistes
solutions
du
Hamiltonien
de
Breit-
Dirac.
Les expressions des sections efficaces de photoioni-
sation
à
employer
lorsqu'on
utilise
des
fonctions
d'onde
relativistes décrites par Pratt et al.
(1973) et Walker and
Waber (1973) ne sont pas détaillées ici. Les fonctions d'on-
de
relativistes
peuvent
être
calculées
dans
le
cadre
d'un
modèle à potentiel central. La généralisation relativiste du
modèle de Hartree-Slater, ou méthode du potentiel central de
Dirac-Slater,
a
été
utilisée
pour
calculer
essentiellement
les
sections
efficaces
des
orbitales
internes
des
éléments
neutres
lourds
(Tambe
and
Manson
1984)
et
des
ions
multi-
chargés
(Ong
et
al.
1979)
dans
leur
état
fondamental,
et
étudLer
les déplacements des minima
des sections efficaces
(Kim
et
al.
1981)
par l'apport au
cas non relativiste.
Nous
utilisons dans le chapitre II le modèle du potentiel central
paramétrique relativiste (Luc-Koenig 1972) qui est une géné-
ralisation
du
potentiel
paramétrique
de
Klapisch
(1971).
Ceci
permettra de
comparer les valeurs des sections effica-
ces en théories relativiste et non relativiste pour les ions
moyennement lourds et multichargés.
3.3) Méthode de Dirac-Fock
Le
formalisme
de
la
méthode
HF
généralisé
au
cas
relativiste
(Grant
1970)
conduit
aux
équations
de
Dirac-
Fock. La méthode Dirac-Fock a été utilisée pour calculer les
sections
efficaces
de
photoionisation
à
partir
des
états
fondamentaux
des
alcalins
(Chang
and
Kelly
1972,
Ong
and
Manson 1978,
1979)etdes gaz
rares
(Ong and Manson 1980)
et
pour analyser la polarisation des photoélectrons.
37
III.
MODELES AU-DELA DU MODELE A PARTICULES INDEPEN-
DANTES
Tous les modèles à particules indépendantes utilisant
un potentiel central local négligent complètement les effets
de
corrélation entre
les
électrons.
La
méthode HF ne tient
compte que de l'interaction électrostatique entre l'électron
actif et le coeur.
Pour
tenir
compte
des
corrélations
de
manière
plus
complète,
il
faut
recourir
à
des
modèles
théoriques
plus
élaborés.
Nous
ne
détaillerons
pas
ces
méthodes
décrites
dans
plusieurs
articles
de
revue
(Manson
1976,
Burke 1976,
5tarace 1982). an peut distinguer les méthodes qui cherchent
à
améliorer
les
fonctions d'onde des états initial et
final
mis
en
jeu
·dans
l a t ransi t i on
de
ce Il es
qui
di rect ement
tentent
d'améliorer l'élément
de matrice dipolaire.
Dans la
première catégorie se trouvent les méthodes d'interaction de
configuration,
de
"close-coupling"
et
de
matrice
R.
les
méthodes
basées
sur
la
théorie
des
perturbations à
N corps
(MBPT)
ou
sur
l'approximation
de
la
phase
aléatoire
avec
(RPAE)
ou
sans
échange
(RPA)
se
classent
dans
la
seconde
catégorie.
Ces méthodes utilisent en général les fonctions d'on-
de
obtenues
dans
un
modèle
à
particules
indépendantes,
en
général
le
modèle Hf comme point
de départ.
De plus
il
est
possible d'y inclure les effets relativistes.
Ces méthodes ont été assez peu employées pour calcu-
ler des sections efficaces de photoionisation dans les alca-
lins
ou
les
ions
de
leurs
séquences
isoélectroniques.
la
méthode
"close-coupling"
a
permis
d'obtenir
la
section
efficace
de
photoionisation
à
partir
de
l'état
fondamental
de
Na (Butler and Mendoza 1983)
et à
l'intérieur de
la sé-
quence isoélectronique de Na (Butler et al.
1984). La photo-
38
ionisation des
états
fondamentaux
de
Na et K a été étudiée
par
la MBPT
(Chang 1974).
La version relativiste de
la RPAE
a
été
utilisée
pour
étudier
la
photoionisation
des
états
fondamentaux
des
alcalins
(Johnson and
Soff 1983,
Fink and
Johnson
1986).
Les
caractéristiques
de
la
photoionisation
des
états
exci tés
nd
de
Rb
et
Cs ont
été obtenues à l'aide
de la RPAE (Avdonina and Amusia Ya 1983).
IV.
RESULTATS ANTERIEURS CONCERNANT LES ETUDES SYSTE-
MATIQUES DES CARACTERES NON HYDROGENOIDES DE LA
PHOTOIONISATION
Ce
sont
les
modèles
à
particules
indépendantes
non
relativistes,
en
particulier
ceux
utilisant
un
potentiel
central
non
couloml::1ien
qui
ont
été
le
plus
largement
em-
ployés pour calculer les sections efficaces de photo ionisa-
tian des atomes neutres et des ions.
Les études de photo ionisation qui utilisent les modè-
les
théoriques plus élaborés que le modèle à particules in-
dépendantes sont peu nombreuses et
fragmentaires.
Les modè-
les
tenant compte des corrélations conduisent à des calculs
bien plus longs et plus compliqués qui ne sont justifiés que
pour
des
études
très
ponctuelles.
De telles études sont
en
général
réalisées
lorsque
les modèles
les
plus
simples
ne
permettent
pas
de
reproduire
correctement
les
résultats
expérimentaux.
Le
modèle
à
particules
indépendantes
est
bien
plus
approprié
pour
une
phase
exploratoire
permettant de
mettre
en évidence des propriétés nouvelles,
de dégager des carac-
tères
généraux,
et
donc
pour
des
études
de
systématique.
Bien souvent ces caractères conservent toute leur généralité
en utilisant les modèles plus élaborés (Avdonina and Amusia
Ya
1983).
Les
résultats
de
photoionisation
concernant
la
39
série
de
Rydberg
ns
(n
~ 14)
de
Na (Aymar 1978)
indiquent
par exemple,
que les effets dQs aux diverses corrections de
corrélation par
rapport
au modèle du potentiel central sont
surtout
importants
pour
l'état
fondamental
et
les
états de
Rydberg peu excités.
La relative simplicité du modèle à potentiel central
a rendu possible l'exploration
systématique de
la photoio-
nisation
à
partir
des
états
fondamentaux
de
nombreux
élé-
ments du tableau périodique ; ces études ont permis de déga-
ger les caractéristiques non hydrogénoldes de
la photoioni-
sation des états
fondamentaux
et leur évolution en fonction
de Z,
z et N.
Le
principal
caractère
non
hydrogénolde
concerne
la
présence d'un minimum appelé minimum de Cooper (1962),
dans
la courbe de section efficace crn~(€). Il est à noter que ce
minimum
a été observé
pour
la
photoionisation des
alcalins
(Mohler and Boeckner 1929, Ditchburn et al .. 1943) bien avant
que
les
théoriciens
n'en
donnent
une
interprétation
claire
(Bstes 1947,
Seston 1951,
Cooper 1962).
Un autre
caractère
non hydrogénolde concerne la présence de maxima mis en évi-
dence
expérimentalement
dans
les
gaz
rares
(Ederer
1964,
Jaeglé et al. 1967).
Les études théoriques de
systématique de
la photoio-
nisation
des
états
fondamentaux
concernent
soit
la
couche
externe,
soit
les
couches
profondes
(Manson
1977,
Starace
1982).
Pour les atomes neutres l'évolution en fonction de
Z
a été étudiée en particulier
par
Manson and Cooper (1968) et
Combetfarnoux
(1969,
1971).
Ces études ont
été étendues à
certaines séquences isoélectroniques -
évolution avec z à N
constant
(Lamoureux
and
Combet farnoux
1974,
Combet
farnoux
and La.oureux 1976,
Msezan·e et
al.
1977).
D'autres
études systématiques concernent l'évolution en fonction de z
le
long de
séquences
isonucléaires -
Z constant -
(Combet
40
farnoux
and
Lamoureux
1976,
Reilman
and
Manson 1978,
Chao
and Manson 1981).
En ce qui concerne la photoionisation des états exci-
tés des atomes neutres ou des ions, lorsque nous avons abordé ce
travail
il y avait très peu d'études systématiques,
et ceci
même pour
les systèmes à un électron de valence.
L'étude de
la systématique
de
la
photoionisation
des
états excités
le
long
des
séries
de
Rydberg
des
alcalins
légers
Li-K
avait
été abordée au Laboratoire à l'aide de
la méthode du poten-
tiel paramétrique de Klapisch (1971) par Aymar et al.
(1976)
et Aymar (1978). Ces travaux ainsi que ceux entrepris simul-
tanément dans Cs par Msezane and Manson (1975) ont permis de
prévoir
l'existence de
minima multiples dans les courbes de
sections
efficaces crni,i,(e:)
des états excités,
minima
ja-
mais observés
ou
prédits
pour
la
photoionisation des
états
fondamentaux.
Par ailleurs de nombreuses études ponctuelles,
essentiellement
théoriques,
portant
sur
des
états
excités
des
alcalins
ont
mis
en
évidence
divers caractères non
hy-
drogénoldes
marqués
près
des
seuils,
non
prédi ts
pour
la
photoionisation des états fondamentaux
(Chichkov and Shevel-
ko
1981,
Avdonina
and
Amusia
Va
1983,
Lahiri
and
Manson
1982,
1986).
Nous
reviendrons au chapitre II sur les résul-
tats
obtenus
par
l'équipe
de
Manson,
parallèlement
aux
notres, concernant la systématique de la photoionisation des
états excités.
En ce qui concerne la photoionisation des états exci-
tés d'autres atomes à un électron de
valence,
les résultats
théoriques
étaient
et
sont
toujours
fragmentaires
(Msezane
and Lee 1985).
Pour
les
ions
monovalents
il
n'existait
pour
ainsi
dire
aucun
calcul
concernant
la
photo ionisation
des
états
excités,
excepté ceux réalisés par Burgess et Seaton (1960)
et donc bien sOr aucune systématique. Par contre des résul-
41
tats
avaient
été obtenus
pour
la
photo ionisation des
états
fondamentaux des premiers éléments des séquences isoélectro-
niques des alcalins (Hc Dowell and Chang 1969, Hc Ginn 1970,
Black
et
al.
1972,
Shevelko
1974,
Tiwari
et
al.
1975,
Reilman
and
Hanson
1979).
Ces
études
ont
mis
en
évidence
certains caractères non hydrogénoldes particuliers aux ions,
et leur évolution le long des séquences isoélectroniques des
alcalins.
Ce travail a pour but d'étendre et de généraliser les
études précédentes portant sur la photo ionisation des états
excités
des
systèmes
à
un
électron
de
valence.
En considé-
rant
un
grand
nombre d'états excités
pour divers atomes et
ions monovalents, nous étudions la systématique de la photo-
ionisation
pour
la
séquence
des
alcalins,
les
séquences
isoélectroniques des alcalins et les séquences isoléectroni-
ques homologues à celles des alcalins.
Nous mettons l'accent
sur les caractères non hydrogénoldes de la photoionisation au
voisinage
du
seuil
dl ionisation,
en
insistant plus parti-
culièrement sur l'existence des minima des sections effica-
ces
de
photoionisation.
Nous
étudions
l'évolution
de
ces
caractères
le
long
des
séquences
étudiées
et
le
long
des
séries de Rydberg de chaque élément étudié.
Nous
avons
utilisé
un
modèle
de
potentiel
central
non
relativiste, puis
nous
avons
évalué
l'influence
des
effets relativistes sur les sections efficaces de photoioni-
sation
des
ions
mul tichargés
moyennement
lourds
à
l'aide
d'un modèle relativiste à champ central.
La systématique de
nos résultats est analysée en utilisant la théorie du défaut
quantique.
42
B. RECOMBINAISON RADIATIVE DES ATOMES ET DES IONS
Nous
rappelons
dans
la
section
1 de
cette
partie
B
les
définitions
et
la
signification
physique
des
grandeurs
fondamentales
qui
caractérisent
la
recombinaison
radiative.
Nous
donnons
ainsi
les
expressions
générales
de
la
section
efficace
de
recombinaison
rad i a ti ve
et
des
co e f fic i e n t s
de
recombinaison
radiative.
Les
modèles
théoriques
utilisés
dans
les
calculs
de
recombinaison
radiative
sont
décrits
dans
la section II.
Nous présentons dans la section III
les
résultats obtenus antérieurement sur la recombinaison radia-
tive des systèmes à un électron de valence, et particulière-
ment des alcalins et des ions de leurs séquences isoélectro-
niques.
1. DEFINITIONS - FORMULES GENERALES
Nous nous intéressons principalement à la recombinai-
son radiative des systèmes à un électron de valence, et nous
nous
limiterons
à
des
définitions
et
formules
générales
relatives
à
ces systèmes.
Celles-ci sont
facilement généra-
lisables à des systèmes électroniques plus complexes.
1) Définitions
Dans
le
processus
de
recombinaison
radiative
des
systèmes
monovalents
que
nous
considérons,
un
ion
XZ +
de
charge
Z
dans
son
état
fondamental
ini tial
1S
se
combine
o
avec
un
électron
libre
incident
pour
produire
un
atome
ou
ion x(z-1)+ de charge
(z-1)
dans un état final nt 2L. Dans le
même
temps
un
photon
de
fréquence
v
est
émis
suivant
le
schéma
(1.53)
43
Le nombre
QnR. (\\l)d v de
photons émis par unité de volume et
unité
de
temps
dans
l'intervalle
(\\l,\\l+d\\l)
correspondant
à
l'intervalle de
vitesse
(v,v+dv)
nous
permet
de
définir
la
section efficace de capture radiative cr;~ (v) à l'aide de la
relation (Agnew and Su. .ers 1965, Rothe
1969)
:
( 1. 54)
Dans
l'équation
(1.54),
N
est
le
nombre
d'électrons
par
e
unité de volume,
N
le nombre d'ions XZ+ par unité de volu-
+
me,
v la
vitesse
relative de
l'électron incident,
f(v)
la
fonction
de
distribution
normalisée
des
vitesses
des
élec-
C
trons libres, et crnR.(v) a la dimension d'une surface.
Le coefficient de
recombinaison radiative sur l'état
nR. est défini par la moyenne sur la vitesse :
(l.55)
Il
appara.tt
d'après
(1.54)
et
(1.55)
que
N Nan (T)
repré-
e +
nX.
sente
le
nombre
de
recombinaisons
radiatives
sur l'état nR.
par unité de volume et unité de temps.
Le
coefficient
de
recombinaison
radiative
sur
la
couche n se déduit de anR.(T)
par
n-1
an(T) =
~ anR.(T)
(1.56)
R.=O
Le coefficient de recombinaison radiative total sur tous les
états s'écrit:
a
(1.57)
t (T) =
L an (T)
n:n o
où
no
correspond
à
la sous-couche ou couche non occupée la
(z-1)+
pl us basse de X
•
44
2)
Expressions générales
Le processus de capture (1.53) dans lequel l'électron
incident
passe
d'un
état
libre à
un état
lié avec émission
d'un
photon
est
l'inverse
du
processus
de
photoionisation.
L'expression de
la section efficace de
recombinaison radia-
e
tive
an.t (v)
peut
être
obtenue
directement
à
l'aide
de
la
règle d'or de Permi (Sobel'man 1972, Hahn and Rule_ 1977), de
manière analogue à celle de
la section efficace de photoio-
nisation.
Plus simplement
a~.t(v) est liée à a~.t(\\)) par le
p r i nci pe
de
mi c r 0 r év ers i b il i t
des
pro ces sus
di r e c t
et
in-
é
verse (Massey 1969, Sobel'man 1972)
:
(1. 58)
où c est
la
vitesse de
la lumière et p l'impulsion de
l'é-
lectron.
En tenant compte de la relation
(1. 59)
où e:
est
l'énergie cinétique de
l'électron incident et
In.t
le potentiel d'ionisation de l'électron capturé, l'intégrale
sur les
vitesses dans (1.55)
peut se transformer en une in-
tégrale
portant
sur
e:.
Pour
une
distribution
maxwellienne
des vitesses des électrons
2
mkT)
f( v, T) = 41TV (21T
3/2 exp (_~~~)
( 1. 60)
on obtient alors :
2
ex n.t ( T)
= (3 286 . 34 ) 2 ( 2.t+ 1 ) ( k T) - 3/ Sco (e: + l n.t ) 2a~.t ( e ) exp (-TIJde:
o
(1.61)
où k est la constante de Boltzman,
T la température électro-
nique.
Toutes
les
énergies
(e:,
In.t'
kT)
sont
exprimées
en
45
Rydbergs,les sections efficaces
~ -1
Cm S
•
II. MODELES THEORIQUES
Les sections efficaces de capture et les coefficients
de recombinaison radiative sont en général calculés à partir
des sections efficaces de photoionisation.
1) Modèle hydrogénolde
Nous rappelons les résutlats des modèles hydrogénolde
et de
Kramers
pour les coefficients de
recombinaison radia-
tive.
1.1) Calcul exact. Lois hydrogénoldes
Pour l'hydrogène et les ions hydrogénoides,
les coef-
ficients
de
recombinaison
radiative
peuvent
être
calculés
exactement à
partir des expressions analytiques connues des
sections
efficaces
de
photoionisation
(Gordon
1929).
Le
coefficient de recombinaison radiative aZ(T) d'un ion hydro-
génoide
de charge Z est
relié à celui de
l'hydrogène par:
(1.62)
Boardman
(1964)
a
ainsi
calculé
aH n (T)
pour
n
=
1 -10,
3
6
nX.
~
= 0- (.n-1), 10
< T < 10
K.
Burgess
(1964)
a déterminé
a~~(T) pour
2
n =
1-20, ~ = 0-(n-1), 0 ~ T/z
< œ.
Les caractères hydrogénoIdes spécifiques sont détail-
lés dans l'annexe II (voir en particulier la figure 1). Pour
~ et T fixés, a~~ a une décroissance monotone avec n pour
~ < 3 et présente un maximum pour
~ > 3. Pour n et T fixés
46
l'importance relative des
a~R. dépend considérablement de n.
Pour n et
R. fixés,
a~R.(T) a une décroissance monotone avec
T. Cette même décroissance a donc lieu pour a~(T) et
a~(T).
1.2) Modèle de Kramers et approximation de Kramers-
Gaunt
Le modèle hydrogénolde de
la
recombinaison radiative
est
d'importance
théorique
fondamentale
puisqu'il
permet
d'avoir
des
résultats
exacts.
Il
est
d'utilité pratique
du
fait
qu'il constitue une bonne approximation pour la recom-
binaison radiative sur des états très excités de systèmes à
plusieurs
électrons,
en
particulier
de
systèmes
à
un
seul
électron de valence.
Il y a souvent besoin de calculer beau-
coup
de
coefficients
de
recombinaison
correspondant
à
un
grand
nombre
d'états
excités.
Le
calcul
direct
de
a~R.(T)
devient
difficile
et
compliqué
lorsque
n
devient
grand
(Burgess
1964).
On utilise alors des expressions approchées
pour
les
coefficients
de
recombinaison
radiative.
En
se
servant de l'approximation de Kramers de la section efficace
de photoionisation (1.41) on obtient:
2
3/2
2
2
a~r(z,T)
14
3
1)z(+-J
=(S.197X10-
cm s -
ex p(+-IE 1 (+-)(1.63)
ln kT
n kT)
n kT
al
1dt.
où
E
= f exp(-t)t-
1(x)
x
Les
coefficients
a~~ (z , T) sont alors en général déduits de
a~r(z,T) en utilisant la relation
Kr(
) _ 2R.+1
Kr(
T)
anR. z,T
- ~n
z,
•
( l .64 )
n
Des écarts importants par rapport aux valeurs exactes
des
coefficients
de
recombinaison
peuvent
se
produire
pour
les
résultats
du
modèle
de
Kramers,
écarts croissants
avec
la
température.
Une
amélioration
importante
de
ces
résul-
tats
est
obtenue
en
utilisant
l'approximation
de
Kramers-
47
Gaunt (équation (1.42)~ Il vient alors:
2
3/2
2
14
3
(1.65)
C
c ~ (T) = (5. 197 x 10-
cm s -1 ) z
~kTJ
5n (~T)
où
Sn(h) = (exP(-):rU) ( 1+U) - 1gn(U) dU.
a
5
Pour
des
températures
relativement
faibles
TIz 2
< 10
K,
diverses
expressions
simplifiées
d'usage
plus
pratique
ont
été obtenes (voir annexe II) pour ()~r(z,T) et ()~(T).
Par
ailleurs
plusieurs
auteurs
(Hahn
1975,
Hahn
and
Rule
1977,
Lee and Pratt 1976,
Kim and Pratt 1983)
ont cal-
culé
des
sections
efficaces
de
capture
d'électrons
très
énergétiques par des
ions très chargés en
partant de
formu-
les de Kramers modifiées pour la section efficace de
photo-
ionisation.
Ces
formules
introduisent
des
facteurs
de
cor-
rection
qui
tiennent
compte
de
l'écrantage
incomplet
du
noyau
par
les
électrons
;
ainsi
divers calculs ont été ef-
1
fectués
en
introduisant
une
charge
effective
Zeff
= ï( z+Z)
dans la formule (1.41) de
Kramers.
2)
Autres modèles théorigues
De nombreux
calculs de
coefficients de recombinaison
radiative
()n et ()t
ont
été
réalisés en combinant
le modèle
hydrogénolde
à
des
modèles
plus
réalistes
tenant
compte
du
fait
que
l'état
fondamental
et
les
états
moins
excités
de
(z-1)+
'.'
X
ne sont pas hydrogénoldes. Les coefficients ()n! pour
ces
états
profonds
sont
en
général
dédui ts
des
sections
efficaces
calculées
par
la
méthode
du
défaut
quantique
(Moskvin
1963,
Norcross and Stone
1966) ou
les méthodes du
champ central décrites
dans la partie A (Caves and Oalgarno
1972,
Barfield 1980,
Woods et al.
1981).
Une autre approche
utilisée
par
Lee
and
Pratt
(1975,
1976)
pour
calculer
des
sections
efficaces
de
capture
consiste
à
relier
la densité
de
section
efficace
de
capture
(transition
libre-lié)
à
la
48
section
efficace
de "Bremstrahlung" (transition
libre-libre)
en utilisant la théorie du
défaut quantique.
III.
RESULTATS ANTERIEURS OBTENUS POUR LA RECOMBINAI-
SON RADIATIVE DES ATOMES ET DES IONS
Les
études
théoriques
antérieures
concernent
la
recombinaison
radiative
d'électrons
soit
très
énergétiques
(kT »
1 eV,
1 eV correspondant à une température électroni-
4
que
de
1.2x10
K),
soit
au
contraire
très
peu
énergétiques
CT <
5
10
K).
Dans
la
première
classe
de
travaux,
les
résultats
concernent
des
ions
très
chargés intervenant dans les plas-
mas
d'astrophysique
OIJ
les
impuretés
apparaissant
dans
les
plasmas
de
fusion
thermonucléaire
contrôlée
(Hahn
1975,
Hahn
and
Rule
1977,
Lee and
Pratt 1976,
Barfield 1980,
Kim
and Pratt 1983). La plupart de ces études prennent en compte
certains
effets
relativistes.
Nous
ne
détaillerons
pas
ces
travaux qui ont permis d'obtenir certaines lois d'échelle en
fonction
du
nombre de
charge
Z,
de
la charge
de
l'ion
z
et
de l'energie des électrons incidents.
Tous
les
calculs
que
nous
avons effectués concernent
des
systèmes
recombinés
à
un
électron
de
valence
pour
des
5
températures
électroniques
T
<
10
K.
Il
s'agit
de
calculs
de
recombinaison
radiative
dans
K,
Rb,
Cu
et
Ag
ainsi
que
dans
certains
ions de
leurs séquences isoélectro-
5
niques.
Dans
la zone de
température T < 10
K les résultats
antérieurs
sont
très
fragmentaires.
En
ce
qui
concerne
les
alcalins
ou
les
ions
de
leurs
séquences
isoélectroniques,
les
r
s u I tats
portent
sur
quelques
cxn.t (T)
de
Cs
(Norcross
é
and
Stone
1966,
Weisheit
1972b),
quelques
cxn.t (T)
et
cx (T)
t
de Li
(Caves and Dalgarno 1972),
les cxt(T)
de tous les alca-
lins Li-Cs
(Moskvin 1963) et
finalement
sur
les cx (T)
des
t
49
ions
Ca+
(5hull
and
5teenberg
1982)
et
Fe 7+
(Woods et
al.
1981). Aucune étude systématique n'a été réalisée. Le but de
notre travail est d'étudier les caractères non hydrogénoldes
de la recombinaison radiative le long des séquences isoélec-
troniques de K et Rb et de celles des éléments homologues Cu
et
Ag,
et
d'analyser
la
systématique
des
coefficients
de
recombinaison radiative à faible température.
51
CHAPITRE
II
P!:IOTOIONlSATION E,T RECOMBINAISON RADIATIVE DANS
LES SEQ..U,ENŒSI ~LECTRON 1QUES DU POTASS1UFt.-.ID!
RUBIDIUM, DU CUIVRE ET DE L'ARGENT
L'objet de notre travail est l'étude de la systémati-
que de
la photoionisation des états excités et de
la recom-
binaison
radiative
dans
les
séquences
isoélectroniques
des
alcalins K et Rb,
et dans les séquences isoélectroniques de
leurs éléments homologues Cu et Ag.
Dans ce chapitre nous résumons les résultats de cette
étude dont l'essentiel figure dans les articles déjà publiés
présentés
en
annexes.
Nous
récapitulons
tout
d'abord
le
contenu des articles puis nous donnons une présentation glo-
bale de
nos résultats dans la par~e A pour la photoionisa-
tian
et
dans
la
partie
B pour
la
recombinaison
radiative.
Nous
y mentionnons
les
points
les
plus
importants de
notre
étude
et
nous
illustrons
les
résultats
les
plus
marquants
par des exemples significatifs.
Dans l'annexe
I,
le modèle théorique utilisé pour le
calcul des sections efficaces de photoionisation est défini,
et
les
méthodes
numériques
de
calcul
mises
en
oeuvre
pour
l'obtention des sections efficaces sont données en appendice.
Dans le cadre de ce modèle les sections efficaces de photo-
ionisation
à
partir
des
états
fondamentaux
et
excités
nR.
(n ~ 20, 0 ~ 9.. ~ 4) de Rb et s-" ont été calculées.
L'exis-
tence
de
minima
et
de
maxima
dans
les
courbes
de
sections
efficaces
de
photoionisation
près
des
seuils,
l'évolution
des caractères non hydrogénoldes le long de séries de Rydberg
52
ns-ng et leur variation isoélectronique de
Rb à Sr+ sont ana-
lysées à l'aide de la théorie du défaut quantique.
La métho-
de
d'analyse de la systématique des caractères non hydrogé-
noides de la
photoionisation des états excités est exposée.
L'étude de la systématique est étendue aux autres alcalins Li,
Na,
K et Cs pour lesquels on dispose de résultats antérieurs.
Dans l'annexe II,
le modèle théorique utilisé pour le
calcul des coefficients de
recombinaison
radiative pour les
systèmes
recombinés
à
un
électron
de
valence est
défini, et
les méthodes numériques pour l'obtention de ces coefficients
à
partir des sections efficaces de photoionisation sont in-
diquées.
Dans le cadre de
ce modèle les coefficients de re-
combinaison radiative o.ng,(T)
(n ~ 20,
Q.
~ 10), o.n(T) (n ~ 10)
et o.t (T)
ont
été
obtenus
dans
l'intervalle
de
température
500 ~ T ~ 6000 K pour Rb.
Les résultats ont été analysés et
les caractères non hydrogénoides de
la recombinaison radia-
tive dans Rb mis en évidence.
A titre de comparaison les ré-
sultats
spécifiques
de
recombinaison
des
modèles
hydrogé-
n o Ld e
et
de Kramers
et
de
l'approximation de
Kramers-Gaunt
ont été explicités.
L'annexe
III
concerne
la séquence
isoélectronique de
K. L'étude de la photo ionisation des états excités au
voisi-
"1
'
é
K F 7+
Z 11+
17+
nage des seUl s est realis e pour
- e
,
n
, K r
et
2 3
M0
+ , celle de la recombinaison radiative dans l'intervalle
3+,
7+
2 3
500 ~ T ~ 10000 K pour K_Ti
Fe
et M0
+ .
Les
modèles
théoriques
de
calcul
et
d'analyse
de
la
systématique
des
caractères
non
hydrogénoides
sont
ceux
utilisés
dans
I
et
II.
L'évolution
de
ces
caractères
le
long
de
la
séquence
isoélectronique est analysée en détail.
L'annexe
IV complète
les
annexes
I
(photoionisation
des états excités de
Rb et Sr+)
et
II
(recombinaison
radia-
tive de
Rb)
en considérant d'autres éléments de
la séquence
53
isoélectronique de Rb : y2+_ Xe17+. De plus cette annexe pré-
13+
sente les résultats obtenus dans les
éléments
Cu-Mo
et
Ag_Xe 7+ des séquences
isoélectroniques
de Cu et Ag,
homolo-
gues à celles du K et Rb.
La systématique des caractères non
hydrogénoldes le long d'une séquence et le comportement sem-
blable
ou
di fférent
des
séquences
de
K,
Rb Cu et
Ag
sont
analysés
par
la
méthode
précédente basée
sur la
théorie
du
défaut
quantique.
La
recombinaison
radiative
des
éléments
Sr+_y2+, CU-Ga 2+ et Ag_Sn 3+
a
été étudiée dans
l'intervalle
de
température réduite 500 ~ T'
~ 5000 K, et la systématique
des caractères non hydrogénoldes de
la recombinaison à l'in-
térieur des séquences isoélectroniques a été analysée.
A.
PHOTOIONISATION
DANS
LES
SEQUENCES
ISOELECTRONIQUES
DU
POTASSIUM, DU RUBIDIUM, DU CUIVRE ET DE L'ARGENT
Nous
présentons dans
la partie A les résultats de
la
photoionisation
des
états
fondamentaux
et
excités dans
les
séquences
isoélectroniques
des
alcalins
K et
Rb,
et
dans
celles
de
leurs
éléments
homologues
Cu et Ag.
Les sections
efficaces ont été calculées dans le cadre d'un modèle mono-
électronique
non
relativiste
à
champ
central
présenté
dans
la section 1. La section II montre comment la théorie du dé-
faut
quantique
permet
d'analyser
les
caractères
non
hydro-
énoldes
des
sections
efficaces.
Les
résultats
concernant
es
caractères
non
hydrogénoIdes
des
sections
efficaces
de
hotoionisation sont présentés dans
la section III. La sec-
ion IV présente une discussion de
la validité des résultats
btenus
et
des
comparaisons
avec
les
résultats
antérieurs.
es
calculs
de
section
efficace
ont
été réalisés en
utili-
ant un modèle non relativiste.
La validité d'un tel
trai-
ement
pour
les
ions
multichargés
a
été vérifiée en calcu-
ant
quelques sections efficaces
à l'aide d'un modèle
rela-
54
tiviste
à
champ
central.
Ces
résultats
sont
présentés
dans
la section V.
1. MODELE
THEORIQUE
UTILISE
POUR
LE CALCUL
DES
SEC-
TIONS EFFICACES DE PHOTOIONISATION
Le
modèle
théorique
que
nous
avons
utilisé
pour
le
calcul des sections efficaces de
photoionisation est un mo-
dèle
monoélectronique
non
relativiste,
à
potentiel
central
non coulombien.
L'expression de
la section efficace de
pho-
toionisation
à
partir
d'un
état
n2. d'un
système à un
élec-
tron
de
valence est
donnée
à
l'approximation dipolaire
par
l'équation (1.30).
Les fonctions d'onde
radiales
Pn~(r) et
P n,(r)
sont solutions de
l'équation de
Sc h r o d i n q e r (1.47).
. e: x.
Dans
notre
étude
nous
utilisons
le
potentiel
paramétrique
introduit par Klapisch (1971), déjà utilisé dans des calculs
de
photoionisation
des
états
excités
des
alcalins
légers
(Aymar et al.
1976,
Aymar 1978). Les fonctions d'onde radia-
les
sont
calculées
en
utilisant
quatre
potentiels
centraux
différents V(r)
:
a) Le potentiel central a une forme analytique simple
dépendant de trois paramètres ;
Les paramètres a , a
et a
sont déterminés en comparant les
1
Z
3
énergies expérimentales avec celles calculées à l'ordre zéro.
Ce potentiel a été utilisé pour Rb,
Sr+,
et
les
éléments
K_Ti 3+
de
la séquence de
K pour lesquels les énergies expé-
rimentales sont connues .
b )
Nous
tenons
compte
des
effets de
la polarisation
du coeur en ajoutant au potential V (r )
défini
en
a)
un
po-
o
tentiel effectif de polarisation V
l(r) de forme:
po
55
(II.2)
où Ct
est la polar isabilité dipolaire statique du coeur (Shevelko and
d
Vinogradov 1978, Chickhov and Shevelko 1981) et r
est le rayon de cou-
c
pure effecti f du coeur. Les paramètres Ct ' C'tz'
et r c sont déterminés
1
Ct3
en comparant les valeurs expérimentales des énergies à leurs valeurs ca~
culées à l'ordre zéro.
Par ailleurs,
l'élément de matrice de
transition dipolaire est modifié et devient l'équation (1.51)
0Cl
Rn~,~,(E) = f Pn~(r)O(r)PE~,(r)dr. L'opérateur dipolaire mo-
o
difié OCr)
qui inclut les effets de
polarisation du coeur a
la forme
(Hameed et al. 1968, Weisheit 1972a,b)
(IL3)
Le potentiel Ver) = V (r) + V
1er) a été utilisé pour Rb-Sr+,
2+
2+
0
po
Cu-Ga
et Ag-In
c) Le potentiel central Ver) est le potentiel paramé-
trique
introduit par
Klapisch
(1971).
Il est représenté par
une
fonction analytique
dépendant
d'un
jeu
de
paramètres,
chaque
paramètre
décrivant
la
distribution
de
charge
d'une
couche du coeur. Le potentiel optimal est déterminé en mini-
misant
Itécart quadratique moyen entre les énergies expéri-
mentales et les énergies calculées au
premier ordre.
Ce po-
tentiel a été utilisé pour Rb et Sr+.
d) Le potentiel
Ver)
est semblable à celui considéré
précédemment. Seul le critère d'optimisation change.
Les pa-
ramètres sont
ici
déterminés en
minimisant l'énergie totale
de
l'état
fondamental.
Ce potentiel ab-initio a été utilisé
pour
tous
les
éléments
des
séquences
isoélectroniques
pour
lesquels les énergies expérimentales sont peu ou pas connues.
Le
potentiel
central
choisi
Ver)
étant
spécifié,
l'équation de Schrodinger
(1.47) est résolue et les éléments
de
matrice
de
transition
calculés
en
utilisant
différentes
méthodes numériques décrites dans l'appendice Qe l'annexe 1.
56
II. ANALYSE DE LA PHOTOIONISATION DES ETATS EXCITES
PAR LA THEORIE DU DEFAUT QUANTIQUE
Le
comportement
hydrogénolde
des
sections
efficaces
de
photoionisation a été
rappelé
dans
la section LA.IL2.1.
La comparaison des sections efficaces le long des séquences
isoélectroniques de
K, Rb,
Cu et Ag avec celles de l'hydro-
gène
est
faite
en
introduisant
les
variables
réduites
des
énergies et des sections efficaces
e:
e:'
= '2
z
CII.4)
O"(e:') =
2
2
Z
o Cz e ")
Nous
avons
mis
en
évidence
dans
notre
étude
divers
caractères non hydrogénoldes très marqués de la photoionisa-
tion
au
voisinage
des
seuils.
Nous
en
illustrons
quelques
uns avant d'en faire une analyse plus détaillée par la théo-
rie du défaut quantique.
1) Comportement non hydrogénolde des courbes de sections ef-
ficaces
1.1) Comparaison avec l'hydrogène
La figure 1 représente les sections efficaces totales
O'S1(hV')
(0 ~ 1 ~ 4) pour les états excités
de
Rb
et
Sr+
comparées à celles de l'hydrogène H. Les caractères non hy-
drogénoldes les plus évidents concernent O'Ss(hv')
qui
pré-
sente
un
minimum
suivi
d'un
maximum
pour
Rb et
un
maximum
pour s-". Par ailleurs O'Sp(hV') et O'Sd(hv')
ont
des
valeurs
très différentes de celles de H et une décroissance monotone
à
partir des seuils moins rapide.
57
1.2) Evolution le long d'une série de Rydberg
La figure 2 porte sur les sections efficaces à partir
2+.
des états nd de Sc
La figure 2(a) montre l'évolution avec
n
des
sections
efficaces
partielles
et
totales.
La
courbe
o~d(O) présente un minimum prononcé correspondant à celui de
O~d, f(O). Dans H O'nR.,R.+1(e:) est toujours très supérieur à 0nR.,R._1(e:),
ce qui est loin
d'être le cas ici.
La courbe 2(b)
présente
l'évolution avec n de 0nd(e:),évolution très différente de cel-
le dans H. En effet pour n > 3 toutes les courbes 0nd,f(e:)
présentent des caractères non hydrogénoldes marqués
; ainsi
pour n = 20 (figure 2 (c ) ) and, f(e:) présente un minimum qui en-
t rai n e une dis con tin u i t é de pen tep 0 u rOnd (e: )( fig ure 2 b ) •
1.3)
Variation le long d'une séquence
La figure 3 montre l'évolution de 06d(e:')
le
long
de
3+.
la séquence K_Ti
Les valeurs de 06d(e:')
sont
très
diffé-
rentes
de
celles
de
H
particulièrement
pour
les
ions
;
la
décroissance avec e:' est bien plus lente.
Il est à noter que
+
0"
(e ")
présente un minimum suivi d'un maximum pour Ca,
un
6d
2+
maximum pour Sc
,
et
seulement
une
décroissance
monotone
pour le neutre K.
Pour les ions hydrogénoldes o~R.(O) ne dépend pas de z
(équation
11.4).
On peut
voir
sur
la
figure
4 que
les
va-
leurs de o~R.(O) obtenues dans la séquence de Rb varient con-
sidérablement
avec
z
ces
valeurs
sont
en
général
infé-
rieures à celles correspondant à H. La variation avec z peut
être
soit
régulière
(états
5s
et
20s
pour
z
> 2) ou très
irrégulière (états nd).
2
10
10'
·J) 10°
L
.-b 1()'
00
I f )
10.2
10.3
,
,
,
,
,
,
,
,
,
,
I
~------.~- -
0
0.1
0.2
0.3
0.4-
0.5 0
QI
0.2
03
0.4
0.5 0
. 0.1
01
0.3
0.4
Q5
h\\j(Ryd)
hV'(Ryd)
hV'(Ryd)
@
@
©
fIGURE 1
2
Variation de OSt avec hv' = (€-€8t)/z
pour t
= 0-4,
pour H(a), Rb(b) et Sr+(c).
59
sc t +
b)
c)
3
a ZOd,?
5
0- eo a.r
cr 20d
-.Q1: ta·'
-"2b
~\\ ,------_...-.
10.1
,x....
---
/
"
-"~I'lIlll':~~__ 1
l
"-
,
"-
tO·s
-,-
r--_ _-T'_ _---'
' ........<,
a
0.25 .
O.SO
0.75
o
0.25
0.50
0.75
e (Ryd)
t (R~d)
FIGURE 2
2+
Sections efficaces des états nd de Sc
.
a) Variation avec n des sections efficaces totale
a~d(O)
et partielles a'd f(O)
et o'd
(0) au seuil.
n
,
n
,p
b) Evolution de 0nd(€)
avec n.
c) Sections efficaces totale
et partielles pour
l'état 20d.
60
10-2.-I-_...,....-_-r---....~-,-~--,-_~_-r-_~-..,._~
o
.2.
.4
.6
.8
1.
e' (R~d)
FIGURE 3
Evolution de CT
( e:' )
le long de la séquence de K.
6 d
Comparaison avec CT
( e: )
de H.
6 d
61
2) Analyse du comportement non hydrogénolde des sections ef-
ficaces
Les
valeurs
des
sections
efficaces
partielles et to-
tales des
atomes
et des
ions
non hydrogénoldes peuvent donc
être
très différentes
des
valeurs
hydrogénoldes
ainsi
que
nous l'avons vu. De fait
les orbitales discrète PnJl.(r) et du
continuum P e ' Jl.' Cr ) sont
contractées
vers
le
noyau
par
rap-
port aux orbitales hydrogénoldes.
Le recouvrement de PnJl.(r)
et de Pe:'Jl.,(r)
est
en
conséquence
modifié,
et
l'élément
de
matrice de -t r ans Lt i on Rnt,t, (e:')
n'est
plus
nécessairement
une
fonction
monotone
positive
décroissante
de e '.
En
fait,
RnJl.,Jl.' (e:')
peut
avoir
des
variations
très
diverses.
Sur
la
figure
S sont
schématisés
6 profils typiques qui correspon-
dent
au
seuil
de
photoionisation
(e:'=0)
placé respectivement
en
A,8,C,D,E
et
F.
A ces
profils
correspondent
les
courbes
de section efficace partielle cr~Jl.,t,(e:') de
type
(a)
à
(f).
Les
formes
(a)
de
type
hydrogénolde,
(b )
avec
un
maximum
près du
seuil,
(c ) avec un minimum de
Cooper et
(d)
avec un
maximum
près
du
seuil
suivi
d'un
minimum
caractérisent
les
courbes
de
sections
efficaces
de
photoionisation
à
partir
des
états
fondamentaux
de
nombreux jléments.
Les autres
ty-
pes de courbes
(e) et
(f)
présentant plusieurs extréma,
jus-
qu'à 3 minima pour le type
(f),
apparaissent uniquement pour
la photoionisation à partir de niveaux
excités.
Un caractère
non hydrogénorde
très marqué est
l'existence de minima dans
les courbes cr'n
n,(e:'),
qui
correspondent
aux
zéros
de
nx , JI.
Rnt,Jl.,(e:').
La
théorie
du
défaut
quantique
(Burgess
and
Seaton 1960,
Peach 1967)
rappelée à la section I.A.II.2.1
est
bien
appropriée
pour
discuter
de
l'apparition
des
minima.
La contribution la plus importante à Rnt,t, (c ! )
pro-
vient
des
régions
où
les
valeurs
de
la
variable
radiale
r
sont grandes,
et où
l'électron excité se meut principalement
dans
un
champ coulombien.
Les autres
forces non coulombien-
nes
qui
prévalent
dans
le
coeur
modi fient
les
fonctions
H ~O.o
Rb-like
lOZ
10' 'I--~'~b~~'~~_L
,
,
,
,
l
,
_ _.....JL-_ _....L
.L
L..:"'_.....JL-_ _- 1
Rb-like
H lOd
.
-
Rb Z.Od
_1O
2 ..
Hb 5.0
1O
.D
-
1:
.D
-
1:
-
0
-
""'
1
0
/"'1.
H4d
' - '
."
\\D
C
-
q
N
,
c
,
b
b
10
b)
l ,
1
,
t
,
,
,
,
,
,
a)
1 l
4
6
8
10
Il
14
16
16
10-1 ,I~Z.~'
1
l
4'~;:'--;;'---:~.----,.----,,....--:-J
4
6
'
,
l
'
8
10
12.
14
16
16
~
~
fIGURE 4
Variation avec z des sections efficaces au seuil 0'0(0) le long de la
n,.
séquence de
Rb.
Comparaison avec les valeurs hydrogénoIdes.
a) états ns;
b) états nd.
63
d'onde
radiales
dans
la
région
externe.
Les orbitales
dis-
crète
et
du
continuum
sont
contractées
vers
le
noyau
par
rapport
aux orbitales hydrogénoldes.
Le déplacement
relatif
de l'une par rapport à l'autre est à l'origine du caractère
non
hydrogénolde
de
la
photoionisation.
Le
déphasage
de
l'orbitale discrète n~ est mJn~
et
celui
de
l'orbitale
du
continuum ô~,(€'). La méthode du défaut quantique donne une
dépendance oscillatoire de Rn~,~'(€') en cos 'TTAn~,~'(€')
(équation 1.46) avec
An~ , ~ , ( E,) = -1.1 n~ + ÔQ,' ( € ' ) / 'TT + XU ' ( n , E')
(IL5)
où
le
paramètre
empirique X est
une
fonction
lentement
croissante de n et
E'
(Peach 1967).
L'apparition des zéros
dans RnQ"Q,'(€')
est
reliée
aux
valeurs
demi-entières
de
AnQ,,~I(E').
Au voisinage du seuil, une valeur approchée de An~,~1
peut
être
obtenue
en
utilisant
dans
l'équation
(I1.5)
les
valeurs limites obtenues pour n = = et E' = 0 :
(11.6)
où la valeur asymptotique X(O)
de X peut
être
extraite
des
tables de Peach E1967). La quantité Al.I~~1 = 1.I~,
-
1.I~ repré-
sente
la
différence
des
défauts
quantiques
correspondant
à
de larges valeurs de n.
Une différence de défauts
quantiques
critique
peut être définie telle que RnQ"Q,' (E') ait un zéro:
Lorsque la valeur de
1 Al.I
,
U 1 1
(mod
1)
est très différente de
celle de
IAl.I~Q,,1 (mod 1), le nombre k de zéros de Rnt,t,(E')
est déterminé par les inégalités (figure
5)
:
f
e
,
Rn2,2.
FO 11
U-I
L
/
1...
If.r.."~-=~~,,
e
-.:t
\\0
o:
E'
,
1.A}'01~1
IAJ'° u:I+1
IAI'°ltl+ 2
1
_ _ 1
1
o
I.A}' 11"
fIGURE 5
Eléments de ,matrice dipolaires et sections efficaces partielles typiques. Les courbes
R n n,(E) a à
f correspondent au seuil placé de A à f
;
dans chaque cas seule la par-
n .., , lU
tie de la courbe à droite du trait vertical est significative. Les types de courbes
cr n n,(E)
(a) à
(f) correspondent aux cas a à f de la figure supérieure. Nombre de mi-
n lU, ..,
nima dans crn~,tl(E) suivant les valeurs de 6~~~,.
65
(ILS)
Lorsque
(I1.9)
on observe en général un changement de forme de la courbe de
photoionisation
pour
une
série
de
Rydberg
donnée
lorsque
n
augmente.
En
effet
pour
les
plus
bas
niveaux
d'une
série
donnée,
le défaut quantique ~nR. peut
être
différent
de ~R.'
la valeur limite pour n = ~ ; de plus la fonction X~R.,(n,€')
(équation
11.5)
peut
être
aussi
différente
de
sa
valeur
asymptotique XR.R.,(O).
Le
nombre
critique
k
de
zéros
n'est
alors atteint que pour les états les plus excités.
Les
différentes
formes
de
courbes
dépendent
de
la
di f f r e n cel ~ UR.2! 1 - 1~
é
U~ R. 1 1.
Les
ex e mp Le s pré sen tés dan s la·
section
III montreront
que ce modèle simple décrit bien les
caractères non hydrogénoldes de
la
photo ionisation à partir
des
niveaux excités et leur évolution le long des séries ou
séquences étudiées.
III.
PRESENTATION GLOBALE DES RESULTATS
Les
sections
efficaces
de
photoionisation
ont
été
23+
calculées pour les états nR. (n ~ 20, 0 ~ R. ~ 4 ) de K-Mo
,
7+
Rb X 17+
C
M 13+
-
e
,
u- 0
et Ag-Xe
Seule
la
photoionisation
de
l'électron externe
de
valence
est
considérée
et
les
effets
d'autoionisation sont négligés.
Ce traitement est valable au
voisinage
des
seuils.
Les
calculs
ont
cependant
été
effec-
tués au delà de ce voisinage à des énergies de
photoélectron
plus grandes, en
vue de détecter les divers minima qui appa-
raissent dans lescourbes cr~R.,R.' (E') et d'analyser la systéma-
tique de
ces minima.
Parallèlement à ces calculs,
l'analyse
de
la
photoionisation
des
états
excités
de
la séquence des
66
alcalins
Li-Cs
a été
faite.
Les détails de
tous les
résul-
tats se trouvent dans les annexes
l,
III et
IV.
Nous
en il-
lustrons quelques uns parmi les plus significatifs.
1) Evolution avec n le long d'une série de Rydberg d'un élé-
ment donné
Cet t e
vo lut ion
est
dis c u t é e
sur
l' e xe mp Le
par tic u-
é
lier des sections efficaces de
photoionisation des états nd
2
de
In + (voir annexe
IV).
La figure
(6a) montre l'évolution
de la section efficace totale crnd(E) le long de la série nd.
Les figures (6b) à (6d) montrent les sections efficaces par-
tielles
pour quelques
valeurs
particulières de
n .
La
forme
des courbes cr d
(E) et cr d f(E)
change le long de la série:
n
,p
n
,
lorsque n augmente cr d
(E)
passe
du
type
(a)
au
type
(b )
n
,p
puis au type (c), tandis que crnd,f(E)
change
de
(d)
à
Ce ) •
En effet les valeurs asymptotiques
It.~dpl = 0.74 et lt.~dfl =
1.57 sont proches des valeurs critiques
It.~~pl =
0.75
et
It.~~fl
+
1 = 1.48 caractéristiques respectivement de l'ap-
parition
de
un
minimum
(type
c )
ou
deux
minima
(type
e ) ,
(voir figure 5). Pour n grand (figure
d ) cr d
é
(E) et cr d f(E)
n ,p
n ,
sont
bien
de
type
(c )
et
(e)
respectivement
l'évolution
pour les valeurs de n plus faibles est liée au fait que
~nt
et Xt
'
(équation
II.5)
n'ont
pas
atteint
leurs
valeurs
t
asymptotiques.
Il
est
à
noter
que sur
la
figure
6 seule la
zone près du seuil est représentée,
le second zéro de crnd,f(E)
apparaissant
à
plus
haute
énergie.
L'évolution
avec
n
se
traduit
par
un
déplacement
de
la
position
des
minima
qui
s'éloignent du seuil lorsque n croit puis finalement devien-
nent
stationnaires
pour
n grand.
Les
minima absents pour n
petit affectent en
fait
la distribution des forces d'oscil-
lateur
vers
les
niveaux
discrets
nt et les changements de
forme de
(b) à (c) ou de
(d) à (e) correspondent à un dépla-
cement
du
minimum de EnR. <0 à E > O. Pour les valeurs de no
voisines de ce changement les sections efficaces sont parti-
culièrement faibles.
67
L'évolution
avec
n des
sections efficaces n'est
pas
toujours aussi marquée. En particulier ici les deux sections
efficaces partielles
changent de forme lorsque n augmen-
te et ceci affecte beaucoup l'évolution de la section effi-
cace
totale.
Dans de nombreux cas les caractères non
hydro-
génoldes
ne
sont
visibles
que
sur
les
sections
efficaces
partielles.
Cependant
dans
tous
les
cas
étudiés
on
observe
une
évolution des
caractères hydrogénoldes
pour
les
n fai-
bles uniquement. Pour les n grands les caractères non hydro-
génoldes
se
stabilisent,
la
position
des
minima
devenant
stationnaire.
2)
Séquence des alcalins Li-Cs
Les résultats concernant la photoionisation des états
excités des alcalins sont synthétisés dans la table 1 et la
figure 7.
Dans la table 1,
la forme de chaque courbe
(voir fi-
gure 5) de section efficace partielle crnl,l'(~)
est
donnée
pour chaque transition nl .... ~l'
des alcalins Li-Cs.
Dans la
même table, les différences de défauts quantiques asymptoti-
ques 6~ll' sont comparées aux différences de défauts quanti-
ques critiques 6~~l' (équation II.7) extraites des tables de
Peach
(1967).
La figure
7(a) montre l'évolution des -défauts
quantiques du Li
au
Cs.
Pour les orbitales pénétrantes (s,p
et
orbitales
d
des
alcalins
les
plus
lourds) ~l augmente
avec Z.
Par contre pour les orbitales f le défaut quantique
est toujours très faible.
On peut voir sur la table 1 que les valeurs de 6~~l'
déterminent bien l'apparition des minima dans les courbes de
sections
efficaces
des
alcalins.
Ceci
est
aussi
illustré
dans la figure 7(b) pour les transitions nd .... €p
et nd .... €f.
Pour les transitions nd .... €p
il existe deux zones correspon-
a
dans à 6~dp supérieur ou inférieur à 6~dp. Ces zones corres-
10'
,
,
,
,
.
.
.
,
,
,
i
'
!
!
• r
i i
«
i
i
'
1
a)
b)
d}
eJ
ln!'
und
In z ,
ln 2.
In 2+
lT
C1
C1
u
16d
20 d
- -
C1ec!,p
O"i6d.p - -
C1ZOd.p - -
S
C1
C1ZOeJ.r •• --_••
10°10-1'\\-
6 d ,f
0" I6d,r •••• -
6
8
"~,,_,,._,..._--_..--
h.J
10
Ji'
/,;.;~~~;/
!. 10"
12
b
1
!
.............
-;.....................
)
20
";,,
co
i
............... ---J'!..
/
-.0
•••....,.~.~.
lie)
0,2
1
1
-----.....__
:
\\\\ /1
:'(e)
:
1
,
1
--ÜZ~
/
\\ , '
-------
(b)
1 1
_
JVL__ (c)
1 1
---
, /
t ,
__ - . __
1
\\ 1
__
l ,
Kr ,
"
i "
i
,
,
•
..
1
.
'
, !
l
,
1 .
"
i
i
o
0.1
Qi
0.3
0.4
O~O
nI
0.2
0.3
O.L
0.5 0
0.1
Q2
0.3
0.4
0.50
0.1
O.Z
0.3
0.4
().5
E(Ryd)
t(Ryd)
e(R,Yd)
E(Ryd)
r
2
IGURE 6
Evolution avec n des sections efficaces totales et partielles le long de la série nd de In + .
a) 0nd(€)
pour n = 5,6,8,10,12 et 20.
Sections efficaces partielles et totales pour n = 8(b),
16(c) et 20(d). Dans ces trois
figures,
les types des courbes 0n~,tl(€) sont indiqués.
69
TABLE 1
Eléments
Transition
61-111'
Li
Na
K
Rb
Cs
ns -+ e;p
-0.26
-0.49
-0.47
-0.49
-0.50
-0.37
(b)
(c)
(c)
(c)
(c) 6s, 7s
np -+ e; s
0.26
0.49
0.47
0.49
0.50
0.71
(a)
(a)
(a)
(a)
(a) 6p
np -+ e;d
-0.05
-0.84
-1.44
-1.30
-1.10
-0.42
(a)
(c)
(d) n < 9
(c)
(c) 6p
(e) n :> 10
nd -+ e;p
0.05
0.84
1.44
1.30
1.10
0.75
(a)
(b) n < 3
(c)
(c)
(c) 5d, 9d
(c) n , 4
nd -+ e;f
0
-0.01
-0.26
-1.32
-2.43
-0.48
( a)
(a)
(a)
(c)
(e) 5d
(f) 9d
nf
-+ cd
0
0.01
0.26
1.32
2.43
0.78
(a)
(a)
(a)
(c)
Table 1
Pour chaque transition ni -+ e;l' et chaque élément,
comparaison
des
différences
de défauts quantiques
asymptotiques 61-1
et cri tiques 6~"
et
type
de
1 1,
forme des courbes de sections efficaces 0ni,i,(e;).
a)
4J
.
r
'1
.: c ~ (c)1mi.nimum
II
e
JJ.idp
{f
7
:l...
<1
1
/
(a)
3 1
I l
~
0 1
..(f}3minima
1
IA}'Odfl.l
~ 2~
1/
Id ~
2,
/
(e)2minima
0
r-,
1
/
.1
/
1
-c...I,j
f
I~ Illp"dfl+1
/
L
1
1 J
/ /
(c) 1minimum
l!.pOdf
o
O.
9
cr=
•
i
i "
,
Li
Na
K
Rb
Cb
Li
No
K
Rb
Cb
r IGURE 7
Oéfauts quantiques et différences de défauts quantiques asymptotiques le long
de la séquence des alcalins
a) ~t pour les orbit~les s, p, d et f.
b) 6~dp et 16~dfl. Les éléments sont repérés par des signes différents suivant
la forme de 0nt,t'«()
: 6(a~, o(b),
.(c) et + (e) ou
(f).
71
pondent
aux
types
de
courbe
(c)
et
(a)
respectivement
et
l'on
peut
voir
que
les points et triangles se placent dans
les bonnes zones. De manière analogue pour les transitions nd ~ ~f
les
triangles,
points
et
croix
se
placent
assez
bien
dans
les
zones différentes, séparées par les lignes horizontales cor-
respondant à 16'1l~fl + k (k:O,1,Z).
Un
dernier
point
à
remarquer
concerne
l'évolution
di fférente
des
caractères
non
hydrogénoldes
avec
Z suivant
la
transition
nt ~ €:t'
considérée.
Ainsi
pour
les
transi-
t ion s n s ~ e pou np ~ es t 0 u s les a l cal i nson t
u n c 0 mp 0 rte -
ment assez semblable. Par contre pour les transitions nd ~ ef
ou
nf ~ e d des
caractères
non
hydrogénoldes
nouveaux
appa-
raissent
lorsque
Z augmente.
Ceci
est
bien sûr
directement
lié à l'évolution différente des 'Ill avec Z suivant la valeur
de l
("figure 7a).
3) Evolution le long d'une séquence isoélectronigue.
Compa-
raison des séguences de K, Rb,
Cu et Ag
Là
encore
la
systématique
des
caractères
non
hydro-
génoldes et leur évolution découlent simplement de la varia-
tion avec z des défauts quantiques et de
leurs différences.
3.1.
Variation isoélectronique des défauts guantigues
et de leurs différences
La
figure
8 montre
la
variation
des
défauts
quanti-
ques asymptotiques 'Ils' Up' U et U en fonction de la charge
d
f
résiduelle z le long des séquences isoélectroniques.
La va-
riation isoélectronique des défauts quantiques dépend consi-
dérablement
de
la
valeur
de t
(Edlèn
1964).
Pour Q, petit
(s,p),
le défaut quantique 'Il
dû
principalement
à
la
péné-
nt
3.8
1
I
l
,3.5
1
1
.
2.2
1
c)
a} 1
1
b) lao
.0 1 \\.
1 "'0
3.0
~
Ag
--"
/
' "
b
1.0
q
" ' - -
R
~
2.0
-----------..-
:,'----.-.
- - - -
Cu
2.0
,,
i
---------------
K
,
-------
0..
N
".
01
,
~
-,
"
'.
10
:
t
:
•
i
i
'. "
d)
- ,
"
Ag
1
1
-----.---- __
1.0
_ - - - - - - - - R b
--- ------------
1
0.6
n1 ~-----------~----------
Cu
o
5
o
5
10
15
5
10
15
1J
'lJ
~
FIGURE 8
Variation des défauts quantiques asymptotiques ~s' ~p' U
et ~f
d
le long des séquences de K, Cu,
Rb,
et Ag.
73
tration
de
l'orbi tale
nx. dans
le
coeur
décroi t
lorsque
z
croi t
le
long d'une
séquence.
Pour 1 grand
(f)
ce sont les
effets de
polarisation du
coeur
qui
contribuent le plus au
défaut quantique~n1 ; pour ces orbitales non pénétrantes ~n1
croit
d t ab o r d
avec
z,
atteint
un
maximum et
puis
décroit.
Pour le défaut quantique des états nd, ainsi qu'en a discuté
Manson
(1969), il
dépend considérablement de l'élément étudié
en
raison
de
l'existence de
barrières de
potentiel dans le
potentiel effectif vu par
l'électron d de certains éléments
particuliers. La variation isoélectronique de \\.Id
pour
les
séquences de
K et Rb diffère de celle observée pour les sé-
quences
de
Cu et
Ag
aux
faibles
valeurs de
z ,
ainsi
qu'il
appara1t dans la figure 8.
A l'exception de ces faibles
va-
leurs,
la décroissance monotone
avec
z résulte de
la péné-
tration de l'orbitale nd dans le coeur.
La
figure
9
montre
la
variation
des différences
des
défauts quantiques
asymptotiques 6\\.1
,
en
fonction
de
z
le
11
long des séquences. Les trois séries de courbes \\.Is'
\\.Ip' \\.Id
(z
~ 3) sont très semblables (figure 8), et les écarts entre
les courbes d'une série donnée sont voisins des écarts entre
les courbes d'une autre série. Ainsi 6\\.1
et
à
un
degré
sp
moindre 6\\.1dp
dépendent
peu
de
la
séquence.
Il
est
à
noter
que
les
courbes
correspondant
aux
séquences
Rb,
Cu et
Ag
sont pratiquement confondues.
Il
n'en est plus de même pour
6\\.1df et 6\\.1fg qui dépendent de chaque séquence, en raison des
variations très différentes de \\.Id et \\.If avec
z.
Les
valeurs
de 6\\.1~t, déterminent bien comme pour les alcalins l'appari-
tion des minima dans les courbes des sections efficaces des
séquences isoélectroniques de K, Rb,
Cu et Ag.
Ceci est il-
lustré
sur
les
figures
9(a)
et
9(b)
pour
les
transitions
nd ~ E'P et nd ~ E'f. Les éléments dont a~d,V(E') est du ty-
(c) sont repérés par des points et ceux pour lesquels a~d,f(E')
est de type (e) par des croix ; les points et croix se trou-
vent
dans
les
bonnes
zones
séparées
par
les
valeurs
de
16 \\.1 ~ 1 ,1 + k .
1.6
1
•
•
i
•
,
a)
ne
.
1
•
\\
i
i
shape(c)
c)
1.0
•
t
1
0.5.
Q..~'~
1J. 0
\\'
-0
Rb?..................
Cu,Ag
JI dp
h
"
:l-..
,/
s ape,Q
0-
~
A
.q
~...-
Cu,Rb, 9
......' ...
/
<3
K~-......--...---..----------
.........
a,
........"-..-
o.
<1
Z.O ;=:;====:::1:====---:!
-,!_ _..J"'U,
......-..-....--;7--....------
b)
o,
,
,
i
,
l.âuO 1 sha~(e
o
5
10
15
r df +1 .
.
11
-:t
r-,
1.0
•
,
•
j
•
d)
shape(c
1.0
1»
....
AS
---
JApOdf'
CIo
»<;
"
'
.......
~.q--
/
H ~
(
1
,
-_.._
-
shap«; a.
- 0 1 ~-------_.
1
~
i
,
i
1 '
.._-..-..-.._-------
O
5
10
15
o,
y
,
,
i
,
~
o
.5
10
15
~
FIGURE 9
Variation des différences de défauts quantiques asymptotiques ~Ull' en fonction de z.
Dans les figures
(a) et
(b)
les éléments pour lesquels a~d,~(€I) est de type (c) sont
repérés par des
., ceux pour lesquels a'd 9.~€') est de type (e) par des +.
n
,_
75
3.2. Systématique de la photoionisation
Nous
allons
maintenant
illustrer
la
systématique
de
la photoionisation des états excités ns, nd et nf.
3.2.1. Etats ns
La figure
10 montre la variation avec n des sections
efficaces au seuil a'
(0)
le long des quatre séquences. Com-
ns
me pour z donné la différence de défauts quantiques asympto-
tique ~~
est quasiment indépendante de la séquence (figure
sp
9c),. les quatre séries de courbes sont très similaires.
Les
valeurs
obtenues
pour
la
séquence
du
K s'écartent
le
plus
des valeurs obtenues dans les autres séquences ; il en était
de même dans la figure 9c. En particulier la série a'
(0)
de
ns
Ca+ ne
présente
pas
de
minimum,
puisque toutes les courbes
correspondantes a'
(E')
sont
de
même
type
(b).
Les
valeurs
ns
a'
(0)
des
atomes
neutres
(formes de
type
(c))
et des
pre-
ns
miers ions des séquences (types (b l ,
(c ) )
diffèrent de cel-
les de
l'hydrogène,
en
raison d'importants effets d'annula-
tion dans les éléments de matrice de transition R
(E').
ns,p
Les minima très accusés de Zn+, s-" et Cd+
proviennent
du
changement de forme de (b ) à Cc ) de a'
(0)
le
long
de
leur.
ns
série
ns
respective.
Pour
les
ions
suffisamment
chargés
(z ~ 3), les valeurs des sections efficaces tendent réguliè-
rement et progressivement vers les valeurs de l'hydrogène le
long des séquences.
3.2.2. Etats nd
La figure
11 montre la variation avec n des sections
efficaces au seuil a~d(O) le long des quatre séquences. Elle
indique clairement de grandes différences entre les séquen-
ces, ~~df dépendant particulièrement de
la séquence
(figure
9b).
Les minima
très accusés qui apparaissent ont pour ori-
gine le changement de forme de a~d,f(E')
de
(b)
à
( c )
pour
a
lO l
'
, --,--'
,
1
__
_L-'----1....--1--.
1
1
'
0) K-like
d) Ag-like
lOt
:Ai 1O'.f"/
»>:
~ ______
L.
10
E
....
s,~b '00r7
19-.,g
~
... c
b
IO-'f
~ 10-'
\\0
,....
10-1, •
•
,
•
,
4
6
1
10
'2
II,
16
" 20
n
10-3
t.
6
8
ta
12
tI.
16
18 20
4
6
8
ta
12
II.
16
18 20
4
6
8
10
12
II.
16
18 20
n
n
n
fIGURE
10
Variation avec n des sections efficaces au seuil a'
(0)
pour
ns
les séquences de K(a),
Cu(b),
Rb(c)
et
Ag(d).
.
lOI, . ,
,
lOS
,
ft
,
0
,
,
,
!
!
1
o.) K-Iike
c) Rb.like
d) Ag-like
~
4
Sb + Ag
Krl~
Rb Tc:6 +
1
F.7• _
:.-----::::
101
~r+
:i
~
J:
1:
x.17+
....
1
'0 10
-ôlO
A 10+
...."0
.c
-"'0
RhS + . 9
,c
b
MaS +
b
10°
•
-..J
-..J
4
6
8
\\0
t2
t4
.6
18 20
4
6
8
10
12
14
16
t8
20
4
6
8
10
12
t4
16 t8
20
-1
- - 4
n
n
n
10
1
i
;
i
,
1
6
10
14
III
zz
n
fIGURE 11
Variation avec n des sections efficaces au seuil a~d(O) pour
les séquences de K(a), Cu(b),
Rb(c) et Ag(d).
78
2+
Ca+, Br 6+ et Rh 8+ ou de (d) à (e ) pour In
Les
minima
sont
très marqués pour Ca+ et In 2+
car
pour
ces
ions
simultané-
ment cr'd
(e:')
change
aussi
de
(b )
à
(c ) le
Lon q de
la sé-
n ,p
quence. La présence de minima dans cr~d,f(e:') (voir figure 9)
explique aussi que les valeurs cr~d(O)
pour
beaucoup
d'ions
soient
très
di fférentes
de
celles
de
l' hydrogène.
Les
con-
tributions relatives de cr'd
(e:') et cr'd f(e:')
dans cr'd(e:')
n ,p
n ,
n
dépendent considérablement de n et de chaque élément étudié,
et bien souvent on a cr'd f(e:')
< cr'd
(e:').
Il
en
résulte
n
,
n
,p
que l'évolution des valeurs de cr~d(e:')
vers
celles
de
l'hy-
drogène n'est régulière le long d'aucune des séquences.
3.2.3. Etats nf
Dans
les
séquences
isoélectroniques
de
K,
Cu et
Rb
les sections efficaces cr~f(e:') ne
sont
pas très différentes
de
celles de
l'hydrogène,
en
relation avec la
faible
valeur
relative de' 6lJ.
(voir
figure
9d).
Nous
ne discuterons donc
f g
que le cas de
la séquence de
Ag.
La figure 12 présente l'é-
volution avec n des sections efficaces au
seuil
cr~f(O)
le
long de la séquence de Ag.
Les valeurs de cr~f(e:')
dépendent
principalement de celles de cr~f,g(e:'). Les valeurs de cr~f(O)
de
Ag sont les mêmes que celles de
l'hydrogène et diffèrent
5+
7+
considérablement de celles des ions les plus chargés Te
-Xe
.
De
fait
les
minima
très
accusés
qui
apparaissent
provien-
nent du changement de
forme de cr'f
(e:')
de
(b )
à
(c )
le
n
,g
long
de
la série
nf.
Ce changement de
forme
intervient
pour
5+
7+
(
)
..
( )
Te
-Xe
alors que cr' f
e:'
est
de
forme
hydrogénoide
a
3
n
,g
pour Ag-Sn +, en relation avec les valeurs relatives de AlJ. f g
(voir figure 9d). Là encore le minimum le plus accusé obser-
6+
vé pour I
est dû au
fait que les valeurs de cr
et
1 2 f,g(O)
cr 12 f,d(O) sont simultanément très faibles. Ainsi les carac-
tères non hydrogénoldes n'apparaissent que pour les ions les
plu s cha r g s et l' évolut ion
de cr ~ f ( e: ') ver s des val e urs h y d r
é
0 -
génoldes est
très irrégulière le long de
la séquence de
Ag.
79
6
8
10
12
14
16
18
20
n.
FIGURE 12
Variation avec n des sections efficaces au seuil
cr~f(O) pour la séquence de Ag.
80
3.3. Discussion
Les paragraphes précédents montrent clairement que la
théorie
du
défaut
quantique
et
les
formules
(11.8,9)
sont
bien
adaptées
à
l'analyse
de
la
systématique
de
la
photo-
ionisation des états excités des systèmes à un électron.
Un
résultat
intéressant concerne la quasi invariance de
la va-
riation
isoélectronique
de
la
photoionisation
à
partir
des
états ns le long des quatre séquences étudiées.
Il en est de
même
pour
la
photoionisation
à
partir
des
états
np
(voir
annexe
IV).
Par contre
le comportement isoélectronique pour
la photo ionisation à partir des états nd et nf dépend beau-
coup de la séquence étudiée.
Un autre point à souligner con-
cerne
le
comportement
isoélectronique
particulier
obtenu
pour
la
photoionisation
à
partir
des
états
nf dans
la
sé-
quence
de
Ag.
Les
caractères
non
hydr.ogénoldes
sont
plus
marqués pour les ions relativement chargés que pour les pre-
miers ions de la séquence.
En résumé, des caractères non hydrogénaI des très mar-
qués
et
très
divers
ont
été mis
en
évidence
dans
les
sec-
tions
efficaces
partielles
et
totales
de
photoionisation
à
partir des états fondamentaux et excités nt (n ~ 20, t
< 3),
dans les séquences isoélectroniques de K, Rb,
Cu et Ag.
Ces
caractères sont
très
étroitement
liés aux valeurs relative-
ment importantes des défauts quantiques des états nt concer-
nés.
Des évolutions régulières et irrégulières de ces carac-
tères non
hydrogénoldes
le long des séries de
Rydberg ns-nf
et
le
long
des
séquences
étudiées
ont été observées.
Enfin
le
comportement
similaire
ou
différent
de
ces
séquences
a
été noté.
81
IV. DISCUSSION CRITIQUE DES RESULTATS OBTENUS
La validité des résultats obtenus concernant les sec-
tions efficaces de photoionisation a été analysée d'une part
en étudiant la sensibilité au choix du potentiel utilisé,
et
d'autre part en comparant nos résultats à ceux obtenus anté-
rieurement. Par ailleurs notre modèle d'analyse de la systé-
matique des caract~res non hydrogénoldes est comparé à celui
de l'équipe de
Manson.
Les
sections
efficaces
de
photoionisation
des
états
n~
des
premiers
éléments
des
séquences de
K et
Rb
ont
été
calculées en utilisant trois différents modèles de potentiel
central (a),
(b ) et (c) décrits dans la section I. Rappelons
que seul le modèle (b) prend en compte les effets de polari-
sation de coeur. De la comparaison des résultats ainsi obte-
nus on peut tirer plusieurs conclusions.
a) Pour
tous
les
états
où
des
effets
d'annulation
dans
les
éléments de matrice de
transition conduisent à des
minima dans les courbes de photoionisation, les sections ef-
ficaces
sont très faibles
par rapport à celles de
H et donc
sensibles au
choix du potentiel.
Par contre en
l'absence de
tels effets d'annulation,
les résultats obtenus avec diffé-
rents
potentiels
sont
très
voisins.
Ce point
est
illustré
dans l'annexe 1 sur l'exemple particulier des sections effi-
caces de photoionisation de Rb et Sr+. Quelques comparaisons
typiques sont aussi données dans la colonne
(3)
de
la table
2 correspondant aux états excités de Rb.
Il est très net que
les
différences
les
plus
grandes
entre
les
résultats
(a),
(b )
et
(c)
apparaissent
pour
le
niveau
6s
dont
la
section
efficace cr
est très
petite
6 s(O)
à
cause de
la présence d'un
minimum de
Cooper près du seuil.
82
TABLE 2
Autres résultats
Nos
Résultats
Etat
Energie
théoriques
résultats
expérimentaux
Moskvin C1963)
5p
e: = 0
.14.0 ta)
~ 14
13.0 (b)
12.5 Cc)
{e: = 0.016
l13.0 (al
11 .5
9.6tO.2 CKlyucharev
À = 0.44 Ilm
12.2 (b)
and Sepman 1975)
11.9 Cc)
6p
{e: = 0.04
rO.7
-1
(al
6P1/2 15±4 CAmbartzu
\\) = 14404 cm
9.7 (b )
mien et al. 1976)
9.9 Cc)
6P3/2 17±4
"
{e: = 0.17
-1
l3.3 (al
6P3/2 1• 9±0.5
"
\\) = 28806 cm
3.3 Cb)
3.2' Cc)
4d
e: = 0
~35.7 (al
= 40
34.0 (b )
33.3 (c)
6s
e: = 0
11.0 (al
~
1
0.77 (b )
0.85 CC)
Table 2
Comparaison des résultats obtenus pour Rb à l'aide
des trois modèles de
potentiels a),
b) et c)
avec
des
résultats
théoriques
et
e xp ri me n t au x
anté-
é
rieurs.
83
b ) Les
différences
entre
les
résultats
provenant
de
l'introduction
des
effets
de
polarisation de
coeur
(compa-
raison des résultats
(a) et
(b))
sont souvent du même ordre
de
grandeur que les différences entre les résultats obtenus
avec
les
potentiels
(a)
et
(c ) qui négligent tous deux
les
effets de
polarisation du
coeur.
Ainsi
la validité des ré-
sultats dépend beaucoup de la qualité du potentiel représen-
tant les effets du coeur et non pas uniquement des effets de
polarisation de coeur.
c ) Les
effets
de
polarisation
de
coeur
augmentent
avec
la
charge
Z de
l'élément
considéré
et
sont
beaucoup
plus importants dans les premiers éléments de la séquence de
Rb que dans ceux de la séquence de K. Le rOle de ces effets
diminue le long d'une série de Rydberg n~ donnée, confirmant
les
résultats
obtenus
antérieurement
par
Aymar
(1978).
De
plus les travaux de Shevelko (1974) ont aussi montré que ces
effets
diminuent
le
long
des
séquences
isoélectroniques.
Le
meilleur
test
de
validité
de
nos
résultats
est
fourni
par la comparaison de ceux-ci aux données expérimen-
tales.
Malheureusement
celles-ci
sont
très
peu
nombreuses,
concernant essentiellement les niveaux
fondamentaux
4s de
K
(Marr and Creek 1968, Sandner et al.
1981) et 5s de Rb (Harr
and
Creek
1968)
et
les
niveaux
5p
et
6p
de
Rb
(Klyucharev
and
Sepman 1975,
Allbartzumian et al.
1976)
encore faut-il
noter
que
pour
ces
états
excités
les
sections
efficaces
n'ont été mesurées que pour quelques longueurs d'onde préci-
ses. Les courbes de sections efficaces des niveaux fondamen-
taux des alcalins présentant un minimum de Cooper sont par-
ticulièrement sensibles au
détail
des
fonctions d'onde.
Les
calculs réalisés avec le potentiel (b)
reproduisent bien les
données expérimentales de Rb
; l'accord est un peu moins sa-
tisfaisant
pour K mais il
faut noter que les effets d'annu-
lation apparaissant dans les éléments de matrice sont parti-
culièrement grands dans ce cas.
Aucune conclusion concernant
84
la validité de l'ensemble des résultats ne peut être déduite
de
la seule comparaison portant sur les états fondamentaux,
dont les sections efficaces sont particulièrement sensibles.
En ce qui concerne les niveaux excités de Rb la table 2 mon-
tre
que
l'accord
théorie
expérience
est
moyen mais non si-
gnificatif vu le peu de données expérimentales.
3
De manière pratique, pour les
éléments
K_Ti +
dont
les
polarisabilités
statiques
dipolaires
sont
faibles
nos
calculs ont été réalisés en utilisant le potentiel (a)
ces
résultats
sont
quasiment
identiques
à
ceux
obtenus
par
Aymar
et al.
(1976)
avec le potentiel
(c).
En raison du bon
accord avec les résultats expérimentaux obtenus avec le po-
tentiel
(b )
pour
Rb
5s,
ce
potentiel
est
utilisé
pour
les
premiers éléments des séquences de Rb, Cu et Ag dont les po-
larisabilités
dipolaires
statiques sont
importantes
(Chich-
kov and
Shevelko 1981).
Pour les ions plus chargés dont les
spectres d'énergies sont peu ou pas connus nous utilisons le
potentiel ab initio décrit dans la section I.
Chaque fois que cela a été possible nos résultats ont
été
comparés
aux
résultats
théoriques
obtenus
par d'autres
auteurs. Quelques résultats typiques sont donnés dans la ta-
ble 2 pour Rb et dans
la
table
3 pour certains éléments de
la
séquence
de
K.
Un
accord
satisfaisant
est
obtenu,
les
états
concernés
ayant
des
sections efficaces
peu
sensibles
au modèle choisi. D'autres comparaisons réalisées pour des
t a t s ns e t
é
nd de Cu et Ag dont les sections efficaces présentent un ou
plusieurs minima montrent que nos résultats diffèrent un peu
plus de ceux calculés par d'autres auteurs (voir annexe IV);
cependant
les
formes
des
courbes
de
section efficace
(type
(c ) ou
Ce ) ) prédites sont
les
mêmes,
le désaccord
interve-
nant
au
niveau
de
la position exacte des extrema.
Des
don-
nées expérimentales et théoriques additionnelles sont néces-
saires pour mieux juger de
la validité de l'ensemble de
nos
résultats.
TABLE 3
Nos
Moskvin
Hsezane (1984)a
Mc Ginn
Black et al.
ReilIRan and
Elément
Etat
résultats
(1963)
H5
l
V
(1970)
(1972)
Manson (1978)
K
5s
0.33
0.52
4p
4.72
4.80
3d
27.14
35.00
31 .35
24.83
24.76
Ca+
4s
0.198
0.171
0.209
Fe 7+
3d
0.698
0.766
(Xl
Vl
a H5, Hartree-51ater
l,
longueur
V,
vitesse.
Table 3
Comparaison des
sections efficaces
au
seuil
obte-
nues
pour
quelques
éléments
de
la
séquence
de
K
avec des résultats théoriques antérieurs.
J
86
L'analyse de la sensibilité de nos résultats au choix
du
potentiel
et
les
comparaisons
aux
résultats
antérieurs
montrent
clairement
que
notre
modèle
reproduit
de
manière
satisfaisante les caractéristiques de la photoionisation des
états
excités.
Ce modèle est donc tout
à
fait
adapté à des
études intensives de
systématique.
Nos
résultats concernant
ces
études
de
systématique
sont
à
comparer
à
ceux
obtenus
par l'équipe de Manson
(Msezane and Manson 1982,
lahiri and
Manson 1982, 1986, Manson 1985). Les travaux de cette équipe,
menés
parallèlement
aux
nôtres
à
l'aide
du
potentiel
Har-
tree
Slater, ont
porté
sur
la
photoionisation
de
quelques
états
excités
des
alcalins
et
sur
la
photoionisation
des
états
fondamentaux
de
tous
les éléments du tableau périodi-
que,
ces derniers
travaux ayant pour but d'analyser la sys-
tématique des minima apparaissant
dans les sections effica-
ces
partielles
correspondant
aux
diverses
sous-couches.
Lorsqu'une
comparaison
avec
nos
résultats
est
possible,
l'accord est en général satisfaisant. L'interprétation qu'ils
donnent
de
l'existence
des
minima
et
de
l'évolution
de
la
position
de
ceux-ci
avec
Z est
aussi
similaire
à
la
nôtre
puisque basée sur la différence entre le déphasage des fonc-
tions
du
continuum
et
le
défaut
quantique
des
états
liés.
Une
di fférence
notable
par
rapport
à
notre
étude
concerne
les
valeurs
critiques
correspondant
à
l'apparition
des
zé-
ras: ils utilisent la valeur b,1Jo
= 0.5 quelle que soit la
transition n~ ~ E~' considérée, valeur beaucoup moins préci-
se que nos valeurs b,1J~~,. En particulier leur modèle ne per-
met
pas d'expliquer
la différence de
forme observée parfois
pour
les
sections
efficaces
correspondant
aux
transitions
n~ ~ e:(~+1)
et
n(~+1) ~ E~.
Une
illustration
de
ce
point
peut
être
trouvée
dans
la table
1 à
propos des
transitions
ns ~ cp (type (c)) et np ~ ES (type (a)) de Cs.
87
V. CALCULS RELATIVISTES
Les
résultats
précédents
ont
été
obtenus
à
l'aide
d'un modèle à champ central non relativiste.
Les effets re-
lativistes
peuvent
être
importants
pour
la
photoionisation
d'éléments
de
charge
nucléaire
Z relativement
élevée,
même
aux
basses énergies.
Nous
avons
évalué
ces effets pour
les
ions
multichargés
moyennement
lourds
à
l'aide
d'un
modèle
relativiste à champ central,
et comparé les calculs relati-
vistes aux résultats non relativistes.
1) Modèle relativiste à champ central
C'est
une
généralisation
du
modèle
non
relativiste
introduit
dans
la
section I.A.II.2.1
et
le
traitement
est
analogue. Les fonctions d'onde relativistes
approchées
I~.>
(z-1)+
l
et
~f> du Hamiltonien relativiste du
système X
sont
1
des déterminants de
Slater
(ou des combinaisons de détermi-
nants de Slater) solutions propres
du
Hamiltonien approché
N
2
H
+
=
ca .. p . +
ev(r
(II.10)
D
L (~ ~
S.mc
l
l
l
i))
i =1
Les
déterminants
de
Slater
sont
construits
à
partir
des
N
fonctions
d'onde ~ solutions
propres
du
Hamiltonien mono-
électronique qui s'exprime en unités
atomiques
(énergies et
potentiel en Rydbergs)
:
(II.11a)
~ ~
2
= 2(ca.p + 8c ) + V(r)
(II.11b)
~
où
p est l'impulsion de
l'électron,
c = 1/a l'inverse de la
constante de structure fine. ü et 8, opérateurs agissant sur
le spin,sont
dans la représentation de Dirac
des matrices
d ' 0 rd r e
4 qui
s' exp r i men t
à
l' ai d e
de
mat r i c es d' 0 r d r e
2
88
les matrices de Pauli et la matrice unité.
La solution
I~)
correspondant
à
l'énergie E se présente sous la forme d'une
matrice
à
une
colonne
et
quatre
lignes que
l'on
peut
noter
1]
~
~
où ~1 et ~2 sont des matrices à une
1
(:2
"' )
--
colonne et deux lignes.
L'énergie
totale
E comprend
l'énergie
associée
à
la
2
masse de l'électron E = 2c
+ e:
; e: est
négati f
pour
les
états du spectre discret et positif pour ceux du continuum.
Dans le cas d'un potentiel central, h
commute
avec
D
les opérateurs 12 , j
et parité associés aux valeurs propres
z
j,
m et '11'.
j
est
le moment
angulaire
total
.r = ! + ~), m
le moment angulaire magnétique et la parité
'11'=
(-1)~. L'état
pro pre cor r e s p0 n dan tau x. val eu r sE,
j, met '11' s' é cri t
G( r) / r
IS~jm>]
1 ~)
=
(II.12)
( iF(r)/r IsIjm>
où l
= 2j - ~ et Istjm> est un spineur à deux composantes.
Les fonctions radiales G(r) et F(r) sont solutions du systè-
me
d'équations
différentielles
couplées
du
premier
ordre
ldG +XG- {2C + e: -2~(r)}F 0
crr
=
r
(II.13)
dF _ X F
e: - V(r) G
0
crr
+
2c
=
r
avec X
(_~)t+j+1/2(j+1/2).
=
Les
orbitales
discrètes
(e: < 0)
sont
normalisées
à
co
2
2)dr
l'unité par J (G
+ F
= 1 et celles du continuum par
o
unité d'énergie en Rydbergs
fCO(GG'
+ FF')dr = 'ITô(e:-e:').
o
89
2
Notons que dans la limite non relativiste (E «
c
et
2
IV(r)1
« c ) le système peut être
développé
suivant
les
2
puissances de
.
()
On obtient à l'ordre le plus bas
G
.. P
n t j
n t
(11.14)
Fn t j .. ~ lddr + fJPnt·
2)
Sections efficaces
Nous
nous limitons au cas des systèmes à un électron
de
valence
où
un
seul
électron
actif
passe
d'une
orbitale
liée à une orbitale libre.
L'expression de la section effi-
cace de photoionisation est obtenue de façon analogue au cas
non relativiste (section LA.Il.1.2). On considère dans la jau-
ge
de
Coulomb
et
à
l'approximation
dipolaire
l'élément
de
matrice du Hamiltonien d'interaction qui se réduit à
(41
n , . ,
,lâ.€I~ n' ). En effectuant les calculs on obtient:
E~
J m
n~Jm
cr
(
-15)
1
1
\\'
n .
=
n~J
64.29x10
(E-E.) 2j+1
L
L
ntJ
2,'=2,:t1
jf=2,':t!
x
1(e2, , j'II () (1 ) Il nt j )12 (cllf )
(11.15)
et les règles de sélection
1 j-11
< j'
< j+1.
En
remplaçant
l'élément de matrice réduit
(E2,lj~II()(1)llntj) par sa valeur
(Grant 1970) il vient:
=
(11.16)
On a pour le sous-niveau de structure fine j = j+ = 2, + t
2
A. = ~< F'l G >
+ . ( . \\
) { ( J' +1) <Fil G > + J' <G'
1 F >}2
J
J
-+
+
J
J+
+-
+
+-
+
+ 2,j+3<G'
IF >2
(11.17)
J+1
++
+
et pour le sous-niveau de structure fine j = j
1
= 2, - -Z
90
A. :: 2 ~ - 1<G'
1 F
>2 +
'( 1, 1) rj <F' 1 G > + (j +1) <G_' + 1 F_ >}2
J
J
--
-
J J+
l
-+
-
+ 2)+3<F'
IG >2
(I1.18)
J+1
+-
-
o
En
utilisant
les limites
non
relativistes
des
fonc-
tions
F et
G (équation
(11.14)
on
peut
obtenir
les
limites
des A.
(équations II.17,
II.18)
J
Aj -+ 2~~1(~R: + (~+1)R:) pour tout j où
R~ = I{{ll Pn~(r) (2~;~~1 ~ ddrJp€:,~~1(r)dr}
o
La
limite non relativiste de 0 n'
(équation
11.16)
redonne
no'l"J
alors
l'expression
dans
la
formulation
vitesse
du
dipôle
o~~(€:) pouvant être obtenue dans l'approximation non relati-
viste à partir des équations
(1.21)
et
(1.23),
de
façon ana-
logue à 0n~(d.
Dans
l'approximation
du
modèle
à
potentiel
central
à
un
électron
les
deux
relations
(1.22)
et
(1.23)
donnent des résultats identiques à condition d'utiliser pour
hv la valeur théorique hv = €:
-
€:n~ (équation 1.28).
3) Méthode de calculs et
résultats
Pour
faire
une
comparaison
entre
les calculs non
re-
lativistes et
relativistes nous introduisons une moyenne sur
les sections efficaces 0 n'
(équations
I1.16
et
I1.17)
et
no'l"J+
on ~j _ (é qua t ion sIL . 1 6 e t
1 l . 1 8 )
(2j +1)0
M
n'
+ (2j +1)0 n'
oy _
+
no'l,,~+
-
no'l"J-
o
-
(2j +1
+ (2j +1)
+
-
Plus explicitement on
a
91
(R.+1)a
n ·
(d + R.a n.
(e:-6I)
nJt.J+
nJt.J-
(11.19)
Les seuils d'ionisation correspondant à la photoioni-
sation à partir des niveaux nR.j
et nR.j
diffèrent:
+
-
61 = e: n.
-
e: n0.
Dans
l'équation
(11.19), e:(e:-6I)
est
nll.J+
nJt.J-
l'énergie cinétique du
photoélectron
lors de
l'ionisation à
partir du niveau nR.j (nR.j
).
+
-
Pour
effectuer
les
calculs
relativistes
nous
avons
utilisé
le potentiel
paramétrique
relativiste de
luc-Koenig
(1972) qui est une extension du potentiel d)
(section 1)
in-
troduit
par
Klapisch
(1971)
dans
le
cas
non
relativiste.
Nous nous sommes servis du programme de calculs de Mme E.luc
du
Laboratoire Aimé Cotton pour la résolution des équations
(1 1.13)
et
l' intégrat ion
des
intégrales
radiales
des
équa-
tions (11.17) et (11.18).
Nous avons calculé les sections efficaces a~R.(e:)
(équation
II.19)
à
partir
des
états
fondamentaux
et
peu
7+,
3+,
2 3+,
1 3+,
excités nR. (n ~ 6, R. ~ 2) de Xe1 7+, Xe
Sn
Mo
Mo
5+
3+.
Mo
et Zr
Les résultats au voisinage des seuils sont re-
marquablement
peu différents de ceux des sections efficaces
non relativistes anR.(e:) correspondantes. Les écarts les plus
importants
ne
dépassent
pas
20
% et concernent surtout
les
orbitales pénétrantes s
et à un degré moindre les orbitales
7+
3+
5+
3 + , .
p. Même pour les états nd de Xe
,Sn
,Mo
et Zr
ou 11
apparaît des minima de Cooper (voir Annexe IV)
les différen-
ces ne sont pas notables.
Les écarts entre les positions des
minima dans
les cas non relativiste et relativiste sont re-
lativement
faibles.
Pour
les
ions
multichargés
que
nous
avons étudiés dans le domaine d'énergie considéré les effets
relativistes ont peu d'importance. Le traitement non relati-
vis te
est donc val a b le.
92
B. RECOMBINAISON RADIATIVE DANS LES SEQUENCES ISOELECTRONI-
QUES DU POTASSIUM,
DU RUBIDIUM, DU CUIVRE ET DE L'ARGENT
Nous
présentons dans
la partie B les résultats de
la
recombinaison
radiative
dans
les séquences
isoélectroniques
des alcalins K et Rb,
et dans celles de leurs éléments homo-
logues
Cu et
Ag.
Les
sections
efficaces de
capture
et
les
coefficients
de
recombinaison
radiative
ont
été
calculés
dans
le cadre du modèle théorique décrit dans la section
I.
Les caractères non hydrogénoIdes des coefficients de
recom-
binaison radiative sont présentés dans la section II.
1.
MODELE
THEORIQUE
UTILISE
POUR
LE
CALCUL
DES
SEC-
TIONS EFFICACES DE CAPTURE ET
DES COEFFICIENTS DE
RECOMBINAISON RADIATIVE
Le modèle
théorique
que
nous
avons
utilisé
dans
nos
calculs
est
basé sur
le
principe
de
microréversibilité des
processus
physiques
direct
et
inverse.
La section
efficace
de capture cr~t(Ë) et le coefficient de recombinaison radia-
tive ~nt(T) sur l'état nt d'un système recombiné à un élec-
tron de
valence sont obtenus à partir de la section efficace
de photoionisation cr~t(Ë) à l'aide respectivement des rela-
tions (I.58) et (I.61).
La section efficace cr~t(E) est aupa-
ravant
calculée en
utilisant le modèle théorique et les mé-
thodes numériques décrites dans
la section ILA.1. A partir des
valeurs de cr~t(E), le coefficient ~nt(T) est obtenu par les
méthodes
standards
d'intégrations
numériques
en
calculant
une
intégrale
portant
sur
l'énergie E des
photoélectrons
(équation
I.61)
dont
l'intégrant
décroît
rapidement
lorsque
E croit
des
intervalles
d'intégration
croissants
et
suc-
cessifs sont utilisés jusqu'à ce que la contribution du der-
nier
intervalle devienne négligeable.
La zone d'énergie ef-
fective correspondante croît avec la température T.
93
Les coefficients de
recombinaison radiative an(T) sur
la couche n et total
a (T) sont dédui ts de a
(T)
à
partir
t
n t
respectivement
des
relations
(1.56)
et
(l.57).
Nous
avons
combiné notre modèle avec
le modèle hydrogénoïde
(voir sec-
tion
1.B.I1.1)en considérant
ant(T)::: a~t(T) quel que soit
n si t
> 3 et an(T) ::: a~(T) si n > n
où n
dépend de
l'élé-
L
L
ment considéré (voir Annexe III).
II. RESUL TATS
Les
coefficients
de
recombinaison
radiative
ont
été
4+,
8+
calculés pour les ions qui se recombinent K+_Ti
Fe
et
Mo 24+,
Rb+_y3+, Cu+-Ga 3+ et Ag+_Sn 4+.
Le comportement hydro-
génoide
de
ces
coefficients
a
été
rappelé
dans
la
section
LB.I1.1. La comparaison des coefficients le long des séquen-
ces
isoélectroniques et avec
la séquence de
l'hydrogène est
faite
en
introduisant les variables
réduites de
température
T'
= T/z 2
et
du
coefficient
de
recombinaison
radiative
a'(T') =a(z2 Tl)/z.
Les
sections
efficaces
de
photoionisa-
tion
à
partir
desquelles
les
coefficients de
recombinaison
sont
calculés sont
relatives
à
la
seule
photoionisation
de
l'électron de
valence
(voir section A.III).
Le calcul de ces
sections
efficaces
est
valable
au
voisinage
des
seuils
et
les
effets .d'autoionisation
sont
négligés.
Dans ces
condi-
tions
les calculs des coefficients de
recombinaison ne con-
cernent qu'une zone réduite choisie de température
500 < T < 10
000
K pour les éléments de la
séquence
de
K et
500 < T'
< 5 000 K pour tous les autres éléments. La zone d'éner-
gie
effective
correspondante
des
pho t.o Lec t r o ns
est
celle
é
pour
laquelle les caractères non hydrogénaI des des sections
efficaces
de
photoionisation
sont
les
plus
marqués.
Cette
zone est d'autant plus réduite que la température est faible.
Les détails de
tous
les résultats concernant la sys-
tématique des caractères non hydrogénoides de la recombinai-
94
son
radiative dans
les séquences isoélectroniques de
K,
Rb,
Cu et Ag se trouvent dans les annexes II,
III et IV. Ces ca-
ractères
non
hydrogénoldes
sont
particulièr~ment marqués
pour les coefficients de recombinaison radiative a~t(T').
Nous en illustrons quelques uns parmi les plus remarquables.
1)
Variation de a~t(T~
en
fonction
de
n, t
et T'étant
fixés
Les figures 13(b), 14(b) et 15(b) présentent l'évolu-
tion
avec
n
des
coefficients
de
recombinaison
radiative
a'
(T')
(t
~ 2) calculés pour une température T' = 500 K re-
nt
lativement faible.
La figure 13(b) correspond aux a'
de di-
ns
vers
éléments
de
la
séquence
de
K,
les
figures
14(b)
et
15(b), respectivement aux a'
et a'
d'éléments
de
la
sé-
np
nd
quence de Ag. Ces valeurs
a~Q,
sont
comparées
aux
coeffi-
H
cients a n de H. La plupart des coefficients a'n ont la même
n~
.
H
n~
décroissance monotone avec n que l~s a
correspondants. Cer-
nt
tains autres coefficients présentent des minima et des maxi-
ma et d'autres caractères non hydrogénoldes spécifiques que
nous allons souligner.
A une température
faible
la zone effective d'énergie
des photoélectrons pour le calcul des coefficients a~t et an~
est ressérée près du
seuil. L'évolution avec n de ces coef-
ficients est étroitement liée à celle des sections efficaces
H
au seuil a~t(O) et ant(O).
Le'S
courbes
donnant
l'évolution
des a~t(O) avec n sont données par les figures 13(a), 14(a)
et 15(8).
Les principaux caractères non hydrogénoldes apparais-
sant dans l'évolution avec n des a~t(T') sont les suivants:
H
a)
a'
< a
nQ,
nt
Il apparait dans la figure 13(b) que a'
«aH
pour
ns
ns
K et Ca+.
Le comportement
non hydrogénolde des sections ef-
3
,
10
l
,_ _L'--:--l...!_--LI
10-1!
t :-:-'---1'_.1.---'-
t~'_L-'-------.-' , , , , 1
a)
b)
Z
10-14
10
1
::0 10
c- 10-15
1:
1
-
Il)
-
cf)
0
E
-
0
li)
'-'
c:
1. .
1/)
b
~ c:
10°
10-16~
~
\\.
~
~
\\0
\\JI
10- 1
10-11
10-18 ,
i
10- 2
1
- - . , - -
1
4
1
i
J
l '
4-~1r-~1r--"'---
1
1
1
1
1
1
8
Il
16
lO
6
8
10
12
14
16
18
2.0
n
n
fIGURE 13
Variat·ion avec n des coefficients de recombinaison radiative a'
(1'=500 K)
ns
le long de la séquence de K(b)
reliée à la variation avec n des sections
efficaces au seuil a'
(O)(a).
ns
10- 12
,
i
'
!
!
!
!
toi
,
,
,
,
,
,
1
i
b) Ag- like
I~'~'-'-----l..------L--I-L--
o.) Ag-like
Ag
10-13
'""
/
Cd+
.
-!q
-'
2+
toi
If)e
In
.sCL
':4
.. C
1:
-
~
"ô
10-14
""'0.
.. 1:
~,
8+
• 4+
" , >r
8"
ab
Q
,
Xe
b
7+
'"
0\\
'0
10-15
,
4
6
'0
'2
'4
'6
,. 20
•
10-16 ,
n
- - -· -
·
,
r
•
i
i
1
4
6
8
10 12
14
16 18 20
n
fIGURE
14
Variation avec n des coefficients de recombinaison radiative n'
(T'=500 K)
np
le long de la séquence de Ag(b)
reliée à la variation avec n des sections
efficaces au seuil a'
(O)(a).
np
1O- IZ
•
1
_,~_
•
1
1
•
1
1
b) Ag-like
3
.
10
,
.
,
,
!
!
1
1
T': SOOK
a) AS -like
4+Ag
10-13
H5b
~
C'
/9
. .
10'"
,
,
.
j
•
'
i
~
H
1
•
~.q
Cd+
2
10
!-a
Sp3+
• c:
.~
In2.+
10-14
-
11)-a
.o
~
ô 10
.....,
"'0
.. c
b
10-15
e- 11)'.
:.
..
1
!
\\0
......
,1
lS
4
6
8 .
10
12
14
16
18 20
10-101
--.---",---.:::-::=-"--•
10-"
i
L.
i
i
i
1
n
6
8
10
12 14
16
18 20
n
10'"
4
6
•
10
a
~
~
M
~
n
FIGURE 15
Variation avec n des sections efficaces au seuil a~d(O) le long de la séquence de Ag(a).
Variation avec n des coefficients de recombinaison radiative a~d pour T'=500 K(b)
et
TI = 5000 K(c).
98
ficaces correspondantes a'
(e:')
au
voisinage
du
seuil
con-
H
ns
H
duit à a'
(e:')
« a
(e:')
(figure 13(a)), et donc à a'
«a
ns
ns
ns
ns
De manière plus générale les valeurs de a'n
faibles par rap-
H
n~
port à celles de an~ sont
toujours
observées pour les états
n~ dont
la section efficace présente des caractères non hy-
drogénoldes marqués
ces caractères
se
traduisent
en
fait
par
une
réduction
des
valeurs
des
sections
efficaces
par
rapport à H.
b) Evolution avec n présentant un maximum
La courbe a'
de K présente un maximum
pour
n
= 5 ,
ns
0
lié à la très petite valeur de a
par rapport à celle de
4s(0)
aSs(O)
( figure
13b)
;
un raisonnement semblable explique le
maximum présenté par a'
pour Cd+ ( figure 14b).
nd
c) Evolution avec n présentant un minimum
2+
La figure 15(b)
fait apparaître pour a~d
de
In
un
minimum à n
= 10 suivi d'un maximum. Cette dépendance irré-
o
gulière en n est étroitement liée à celle des sections effi-
2+
caces au seuil a~d(O) de In
visible
dans
la
figure 15(a).
Le caractère non hydrogénolde marquant visible sur la
figure 14(b) est que a'
) aH
pour les
éléments
Ag_In 2+.
np
np
Pour ces éléments a'
(e )
< aH (e ")
au
voisinage
du
seuil
np
-
np
(figure 14(a)), et la décroissance de a'
(c ")
avec e:'
est
H
np
beaucoup plus lente que celle de a
(e:').
De
plus
les
va-
np
leurs relativement grandes des
potentiels
d'ionisation I np
donnent une contribution plus importante à a'
par
l'inter-
2
np
médiaire du terme (e:+l
qui apparaît dans l'équation (1.61).
n p)
La figure 16 compare l'évolution avec n de a'
(T'
=
ns
500 K)
le
long des
séquences
de
Rb,
Cu et
Ag.
On
retrouve
99
les mêmes caractères non hydrogénoldes déjà observés pour la
séquence
de
K et
la séquence de
Ag.
Le point
important
est
que
les
courbes
correspondant
aux
atomes
neutres
sont
re-
groupées pour n suffisamment grand.
Le même regroupement est
visible
pour
les
ions
monochargés
et
les
ions
doublement
chargés.
Ce comportement des coefficients al
est directement
ns
lié à celui des sections efficaces
correspondantes
cr'
(E')
ns
(voir
figure
10).
Il
montre
une
fois
de
plus
et
de
façon
évidente la grande similitude de cr~s(E')
le
long
des
trois
séquences pour une charge résiduelle donnée.
2) Variation de
a~~(T') en fonction de TI, n et ~ étant fi-
xés
Les figures 1S(b) et 1S(c) comparent les coefficients
a~d
pour
certains
éléments
de
la
séquence de
Ag,
calculés
respectivement
aux
températures
T'
= SOO K et S 000 K. Il
est visible que les caractères non hydrogénaI des de a~d évo-
luent avec T~ Une explication plus détaillée des différences
entre les figures 1S(b) et 1S(c) sera donnée ultérieurement,
après avoir discuté de
manière plus générale des caractères
non hydrogénoldes apparaissant dans l'évolution de a~~(T')
avec T'.
Pour
n
et ~ fixés,
le
coefficient
de
recombinaison
radiative a~~ (T 1)
a
en
général
une
décroissance
monotone
..
H (
)
avec la température TI comme pour le cas hydrogénoide an~ T' .
De
très
importantes
différences
avec
ce
comportement
sont
illustrées dans la figure 17, pour a'
(T') de
Zn+ et a'd(T')
ns
n
2+.
de
In
Dans l'intervalle de température considéré certains
coefficients a'
(T')
(n=S-8) et a'd(T')
(n=6-8)
ont
une
ns
n
croissance monotone avec T'. D'autres coefficients a'
(n>10)
ns
et a'd (n > 10) présentent une variation très irrégulière en fonction de
n
-
T'
caractérisée par un ou plusieurs extrema.
Cette évolution
très inhabituelle des coefficients a~~(T')
est
étroitement
liée
à
la
variation
des
sections
efficaces
correspondantes
cr~~(E') en fonction de l'énergie E'. De fait, la zone effec-
100
........... Rb-like
____ Cu-like
-._.- AS-like
4
6
8
10
12
14
16
18
20
n
FIGURE 16
Variation avec n des coefficients de
recombinaison radiative a'
(T'=500 K)
ns
pour les premiers éléments des séquen-
ces de Rb,
Cu et Ag.
161
~6
10-
.......
ï.q
-lsl
8
10
.......
"'fi
-let
-~•c:
...~
l$
8
10-17
-..1~1610
o
10-18
10- 17
a)
Zn+
b) In2 "
10-19
1
~ 10-181
i '
•
i
i
i
1
1000
2000 .
3000
5000
0
1000
.
"000
2000
3000
4000
i
o
sooo
T'(OK)
T'(OK)
FIGURE 17
Variation avec TI
des coefficients de recombinaison
2+(b).
radiative a~t de Zn+(a) et In
102
tive d'énergie des photoélectrons pour le calcul des coeffi-
cients de recombinaison croit avec la température. Lorsqu'un
maximum suffisamment prononcé de a~~(E') apparait dans cette
zone il en résulte un maximum aussi pour a~~(T').
Les
sec-
tions efficaces a'
(El)
de Zn+ sont au demeurant de type (b)
ns
2
ou
(c),
ce Il es cr~i E ') de In + de t yP e (d ) 0 u Ce ) • Le ra pp0 r t du
maximum de a~~(EI) à la valeur au seuil a~~(O) ou au minimum
non nul de a~~(E') dépend considérablement de n, et par con-
séquent certains coefficients a~~(T') ont une variation avec
T'
plus ou moins régulière que d'autres dans l'intervalle de
température conidéré.
Les coefficients qui croissent avec T'
dans
cet
intervalle atteignent un maximum pour une tempéra-
ture
T'
> S 000 K et décroissent ensuite comme prédit par
l'équation (1.61).
La variation des coefficients a~~ (T ,)
avec
T'
illus-
trée précédemment explique bien la disparition observée dans
la
figure
1S(c)
à T'
= S 000 K des extrêma apparus dans la
.
( )
2+
+
2+
flgure 1S b
à T'
= SOO K pour a~d de In
et Cd . Pour In
la croissance de a 1Od (T') avec T'est plus rapide que celle
+
de a~d(T')
(n > 10)
(voir figure 17).
Quant à Cd ,
a'
(T')
Sd
croit avec T'
à partir d'un minimum alors
que
les
a'
(T')
nd
(n > 5) décroissent. La disparition des maxima à T'
= SOOO K
s'est
traduite
par
des
discontinuités
de
pente
dans
les
courbes a~d'
L'évolution
des
coefficients de
recombinaison
radia-
tive a~~(T') avec T'
a permis de mettre en
évidence des ca-
ractères non hydrogénoldes en rapport avec ceux des sections
a~~ (E ') existant au delà du voisinage immédiat des seuils.
3)
Var i a t ion d e a~ ~ ( T ,) a ve c ~, net T'
é tan t
f i x é s
L' évolut ion avec ~ de a~~ (T')
pour n et
T'
fixés
est
analysée
ici
sur
l'exemple
particulier
des
coefficients
103
+
Ci
de Rb et Ca
pour
di fférentes
températures
T' •
S2.(T')
Plus précisément la figure 18 présente l'évolution avec 2. de
Ci
de
Rb pour
T'
= 500 K et 5000 K et celle de
S2.(T')/Ci S(T')
la même quantité pour Ca+ pour
TI
= 500 K et 2500 K. L'évo-
lut ion de CiS2./CiS est liée à celle de Ci S2.'
Pour Rb,
Ci
croit, atteint un maximum pour 2. = 2.
S2.
M(T')
puis d c r o t , L'accroissement de Ci
avec
2.
est
liée
au
é
ï
S2.
poids statistique 2(22.+1) apparaissant dans l'équation (1.61)
et à la variation de 0'132.(0)
qui
augmente
aussi
avec 2. jus-
qu'à
at teindre
un maximum
puis
décroî t ,
La décroissance
de
Ci
pour 2. > 2.
est liée à la décroissance de O'S2.(O)
pour
S2.
M
les grands 2. et aussi surtout au
fait que O'S2.(€')
décroît
d'autant
plus vite avec g'
que 2. est grand.
La variation de
CiS2./CiS
de
Rb est
analogue
pour
toute
température.
Pour
les
grandes températures cependant le maximum est plus important
et il apparaît pour une plus faible valeur de 2.. Ceci est dû
au
fait que Ci
décroît d'autant plus vite avec T'
que 2.
S2.(TI)
est
grand.
Une
évolution
analogue
avec 2.
apparaît
quel
que
soit
n dans
Rb
et
dans
tous
les
éléments
neutres
que
nous
avons
étudiés.
Cette
évolution
est
très
semblable
à
celle
obtenue dans H.
Dans Ca+ le comportement de Ci'n/Ci' est très différent
nA.
n
pour tout n > 6 comme cela est visible sur la figure 18(b).
Quel que soit n > 6 et T', Ci'n/Ci'
présente
un
minimum
pour
-
nA.
n
2. = 2.
En effet dans Ca+ les sections efficaces O'~d(g')
au
seuil
(figure
11a)
et
près
du
seuil
sont
particulièrement
faibles;
pour n > 6 la variation de 0'~2.(0)
avec 2. présente
alors
un
minimum pour
2. = 2 encadré de deux maxima,
évolu-
tion qui se répercute sur la variation de Ci~2. avec 2., De ma-
nière
plus générale un comportement semblable avec un mini-
mum pour un 2.
donné>
2
apparaît
pour
tous
les
ions
pour
0
lesquels l'évolution avec n de O"n (0)
présente
un
minimum
nA.o
très prononcé (voir les figures 11 et 12).
·4
1
1
1
1
1
1
1
.4
o.) Rb
1
b) Ca+
,\\
l
,
• T:SOOK
.3 J
+ T':500K
.3 J
.T=2500K
, \\
o T :SOOO.K
1
\\
, \\
+-
,
.0
\\
1
,
~
.. G
1
<,
~
,
1
.. .2.
...
G
""'.2
...j
J
\\
.. Cl
1
?S
0
1
\\
~
~
1
1
\\
1
1
\\
1
.1 J
1
\\
.1
1
1
\\
1
1
\\
l
1
\\
1
1
\\ 0,
J
,
o s
,
,
,
,
,
'0
1
0
,
1
,
0
t
2
3
4
5
6
7
8
0
Z
3
4
5
6
1
8
t
1
FIGURE 18
: Evolution avec ~ du rapport n8~(T')/a8 (T') pour
divers Tt dans Rb(a) et Ca+(b).
105
Les
caractères
non
hydrogénoldes
très
marqués
des
coefficients de recombinaison radiative étudiés précédemment
ont surtout concerné les a'n(T').
Les coefficients a'(T') et
nN
n
a t (T') en présentent d'autres moins marqués (Annexes II et
III),
tout en ayant une décroissance avec n ou
T'
analogue à
celle
de
H.
Il
n'existe
pas de
résultats expérimentaux
pou-
vant être comparés aux nôtres.
Les quelques résultats,
théo-
riques,
concernent
surtout
le
coefficient
de
recombinaIson
total at(T').
(Annexe
III).
Là
encore
d'autres
résultats
théoriques
et
expérimentaux
sont
nécessaires
pour
une
plus
grande
comparaison
et
pour
mieux
tester
la
validité
de
nos
calculs.
107
CONCLUSION
Le modèle de
champ central
non relativiste utilisant
un potentiel central paramétrique semi-empirique ou ab-initio
nous a permis de déterminer les sections efficaces de
photo-
ionisation
des
états
fondamentaux
et
excités
de
nombreux
éléments
des
séquences
de
K,
Rb,
Cu et Ag.
Les calculs ef-
fectués
concernent
la photoionisation de
l'électron externe
de
valence
au
voisinage
du
seuil
d'ionisation.
Des
valeurs
de
sections efficaces nous
avons déduit les coefficients de
recombinaison radiative d'électrons peu énergétiques sur les
états excités des mêmes éléments.
Dans les séquences de K et
Rb l'étude de la recombinaison radiative à faible températu-
re a été complétée par la détermination des coefficients de
recombinaison
sur
chaque
couche
et
des
coefficients
de
re-
combinaison radiative totaux.
La
validité
des
résultats
de
sections
efficaces
de
photoionisation a été analysée en étudiant leur sensibilité
au
choix
du
potentiel
central
utilisé
et
en
les
comparant
systématiquement
aux
résultats
antérieurs,
malheureusement
très
peu
nombreux.
Par
ailleurs,
des
calculs
relativistes
complémentaires
de
sections
efficaces
effectués
pour
les
ions
multichargés
moyennement
lourds
indiquent
que
les
ef-
fets relativistes ont peu d'influence sur nos résultats.
Ce-
ci justifie entièrement le choix de notre modèle non relati-
viste
pour
le calcul extensif d'un très grand nombre de
va-
leurs de sections efficaces de
photoionisation.
Nous avons donc pu étudier la systématique de la pho-
toionisation à partir des états excités et de la recombinai-
son
radiative
pour beaucoup d'éléments neutres ou
ionisés à
un électron de valence.
Aucune étude de cette ampleur n'avait
été réalisée auparavant dans ce domaine.
108
Tous nos résultats ont été comparés de manière systé-
matique
à ceux obtenus en utilisant le modèle hydrogénolde.
L'analyse
très
détaillée
des
caractères
non
hydrogénoldes
apparaissant dans
les sections efficaces de photoionisation
a été faite en utilisant une méthode basée sur la théorie du
défaut
quantique.
Cette méthode
originale s'est avérée très
performante pour
l'étude de
la systématique de ces caractè-
res.
Les principaux
caractères non
hydrogénoldes concernent
l'apparition
de
un
ou
plusieurs
extrèma-(minima,
maxima)
dans les courbes de sections efficaces partielles crn~,~,(E:).
Notre méthode donne
aisément
le nombre prévisible de minima
et la forme typique caractéristique de
la courbe crn~,~' (E:)
pour
chaque
transition
n~
-+
E:~'
de
chaque
élément
étudié.
Le
nombre
de
minima,
qui
sont
liés
à
la
pré s e nc e
de
zéros
dans
les éléments de
matrice dipolaires,
dépend des valeurs
des différences des défauts quantiques asymptotiques 6~~~, =
~~,-~~ comparées à des grandeurs critiques 6~~~, caractéris-
tiques de chaque transition ~ -+ ~'.
Des
caractères
non
hydrogénoldes
s p c i fiques
de
la
é
photoionisation
des
états
excités
ont
pu
être
dégagés.
Les
sections
efficaces
des
orbitales
excitées
sans
noeuds
(3d,
4f)
peuvent
présenter des minima.
Jusqu'à trois minima peu-
vent apparaître pour certaines transitions n~ -+ ~+1, en parti-
culier pour les transi tians
nd
-+ E: f.
Des
minima
apparaissent
aussi
pour
de
nombreuses
transi tians
n~ -+ E: (~-1 ),
jusqu'à
deux minima pour certaines transitions nf -+ E:d. Tous ces mi-
nima
n'ont
jamais
été
prédi ts
pour
la
photoionisation
des
états fondamentaux.
L' apparition
de
minima
dans
les
courbes
de
sections
efficaces partielles réduit considérablement les valeurs des
sections efficaces
relativement
à celles du modèle hydrogé-
nolde.
L'influence de
ces minima sur les sections efficaces
totales est variable,
particulièrement importante lorsque les
deux
sections
efficaces
partielr~s présentent des minima
109
pour
des
énergies
de
photoélectron
voisines,
faible
lorsque
se u l e l a s e c t ion e f fic ace rel a t ive à l a t r ans i t ion n2. ~ e: ( 2.-1 )
présente des minima.
Nous avons étudié pour chaque élément l'évolution des
caractères
non
hydrogénoldes
le
long
des
séries
de
Rydberg
ns-nf,
en analysant
tout
particulièrement la variation avec
n des sections efficaces au seuil et l'évolution de
la forme
des courbes de section efficace. Dans tous les cas on obser-
ve
une évolution pour les n faibles suivie d'une stabilisa-
tion des caractères non hydrogénoldes pour n grand.
L'évolu-
tion pour n faible est très irrégulière pour les transitions
n2. ~ e:2.' caractérisées par un \\ t.).I2.2.' 1 proche
dl une
valeur
critique 1t.).I~R:1 +k-1
caractéristique
de
l'apparition d'un mi-
nimum
pour
ces
séries
de
Rydberg
on
observe
un
ou
deux
changements de
forme des courbes de section efficace lorsque
n augmente,
puis pour n suffisamment grand la forme de cour-
be
ne
change
plus
et
la
position
des
extrèma
devient
sta-
tionnaire. Lorsque
1t.).Iu,1 diffère des valeurs 1t.).I~2.' l+k-1,
la
variation avec n pour les valeurs de
n faibles est très
ré-
gulière.
Nous
avons
analysé
en
détail
l'évolution
des
carac-
tères non hydrogénoldes des sections efficaces le long de
la
séquence des alcalins Li-Cs et le long des quatre séquences
isoélectroniques considérées.
Nous avons
de
plus comparé le
comportement le long des quatre séquences. Dans tous les cas
la systématique de ces évolutions découle des variations des
différences de défauts quantiques.
Pour une transition nl~e:V
donnée,
des
différences
de
comportement
importantes
résul-
tent
des
di fférences
de
nature
des
orbi tales 2. et 2.'
mises
en
jeu,
en
particulier
du
caractère
pénétrant
ou
non
péné-
trant de celles-ci, qui pour 2. ~ 2
dépend
considérablement
de
l'élément étudié.
Nous allons brièvement résumer les con-
clusions
les
plus significatives auxquelles nous sommes ar-
rivés.
110
En
utilisant
des
résultats
antérieurs
obtenus
pour
Li,
Na et Cs qui complètent ceux que nous avons obtenus pour
K et Rb nous avons analysé l'évolution le long de la séquen-
ce
des
alcalins
Li-Cs.
Pour
tous
les
alcalins
les
transi-
tions n s .... e:p et
np .... e:s ont un comportement semblable.
Par
con t r e
pou r I e s
t r ans i t ion s
n d .... e:f et n f.... e: d des car a c t è -
res
non
hydrogénoldes
nouveaux
apparaissent
lorsque
Z aug-
mente,
particulièrement marqués pour Cs.
La
variation
isoélectronique
le
long
des
quatre
sé-
quences
étudiées
dépend
là
encore
de
la
transition
n~ .... e:~'
considérée
et
est
directement
reliée
à
la
variation avec
z
de
16JJ~~, 1. Pour les valeurs de ~ et ~' faibles, 16JJ~~, 1dé-
croît toujours avec z et par suite les caractères non hydro-
génoldes s'estompent
petit
à
petit lorsque z augmente.
Cet-
te caractéristique a été antérieurement notée pour la photo-
ionisation d'orbitales fondamentales ns et np le long de sé-
quences isoélectroniques.
De plus pour z donné !6u
1
dépend
sp
très
peu
de
Z et
le
comportement
isoélectronique
des
sec-
tions efficaces à partir des états ns et np est très sembla-
ble
pour
les
quatre
séquences
étudiées.
Pour
des
valeurs
plus
grandes
de ~
et ~ "
dans
certains
cas
on
observe
une
augmentation de
16JJ~~1 1 avec z au début des séquences suivie
en sui te d 1 une déc roi s san c e ré qu I i ère . De pl us
\\6 u~ ~ , 1 dépend,
à z donné,
considérablement de
la séquence étudiée,
les or-
bitales
d
et
f
devenant
pénétrantes
pour
Z
suffisamment
grand.
Ainsi
des
caractères
non
hydrogénoldes
absents
pour
les premiers éléments de
la séquence peuvent apparaître pour
des ions plus chargés.
Ceci est particulièrement marqué pour
les transitions nd .... e:f de
la séquence de K et nf .... e:g de la
séquence de Ag.
De plus on peut noter que pour certains ions
.
h a r o
Y10+
1 12+ d
. .
.
t
d
é
aUSSI c arges que
ou
n
es mInIma apparaIs sen
ans
les courbes de section efficace nd .... e:f.
En ce qui concerne la recombinaison radiative ce sont
les coefficients ~n~(T) de recombinaison sur un état n~ donné
111
qui
présentent
les
caractères
non
hydrogénoldes
les
plus
marqués.
Ces caractères, particulièrement frappants pour des
températures
faibles,
découlent
directement
de
ceux
appa-
raissant dans les sections efficaces totales de photo ionisa-
tian
des
états
n1,
et ceci
au
voisinage du
seuil d'ionisa-
tion.
Nous avons analysé l'évolution avec n de Cl
le
long
n1
des séries de
Rydberg ns-nf et ceci à température fixée.
Les
extrêma observés pour certaines séries sont directement cor-
rélés
à
ceux apparaissant dans les courbes de section effi-
cace 0n1(e)
au
voisinage des seuils.
Les caractères non hy-
drogénoldes des sections efficaces de photoionisation se ré-
percutent
aussi sur
l'évolution
avec
la température de nom-
breux coefficients Cl
( T)
lorsque
T
augmente
certains
n1
Cl
(T)
évoluent
de
façon
très
tortueuse
et
la
décroissance
n1
monotone
hydrogénolde n'est
atteinte qu'à partir d'une cer-
taine température.
Finalement la variation de Cl
( T) avec 1,
n1
pour n
et
T fixés
présente elle aussi
parfois
un comporte-
ment très différent de celui obtenu pour H.
Les
coefficients
de
recombinaison
radiative
sur
les
couches n et les coefficients totaux présentent des caractè-
res non hydrogénoldes moins marqués que les Cl
( T) .
Cepen-
n1
dant
les
écarts
par
rapport
aux
résultats du
modèle hydro-
génolde
restent
notables,
particulièrement
pour
certains
coefficients Cl (T) correspondant aux couches n les moins ex-
n
citées.
Pour
juger de
la qualité de nos résultats concernant
la photoionisation et
la
recombinaison
radiative,
nous dis-
posons de
très
peu de résultats antérieurs.
D'autres études
théoriques
et
surtout
des
données
expérimentales
seraient
très souhaitables. En particulier i l est à noter que l'exis-
tence
de multiminima dans
les courbes de
sections efficaces
de
photoionisation des états excités n'est toujours pas vé-
rifiée expérimentalement.
112
L'étude de
l'évolution des sections efficaces de
pho-
toionisation
le
long
des
séries
de
Rydberg
laisse
prévoir
l'existence
d'un
minimum
dans
la
distribution
des
forces
d'oscillateur discrètes de nombreuses séries n~ ~ nl~1 lors-
que
n'
varie.
Il serait intéressant d'étendre nos calculs à
l'étude de ces transitions.
D'autres
observables,
telles
les distributions
angu-
laires
et
la
polarisation
de
spin
des
photoélectrons
sont
connues
pour
être
très
sensibles
au
détail
des
fonctions
d'onde.
Une
étude
systématique
des
caractères
non
hydrogé-
noldes
de
ces grandeurs
serait souhaitable et pourrait être
réalisée en utilisant le modèle du potentiel central paramé-
trique relativiste.
Par
ailleurs
il
serait
intéressant
d'étudier
la
re-
combinaison d'électrons plus énergétiques, c'est-à-dire pour
des températures plus élevées.
Il serait alors nécessaire de
calculer
les sections efficaces de
photoionisation pour des
énergies de
photoélectrons plus élevées en
tenant compte de
l'excitation du coeur.
La prise en compte des effets d'auto-
ionisation ne pourrait se faire que dans le cadre d'un modè-
le plus élaboré que celui que nous avons utilisé.
La
généralisation
de
notre
étude
de
systématique
à
des
systèmes
à
plusieurs
électrons
de
valence
serait, elle
aussi
très
souhaitable,
mais
bien
sûr
là
encore
il
serait
nécessaire
de
prendre
en
compte
les
effets
de
corrélations
en utilisant un modèle théorique plus compliqué que celui de
notre étude.
113
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J. Phys. B: At. Mol. Phys. 11 (1984) 993-1007. Printed in Great Britain
Central-field calculations of photoionisation cross sections of
exdted states of Rb and Sr" and analysis of photoionisation
cross sections of exdted alkali atoms using quantum defed
theory
M Aymar, 0 Robaux and S Wane
Laboratoire Aimé Cottont. CNRS II. Bâtiment SOS. 91405 Orsay Cedex. France
Received 7 June 1983. in final fonn 24 October 1983
A.......d. Photoionisation cross sections for excited ni states (n ~ 20, 1~ 4) of Rb and Sr'"
have been computed in the framework of a single-electron model by the use of a central
potential, The evolution of non-hydrogenic behaviour of photoionisation near threshold
is studied along a given series. Moreover, isoelectronic variations from Rb to Sr'" as weil
as systematic trends along the sequence of alkali atoms Li through Cs arediscussed. The
non-hydrogenic traits. mainly the occurrence of minima in photoionisation cross sections.
are analysed in tenns of quantum defect theory.
.
1. IntrodllCtioa
In recent years, there has been an increased interest in the study of photoionisation
processes of excited atoms and ions because of the importance of these processes in
radiative transfers involved in laboratory, astrophysics or controlled thermonuclear
plasmas. Moreover the advances in tunable lasers have made experiments in which
large numbers of selectively excited atoms are produced possible. From thèse populated
excited levels, ionisation experiments can be perfonned either providing direct
measurement of photoionisation cross sections or allowing the study of collisional
ionisation between different excited species. Most of the experiments involving ionising
processes from excited states deal with alkali atoms,
On the theoretical side, a lot of attention has been paid recently to the analysis of
systematic trends of non-hydrogenic behaviour of excited-state photoionisation (Aymar
et al 1976, Aymar 1978~ Msezane and Manson 1975, 1982, Lahiri and Manson 1982~
Devdariani and Klyucharev 1977). Most of these papen aOO concem the alkali atoms
Li, Na. K or Cs.
Rb has been less thoroughly studied than other alkali atoms and data on photoionisa-
tion cross sections are limited to low-lying states (Klyucharev and Sepman 1975,
Ambartzumian et al 1976, Moskvin 1963. Chichkov and Shevelko 1981). Additional
data on Rb appear to be highly desirable to help interpret the experiments perfonned
by Cheret et al (1982a, b) on ionising collisional processes of highly excited Rb atoms
and to study the systematics of excited photoionisation cross sections in alkali atoms.
t Laboratoire associé à l'Université Paris-Sud.
0022-3700/84/060993 + 15$02.25
© 1984 The Institute of Physics
993
994
M Aymar. 0 Robawc and S Wane
We report here new results on photoionisation cross sections for excited states of
Rb and Sr+-the first ion of the Rb isoelectronic sequence. Calculations are performed
within the framework of a non-relativistic single-electron model by the use of a central
potential as explained in § 2. The results on the outer-shell photoionisation cross
sections for the ns to ng Rydberg series of Rb and Sr" are presented for values of n
up to 20 in § 3. Emphasis is given to the analysis of the non-hydrogenic behaviour of
the photoionisation near threshold, Section 4 concerns, in addition to the new calcula-
tions performed in Rb and Sr", previous results obtained in light alkali spectra Li to
K (Aymar et al 1976) and in Cs (Msezane and Manson 1975, Lahiri and Manson
1982). The systematic trends of the partial photoionisation cross sections of excited
states are analysed in terms of quantum defect theory; the evolution along a Rydberg
series, the trends along the sequence of alkali atoms Li through Cs as weil as the
isoelectronic variation from Rb to Sr+ are discussed.
2. ne single-particle central-field model
2.1. Basic formulae
Within the framework of a single-particle central-field model (non-relativistic) the
cross section (in cm2) for photoionisation of a nl state of a one-electron system is
given (Stewart 1967) in the dipole approximation by
(
)
-18
(1
2
1+ 1 2
)
(Tnl
(1)
e =0.855XI0
(e-elll)
2/+1 Rnl.I-d e)+2/+1 RIIL.I+de)
where elll( <0) is the binding energy of the ni electron and e(>O) is the energy of the
photoelectron (ail energies are in Rydbergs). R rtL.l:d (e ) are the radial matrix elements
given by:
f
RIIL.l'(e) ==
PIII(r)Q(r)P.r(r) dr
(2)
where Q(r) is the dipole operator. The same central potential V(r) is used to generate
PlII(r) and Pal,(r) solutions of the Schrôdinger equation:
d2
l(/+l))
( dr2+E -2 V(r)
~
PBl(r) =0
(3)
with E = elll or e.
The numerical factor in equation (1) implies that the continuum function is nor-
malised per unit energy range so that
Lco P.,(r)P.,I(r) dr= 1rc5(e-e').
(4)
Here Pat(r) has the asymptotic form
Pd(r) -
e-1/4sin[';;r_l1r+ ~ln2J;r+argr(I+I-i:')+8
(5)
1(e)]
,-co
2
.y e
Je
where z - Z - N + 1 is the residual charge of the final ion and 8,(s) is the phaseshift
with respect to hydrogen-like wavefunctions.
Photoionisation cross sections of excited alkal! atoms
995
2.2. General remarks on non-hydrogenic behaviour of thephotoionisation cross sections
The hehaviour of photoionisation cross sections when the potential V(r) either oheys
the Coulomb law or represents a much more realistic potential has been previously
descrihed by Manyauthors (Bethe and Salpeter 1957, Fano and Cooper 1968, Burgess
and Seaton 1960) and only fundamental points will he recalled here.
For hydrogen, the radial matrix elements R ,".Iz1(s) are always monotically decreas-
ing functions of e. Then the partial photoionisation cross sections 0',,1,1,* 1(s) as weIl as
the total cross section 0'rU ( s) are maximum at threshold and drop to zero as e inereases.
For 1#:0, the O'rtl,I+I(e) contribution to the total cross section is much larger than the
0',,1,1-1 (s) contribution. For a given ni series the threshold value 0'",(0) increases as
n: The asymptonc trend for high energies is proportional to e -1-7/2 and approximately
proportional to n-, for n » L
Simîlar hehaviour holds for hydrogen-like ions and the cross section of a hydrogen-
like ion is related to the hydrogen cross section O'H by the relation:
O'(e/ Z2) = O'H(e)/ Z2.
(6)
The comparison of the cross sections calculated in Rb and Sr" with hydrogen-like
values will he carried out using scaled cross sections and energies defined by the
relations:
(7)
For non-hydrogenic atoms or ions, the evolution of the cross sections with n, 1 or
e' is modified. In fact the discrete P",(r) and continuum P.'I' (r) orbitaIs are shifted
towards the nucleus with respect to hydrogen-like orbitais and the overlap of P",(r)
and p.'" (r) is modified. Consequently partial and total cross section values can strongly
difîer from hydrogen-like values. In particular the contribution of the O'~I,I_I (s') partial
cross section is not always small. The MOSt striking non-hydrogenic trait is the
occurrence of zeros in the R ,,1,1'( e') radial matrix elements, giving minima in the partial
cross section curves.
Non-hydrogenic hehaviour of excited-alkali-atom photoionisation cross sections
have been previously studied using central-field models, The light alkali atoms Li to
K were investigated by Aymar et al (1976) and by Aymar (1978) and Cs was analysed
by Msezane and Manson (1975, 1982) and by Lahiri and Manson (1982). Various
non-hydrogenic shapes have been obtained for O'",.,,(e') cross section curves, as can
he seen in figure 1. In addition to the weIl known Cooper minimum (Fano and Cooper
1968) corresponding to case (c), one (e) or two additional minima (f) have been
predicted in some particular cases.
2.3. Central-field models used to eoaluate pnotoionisauon cross sections in Rb and Sr+
Calculations have been performed using three different central potentials V(r).
(i) The cental potential corresponds to the parametric potential introduced by
Klapisch (1971) already employed in the previous photoionisation calculations in light
alkali atoms (Aymar et al 1976, Aymar 1978). This potential is represented by an
analytic function depending on a set of parameters, each parameter describing the
distribution of charges in a shell of the atomic core. The optimal potential is determined
996
M Aymar, 0 Robaux and S Wane
(f)
e
Figure 1. Sc:hematic cross section curves for six typical cases.
by rninimising the root-mean-square deviation between observed and calculated ener-
gies (to the first order) of a few selected levels.
(ii) The central potential has a simple analytical form depending on three para-
meters
Vo=-r-1[z+(Z-z) exp(-atr)+azrexp(-a3r)].
(8)
The parameters are determined here by comparing the experimental energies with
zero-order calculated ones. This potential has already been used successfully to analyse
various multiphoton processes in He and Cs (Aymar and Crance 1980, Crancé and
Aymar 1980).
(iii) Long-range core polarisation effects are taken into accout by adding to Vo an
effective polarisation potentiaJ Vpol with the form
V pol = -!adr-4(l-exp-(r/ rc)6]
(9)
where ad is the static dipole polarisability of the core (Shevelko and Vinogradov 1978)
and rc is an effective core-radius eut-off, The parameters ah a2' a) and rc are adjusted
to yield zero-order ca1culated energies close to experimental values.
In the calculation of radial matrix elements (equation (2» we use the dipole length
fonn of the dipole operator. In approximations (i) and (ii) Q(r) is the usual r operator.
In the third approximation (iii), we used a modified dipole operator which includes
the effects of core polarisation (Hameed et al 1968, Weisheit 19718, b)
Q(r) =r{l- adr-3[1-exp(-r/ rc)3]}.
,-(lO)
The Schrôdinger equation (3) was solved using different numerical methods
described in the the appendix.
3. Resolu for Rb and Sr+
3.1. Introductory remaries
Photoionisation cross sections have been computed for nl series (O"l~4) of Rb and
Sr+ for n values up to 20. Only the contribution of ejection of the outer nl electron
Photoionisalion cross sections of excited alkali atoms
997
to the photoionisation cross sections is considered in this work. Moreover autoionisa-
tion effects which cannot be described in the framework of a single-electron model
are ignored. Therefore the validity of our treatment to describe total photoionisation
cross sections is confined to the near-threshold energy range.
In Rb, autoionised lines corresponding to the excitation of the 4p inner-shell
electron have been obtained for energies larger than 0.8 Ryd above threshold. In Sr"
similar autoionised lines are expected but not yet observed. Nevertheless calculations
are perfonned for higher photoelectron energies in order to deteet the various minima
occurring in O':"'r(e') curves and analyse the systematics of thèse minima.
3.2. Non-hydrogenic behaviour of cross section curees
Total cross section curves for 8/(OEi lEi4) excited states of Rb and Sr" are comparee!
with hydrogen cross sections in figure 2. The non-hydrogenic character is most striking
for 8s levels. The Cooper minimum (case (c » occurring in photoionisation cross sections
of the ground state of the alkali atoms Na to Cs (Marr and Creek 1968) also appears
for aIl excited ns states of Rb and for highly excited ns states of Sr+ (n ;;.13). For
the ground state and low-lying excited states of Sr" the cross sections curves are of
type (b) (see figure 2(c». The cross section curve is simlar to that of the ns Li states.
For 1#: 0, total cross section curves present a hydrogen-like decrease from threshold
(figures 2(b)-(c». However cross section values often strongly difier from H values.
In fact for 1Ei 3 several partial cross section curves O'~l.l· (E') exhibit a Cooper minimum.
For a11 np and nf states of Rb and Sr+, one partial cross section curve is of type (c)
and the other of type (a). For np states the O'~P.d(E') partial cross section curve has
a minimum near threshold; since in this energy range the contribution of O'~p,s(E') is
not negligible, the total cross section curve exhibits no minimum at all but only a slope
discontinuity near the O'~p,d (E) zero. A typical example is shown in figure 3 which
corresponds to the photoionisation of the 5p state of Rb. For the nf states the total
cross section is mainly related to the O'~f.I(E') contribution which is alsmost equal to
the corresponding hydrogenones. Then the total cross section is rather insensitive to
the minimum which occurs in the O'~f.d(E') partial cross section and the O'~f(E') values
for Rb and Sr" do not ditfer much from H values. For nd states of Rb and Sr" bath
102
(a J
10
-
.c
1
2:
t» 10""'
10.2
10-1
0
0.1
0.2
0.3
0.4 0.5 0
0.1
0.2
0.3
0.4 0.5 0
0.1
0.2
0.3
0.4 0.5
hy'(RydJ
FIpre 2. Total scaled cross sections Z2 a 8, (in Mb, 1 Mb -10-'8 cm2) plotted against the
energy of the transition III" - (6 - 6 11, ) / Z2 for 1- Q-4. (ta) H; (b) Rb; (c) Sr".
998
M Aymar, 0 Roba·wc and S Wane
10 ,-L_ _---L_ _---L_ _---L_ _---L...,
2
10
,
1
\\
\\
\\
\\
! 10-'
\\\\
-
\\
a
\\ ..
,..
10-2
'"':'..:
10-1
.
....'""':".....,.:..,..:...........
--
.
10-4
.
0
5
1
2
5
10
15
20
t ( Ryd)
n
F"1pftl 3. Partial and total cross section curves for
F"1pftl 4. Scaled cross sections at threshold for the
the Sp state of Rb: - - , 0'5p(e); ••••, 0'5P.d(6); ---,
ns series: Li, K (Aymar et al 1976), Na (Aymar,
0'5p..(e),
1978), Rb, Sr+ (this work).
400
300
.Q
%: 200
100
5
10
1S
20
n
........ 5. Scaled cross sections at threshold for the np series: Li, Na, K (Aymar et al
1976), Rb, sr" (this work).
Photoionisation cross sections of excited alkali atoms
999
partial cross section curves are of type (c) except O'~.p(e') of Sr" which is of type (b).
For a given nd state, the minimum for O'~d.f(e') occurs for an energy e2 larger than
the energy s~ corresponding to the minimum of O'~d.p(e'). However, around SI, the
contribution to the total cross section of O'~dJ is very large, while around e2 the
contribution of O'~d.P is very smaU. Therefore the total cross section exhibits a minimum
only near e2 (outside the energy range reported on figure 2(b)-(c)). For larger values
of l(l Sil: 4) partial cross section curves never have a minimum (type (a)) and total cross
section values O':"(e') are very close to hydrogen ones.
The presence of minima in partial cross section curves for ni states (1.. 2) has a
great influence on the values of cross sections as shown in figures 4, 5 and 6. In these
figures total cross sections at threshold for ns, np and nd series of Rb and Sr" are
compared with hydrogen values. Previous resuIts obtained for light alkali atoms
(Aymar et al 1976, Aymar 1978) have also been reported. For s states of aIl alkali
atoms, 0'".(0) are much sma11er than H values because of the large cancellation eftect
arising in R"... p(O) matrix elements. For Sr", threshold cross sections are still much
smaller; the minimum in the curve giving 0'".(0) against n corresponds ta the change
from (b) to (c) shape, Le, to a Cooper minimum located very close to the threshold.
For p and d states differences between 0'~1(0) values obtained either for Rb (Sr") or
for H are smaller than for s' states, but nevertheless important (figures 5 and 6).
Moreover, in contrast to the hydrogen case, both partial cross sections give a large
contribution to the total cross section. This is illustrated in figure 7 which shows the
n dependence of O'~d.p(O), O'~dJ(O) and O'~d(O) for Rb and Sr"..
3.3. Comparison with previous works: Discussion
Our predictions for excited-state photoionisation of Rb are compared with previous
experimental and theoretical results in table 1. Photoionisation cross sections of the
3
5
10
15
20
n
Fipn 6. Scaled cross sections at tbreshold for the "d series : U, Na, K (Aymar et al
1976), Rb, Sr'" (tbis work).
1000
M Aymar, 0 Robaux and S Wane
300
R~/
/
/
/
/
/
Rbf
~-- --
/
+
100
_ - - - /
Sr
:0-"----
5
10
1S
20
n
Fipre 7. Partial and total scaled cross sections at threshold for the "d series of Rb and
Sr", Partial cross section values C1'~d.P(O) and C1'~d.l(O) are respeetively referred to by
indexes p and f.
Rb ground state are compared with the measurement of Marr and Creek (1968) in
figure 8. For excited states satisfaetory agreement is obtained with previous results
but data are too scarce to choose between the different central-field approximations
(see § 2.3). On the contrary, for ground-state photo ionisation only the third approxima-
tion corresponding to core-polarisation efleets included in the potential and in the
dipole operator gives results in good agreement with experiments. Consequently the
third approximation has been chosen for the results presented in figures 2 to 7.
0.4 .-J-
L...-_ _...l-._ _--J.._ _--l.
....,
0.3
i! 0.2
-l:I
0.1
o
0.1
0.2
0.3
0.4
0.5
t (Rydl
Fipre 8. Ground-state photoionisation of Rb. Comparison of measurement of Marr and
Creek (1968) wim the predictions provided usina thrce ditlerent central-field models (i),
(ü), (iü) (sec § 2).
Pbatoionisation cross sections of excited a/kali atoms
1001
Table 1. Comparison of the predictions obtained for Rb with three ditferent central·field
models (i), (ii), (ili) (sec § 2) with previous data: (iv), theoreticaJ result of Moskvin (1963)
(only the tbrehsoJd values have been extracted from the small publisbed curves), (v) and
(vi), measurements of Klyucharev and Sepman (1975) and Ambartzumian " al (1976)
respectively.
State
Energy
This work
Previous data
5p
.-0
f2.S
a14 (iv)
(i)
14.0 (ü)
13.0 (ili)
{e -0.016
{U.9 (i)
aiLS (iv)
A-O.44,..,m
13.0 (ü)
12.2 (iü)
9.6:t:0.2 (v)
6p
{e -0.04 Ryd
{ 9.9(i)
6P3/2
17
:t:4 (vi)
"-14404 cm- t
10.7 (ii)
9.7 (iii)
6PI/2
15
:t:4(vi)
{, -0.17 Ryd
{ 3.2 (il
6p3/2
1.9:t: 0.5 (vi)
,,-28806cm- '
3.3 (ii)
3.3(iii)
4d
,==0
f3.3 (i)
a40 (iv)
35.7 (ü)
34.0 (ili)
6s
,-0
0.85 (i)
... 1 (iv)
1.0 (ü)
0.77 (ili)
However, one must notice that the photoionisation cross sections of nd states and
low excited ns states of Rb and Sr + are found to he particularly sensitive to the model.
This is illustrated by figure 9 which shows the threshold values obtained for ns. np
and nd states of Rb and Sr" with the three different central-field models described in
§ 2. The influence of core-polarisation effects introduced in the third approximation
(iii) is evident only for low ns states of Rb and Sr+. For the other states the
40
( c)
(i) .:1····
...
III
. / . Rb
30
-.0
E
e
20
~.#.'
. :
.....
(Iii)
10
l"I Sr·
!!.--
-------------
s
10
1S
20
S
10
15
20
5
10
15
20
n
...... ,. Scaled cross sections at thresbold cak:ulated for Rb. with three ditferent approxi·
matioas and for Sr+ with t'No modela (sec f 2) for the liS (ta), IIp (b) and rad (c) series.
1002
M Aymar, 0 Robaux and S Wane
modifications brought about by the introduction of thèse effects are of the same order
of magnitude as the differences between the predictions of the two models neglecting
core-polarisation effects (Ii), (ü». Thus it appears that the accuracy of the results
greatly depends on the quality of the central core potential and not ooly on the correct
treatment of core-polarisation effects as emphasised in most of the previous theoretical
papers dealing with this problem.
The calculations presented in this paper do not account for relativistic efîects,
However using the relativistic version (Luc-Koenig 1972) of the central-field method
developed by Klapisch (1971) we have checked that relativistic effects are small.
Modifications of cross section values are generally weaker than differences between
the results obtained with diflerent non-relativistic central potentials.
In conclusion, although the overaIl trends of photoionisation cross sections do not
depend on the choice of the potential, additional experimental data are highly desirable
to test the accurac:y of our calculations, Results on partial photoionisation cross sections
and measurements on the spin polarisation and on the angular distribution of the
ejected photoelectron are worthwbile since they provide a much more stringent test
of the wavefunction than the total cross section.
4. Quantum defect theory analysis of trends in the ionisation of exdted states of
alkaH atoms
The results obtained in Rb and Sr+. in addition to those previously obtained in light
alkali atoms (Aymar et al 1976) or in Cs (Marr and Creek 1968, Weisheit 1972b.
Moskvin 1963, Msezane and Manson 1975. Lahiri and Manson 1982) give the oppor-
tunity to discuss the existence of minima in photoionisation cross section curves. The
quantum defect theory is very weil suited to this purpose (Burgess and Seaton 1960.
Peach 1967).
The contribution to the dipole matrix elements comes almost entirely from the
large-r region where the excited electron moves primarily in the hydrogenic Coulomb
field due to the core. The additional non-Coulomb forces which prevail within the
core modify the radial wavefunctions in the external region simply by shifting their
nodes. Both bound and continuum orbitais are contracted and the relative shift of the
two orbitais with respect to each other is responsible for the non-hydrogenic character
of photoionisation from excited states. The phaseshift of a bound orbital ni is measured
by 1TJJ.", where JJ.", is the quantum defect of the ni state. The phaseshift of the continuum
orbital will be denoted 8,.(s '). The quantum defect brings out an oscillatory dependence
of radial matrix elements R"l.l'(e') on JJ.", and 8,.(e') such as
.
cos 1Tâ"f.,.(e')
with
âlll.,.(e') =-p.", + 8,.(e')/ 1T+ XII'(n, s")
(11)
where the empirical parameter X is a slowly increasing Iunction of n and e' (Peach
1967). The occurrence of zeros in the R 1Il.I' (s') matrix elements are related to half
integer values of â"I.I.(e').
Near the threshold, an approximate value of âIll.I·(e') can be obtained by using for
the various quantities involved in equation (11) their limits for n = 00 and e' = O. One
Photoionisation cross sections of excited alkali atoms
1003
obtains
A""".(e') =- AIJ.". + Xu,(O)
(12)
where the asymptotic value X(O) of the X function can be extracted from the table of
Peach (1967). AlJ.u'" IJ.,' -IJ., represents the quantum defect difference for large n
which can be deduced from the effective quantum numbers tabulated by Lindgard and
Nielson (1977). The AlJ.u' values are compiled in table 2 for each ni ~ e' l' transition
of neutral alkali atoms and Sr". In the same table the shape type of each O':.,.,,(e')
cross section curve is given. For a given nl ~ e' l' transition the shape of the cross
section curve appears to be correlated to AIJ.Il"
A critical quantum deïect difterence AIJ.~' for the zero to occur can be defined by
the relation:
AIJ.~' +XU'(O)" =0.5.
(13)
The AIJ.~' values compiled in the Iast column of table 2 describe accurately the
occurrence of minima in the photoionisation cross section of excited states of alkali
atoms and Sr" and the evolution of non-hydrogenic behaviour along a given series.
The shape types of the partial cross section eurve O'~I," (s') expected for different values
of AIJ.". are indicated in table 3. If IAIJ.".I (mad 1) is far from IAIJ.~rl (mad 1) no change
of shape occurs aJong the series as n increases and the number k of zeros is detennined
by the _inequalities:
IAIJ.~·I + k -1 < 141J.".1< IAIJ.~·1 + le.
For low-lying levels, quantum defects IJ.", cao differ from the limiting value IJ., for
Table%. For a given III .. sr transition. we compiled the à~~. critical value deduced from
the quantum defect theory as weil as the asymptotic quantum defect difterence A.~U' and
the shape type of cr~I.I'(B') cross section eurve for each eJement.
Elements
Transition
Li
Na
K
Rb
Sr-
Cs
A.~?r
IIs"ap
-0.26
-0.49
-0.47
-0.49
-0.39
-0.50
-0.37
(b)
(c)
(c)
(c)
(b) "Ci 12
(c) 61.7s
(c) "-'13
0.26
0.49
0.47
0.49
0.39
0.50
0.71
(a)
(a)
(a)
(a)
(a)
(a)6p
"p"sd
-0.05
-0.84
-1.44
-1.30
-0.86
-1.10
(a)
(c)
(d) 11--9
(c)
(c)
(c) 6p
-0.42
(e) 11-' 10
0.05
0.84
1.44
1.30
0.86
1.10
(a)
(b) 11--3
(c)
(c)
(b)"Ci4
(c) Sei,9d
0.75
(c) ,,-'4
(c) ,,-.5
"d" et
0
-0.01
-0.26
-1.32
-1.39
-2.43
(a)
(a)
(a)
(c)
(c)
(e) Set
-0.48
(J)9d
0
0.01
0.26
1.32
1.39
2.43
(ca)
(a)
(a)
(c)
(c)
0.78
1004
M Aymar. 0 Robawc and S Wane
Table 3. Shapes of O'~I.I' (e') cross section curves according to l1"'rr values.
o
----------+-----+-----..,..----- 111",..".1
no zero
1 zero
2 zeros
3 zeros
(a) (b)
(c) (d)
(e)
(f)
large ft. Therefore when one bas
1~1J.1I'1 =0 I~IJ.?t·1 + k - 1
the critical value for k zeros is only reached for highly excited states and a change of
shape in the photoionisation curves occurs for a given series as n increases (see
table 2).
These remarks about the critical value for the zeros to occur generalise similar
results previously obtained by Msezane and Manson (1975, 1982) and Lahiri and
Manson (1982) for sorne particular nl-. el' transitions. This analysis of non-hydrogenic
behaviour of photoionisation from excited states in terms of the quantum defect theory
also explains why the non-hydrogenic traits do not disappear for highly excited states;
in fact the position of the zeros is almost stationary when IJ."I and Xl/'(n. e') reach their
asymptotic values.
The evolution of the non-hydrogenic behaviour of the cross section from Rb and
Sr+ can also be analysed in terms of the quantum defect theory. The isoelectronic
variation of quantum defects for a given nl series strongly depends on the 1 value
(Edlén 1964). For small 1 the quantum defect IJ.rtl mainly due to penetration of the
ni orbital in the core, decreases as Z increases. Core polarisation effects are responsible
for most of the quantum defect for large l; for these non-penetrating orbitaIs
Edlén (1964) showed that IJ."I first increases with Z, then passes through a maximum
and ultimately decreases. Similar behaviour is also expected for intermediate 1values.
These remarks explain why, in the beginning of the Rb isoelectronic sequence tJ.lJ.sp
and A.lJ.pd decrease with Z while tJ.lJ.df and A.lJ.f& increase. Therefore the minimum
occurring in the ulIs.p(e), uIIP.d(e) and ulld.p(e) cross section curves of Rb moves for
Sr+ toward threshold (ns states with n ~ 13, np states, nd states with n SIl5) or even
into the discrète spectrum (ns states with n =El 12; 4d state). This evolution follows the
general trend predieted for the isoelectronic variation of the photoionisation of ground
states involving s or p orbitaIs: light alkali atoms (McGinn 1970, Burgess and Seaton
1960, Black et al 1972); photoionisation relative to the 2p or 3p subshell (Combet
Famoux and Lamoureux 1976). On the contrary, non-hydrogenic behaviour of partial
cross sections U~d.f(E') and U~f.d(e') are almost identical in Rb and Sr+.
S. Conclusion
This work on the non-hydrogenic behaviour of photoionisation of excited states of Rb
and Sr+ extends the previous studies performed in light alkali atoms (Aymar et al
1976) orin Cs (Msezaneand Manson 1975, Lahiri and Manson 1982). The central-field
approximation allowed one to easily calculate Many cross section values and therefore
provided the data required for an extensive analysis of the systematics of excited-alkali-
atom photoionisation. Central-field calculations are expected to be more reliable than
those provided by quantum defeet theory (Burgess and Seaton 1960). However, this
Photoionisation cross sections of exciteâ alkali atoms
1005
last method ls much more appropriate for interpreting the non-hydrogenic behaviour
and the systematics of partial photoionisation cross sections. In particular the number
of minima occurring in partial photoionisation cross section curves has been related
to the difterence of quantum defects of both channels involved in the ionisation process.
Quantum defect thcory allows one to understand the 'evolution along a given Rydberg
series, the isoelectronic variation from Rb to Sr" and the trends along the sequence
of alkali atoms,
Admowledpae."
The authors wish to express thcir gratitude to M Klapsich for suggesting the use of the
phase-amplitude description of continuum wavefunctions. They wish also to thank
A Bar-Shalom for aecess to the corresponding unpublished program.
Appe.db:
Two difterent numerica1 procedures are used to compute radial matrix elements.
A.l
The discrete Pnl(r) and continuum P.,.(r) radial wavefunctions are calculated by solving
the differential equation (3) by using the Numerov method (Froese Fischer 1963) with
the same r-scaled linear mesh (Aymar et al 1976). Continuum orbitaIs are obtained
by outward integration of equation (3) and then normalised by using the Strômgren
procedure (Stewart 1967). The radial matrix element is then evaluated by straightfor-
ward numerica1 quadrature.
The integration range of the P.1·(r) wavefunction, determined by the extension of
the P",(r) bound orbital increases with n. For large values of ra, the mesh suited to
the integration of Pnl(r) is not adapted to the description of the oscillatory behaviour
of P.,,(r). Therefore, when photoionisation of highly excited states (n > 10) is concer-
ned, a different procedure is used to determine the continuum wavefunctions.
A.2
Except near r = 0 for the s electron andnear the classical 'tuming point' due to the
centrifugaI potential barrier for 1~ 0 electrons, Pd·(r) can he expressed in terms of a
phase function ~(r) and an amplitude function y(r) (Fano et al 1976 and references
therein) as
P.,,(r) == y(r)J; sin ~(r)
r> ro.
(A.l)
With the logarithmic variable x =lg r used by Froese Fischer (1963), substitution of
equation (A.l) in the SchrOdinger equation (3) Ieads to the system
y(x) + Wy(x) -1/ y3(X) =0
(A.2)
iP(x) =1/ y2(X)
(A.3)
1006
M Aymar, 0 Robaux and S Wane
with
(A.4)
The system (A.2), (A.3) is solved following the algorithms proposed by Bar Shalom
(1983). The equation (A.3) is solved for ,SiI='o by inward integration. Values of y at
starting points corresponding to large r are computed self consistently with a first
approximation of y obtained by assuming y= O. For large values of " in the range
where Wis important, standard integration methods (prediction-correction procedure)
fail and sophisticated iterative procedures are used. The phase function is then obtained
by solving equation (A.3), for '~'o by a simple composite method (Legras 1963).
One obtains in this way a phase function c,o(') + c,oowhich depends on a parameter c,oo.
Equation (A.l) does not hold for r 'E: '0 and in this region the Schrôdinger equation
(3) is solved by outward integration by the use of the Numerov method. Starting from
an arbitrary slope at the origin, we obtain an un-normalised solution
YI = AP.,,(x).
(A.5)
The required nonnalised PIlI,( , ) wavefunction is then evaluated by the determination
of the constant phaseshift c,oo and the amplitude factor A provided by matching the
inward and outward solutions. Radial matrix elementx are evaluated by writing
RPlI,I,(e) = rJt1 PII/(x)Q'(x)P.,,(x) dx+feCl PII/(x)Q'(x)y(x)J;sin c,o(x) d:c.
(A.6)
Jo
Jtl
The Xl value corresponds to the first node of the continuum wavefunctions. The first
integraJ is evaluated by Simpson quadrature. The second integral 12 is expressed in
terms of a new variable u = c,o(x) as follows:
(A.7)
f(j+l)ft'
12=~.
Z(u)sinudu.
1
1ft'
The integration over each j'TT- (j + 1)'TT interval is evaluated using a Gaussian procedure
with a sinusoidal weight function (Legras 1963).
The bound and continuum wavefunctions being found using two different meshes,
one uses cubic spline interpolation procedure (Ahlberg 1967) to evaluate the integrand
of equations (A.6) and (A.7) at relevant points.
Refereaces
Ahlberg J H, Wilson E N and Walsh J L 1967 The T'Mory of SpliMs and their Applications; Mathematics
in Science and Engineering vol 38 (New York: Academie)
Ambartzumian R V, Furzikov NP, Letokhov V Sand Puretsky A A 1976 AppL Phys. 9 335-7
Aymar M 1978 J. Phys. B: AL Mol Phys. 11 1413-23
Aymar M and Cranée M 1980 J. Phys. B: AL MoL Phys. 13 2527-44
Aymar M, Luc-Koenig E and Combet-Famoux F 1976 J. Phys. B: At. Mot. Phys. 9 1279-91
Bar Sbalom A 1983 T'Msù University of Jérusalem
Bethe H A and Salpcter E E 1957 Quantum Mechanics of One and Two Electron Atoms (Berlin: Springer)
Black J H, Weisheit J C and Allan E 1972 Amon. 1. 177 567-72
Burgess A and Seaton M J 1960 Mon. NOL R. Astron. Soc. 120 121-51
Cheret M, Barbier L, Lindinger Wand Deloche R 1982a 1. Phys. B: AL MoL Phyl. 15 3463-71
-
1982b Cltem. Phyl. Urt. 88229 .
Cbichkov B N and Shevelko V P 1981 Phys. Scr. %3 1055-65
Combet Famoux F and Lamoureux M 1976 J. Phys. B: AL MoL Phys. 9897-909
Photoionisation cross sections of excited alkali atoms
1007
Crance M and Aymar M 19801. Phys. B: AL MoL Phys. 13 4129-42
Devdariani A Z and Klyucharev A N 1977 Opl. Spelctrosk. 42 694-5
EdI~n B 1964 Hœulbuds dt, Physile Spectroscopy vol 27 (Berlin: Springer) pp 80-220
Fano U and Cooper J W 1968 Rft). Mod. Plays. 40 441-507
Fano U, Theodosiou C E and Oehmer J L 1976 Rev. Mod. Plays. 48 49-68
Froese Fischer C 1963 Cali. 1. Plays. 41 1895-910
Hameed S, Herzenberg A and James M G 1968 1. PhYs. B: At. MoL Phys. 1 822-30
Hofsaess 0 1977 Z. Phys. A 281 1-13
Klapisch M 1971 Comput. Phys. CommulL 2 239-60
Klyudwev A 1 and Sepman V Yu 1975 Opl. Speetrosc. 38 712-3
Lahiri J and Manson ST 1982 Phys. Re»: Lm. 48 614-6
Legras J 1963 Prkis d'Analyse Numérique (Paris: Dunod)
Lindprd A and Nielsen S E 1977 AL Data NucL Data Tables 19 534-633
Luc-Koenig E 1972 Physica 62 393-408
McGinn G 1970 1. CMm. Phys. 53 3635-40
-
1972 J. CUm. Plays. 58 772-6
Marr G V and Creek 0 M 1968 hoc. R. Soc. A 304 233-44
Moskvin Yu V 1963 Opl. Sp«:trosc. 15 316-8
Msczane A and Manson S T 1975 Plays. Rev. Lm. 35 364-6
-1982 Phys. Re»: un. 48 473-5
Peach G 1967 Mmao. R. A.stl'OIL Soc. 1113-27
Shevelko V P and Vinogradov A V 1978 Phys. Sc,. 19275-82
Stewart A L 1967 Adv. At. MoL Plays. ji-51
Weisheit J C 1972a Plays. Rev. A 5 1621-30
-
1972b 1. OuaM Speetrosc. Radùzt. Transler 12 1241-8
ANNEXE
II
J Phys. B: At. Mol. Phys. 18 (1985) 3881-3893. Printed in Great Britain
Radiative recombinatioD in rubidium
S Wane
Laboratoire Aimé Cotton. CNRS II. Campus d'Orsay, Bâtiment SOS. 91405 Orsay Cedex,
France
Received 1 May 1985
AIIItract. The rate coefficients for radiative recombination of Rb into individual ground
and excited III states (II ~ 20, 1~ 10), summed over 1< Il (II "!li 10) and over all states. have
beeD computed for the electron temperature range SOO~ T"!li6000 K. Using the principle
of detailed balance, photoionisation cross sections of Rb calculated in the framework of
a sinate.electron model have been used.
The evolution with Il and 1 for given T, with T for given Il and various 1 and with T
of the total radiative recombination coefficient is analysed. The significant non-bydrogenic
features for recombination are outlined. Comparisons are made with the results of the
hydrogenic and Kramers' models and with other results available for alkali atoms.
1. Introduction
Photoionisation from excited atoms or ions and radiative recombination processes
are of primary importance in radiative transfers involved in the laboratory, in astre-
physics and in controlled thermonuclear plasmas. Studies of the recombination spectra,
ionisation and recombination equilibrium, thermal balance, radiative losses and
emission plasma diagnostics ail require the knowledge of recombination cross sections
and radiative recombination coefficients.
Many of the experiments involving ionisation from excited states and recombination
processes deal with alkali atoms. Earlier experimental determinations of photoionisa-
tion cross sections from excited states were derived from studies of radiative recombina-
tion in plasmas; results were obtained by Mohler (1933), Agnew and Summers (1965)
and Rothe (1969, 1971). However experimental results for radiative recombination
coefficients are very scarce.
On the theoretical side, a thorough study of photoionisation cross sections for
excited states of Rb has recently been carried out by Aymar et al (1984). Systematic
trends of non-hydrogenic behaviour of photoionisation cross sections for exeited alkali
atoms have been analysed
.
Previous calculations of radiative recombination coefficients for one-eleetron atomic
systems mainly deal with hydrogen H and hydrogenic ions (Seaton 1959, Burgess 1964).
A few theoretical results have also been obtained for Cs (Norcross and Stone 1966,
Weisheit 1972), Li (Caves and Dalgamo 1972), and the alkali atoms Li to Cs (Moskvin
1963). It is highly desirable to extend these results and to study the systematics of
radiative recombination for alkali atoms.
In this work we present detailed numerical results for the radiative recombination
rate coefficients for Rb atoms in the electron temperature range 5oo=- T=-6000 K. The
required photoionisation cross sections are calculated in the framework of a single-
eleetron model by the method already employed by Aymar et al (1984).
0022-3700/85/193881 + 13$02.25 © 1985 The Institute of Physics
3881
3882
S ~ane
The method of computation for the recombination rate coefficients is outlined in
§ 2. The results are given and discussed in § 3 with emphasis on the non-hydrogenic
features.
Comparisons with the results of the hydrogenic and Kramers' models and with
other results available "for alkali atoms are made.
2. Tbeory and method of calculation
We give in this section the basic formulae used for the computation of the radiative
recombination coefficients, and we recall the results of the hydrogenic and Kramers'
models.
2.1. Basic formulae
In the radiative recombination process of one-electron atoms, an ion X-+ in initial state
ISO combines with a free incident electron to produce a neutral atom X in a specifie
final state nl 2 L while a photon of frequency Il is ernitted.
X+eSo) +e- ~ X(n1 2L) + hv.
(l)
This capture process in which the incident eleetron undergoes a free-bound transition
is the inverse of the photoionisation process. The cross sections, u;/( v) and u:/( Il),
respeetively, are related through the principle of detailed balance (Massey et al 1969)
by
c
th»] C)2
p
"
0'1I/(v)=2(2/+l)
2
ull/(v)
(2)
p
where v is the relative velo city of the incident electron, p is its momentum and c is
the velocity of light.
The corresponding recombination rate coefficient is given by the velocity (or
thermal) average
a'd(T)=(vu~(v»=Log vO';/(v)f(v)dv
(3)
where
m )3/2
(- mv2)
f( v) =4,,",2 ( ï;kT
exp
2kT
is the Maxwellian distribution function of electron velocities, m is the electron mass,
k is the Boltzman constant and T is the electronic temperature.
Using equation (2), alll( T) can be written as an integral over the photoionisation
cross section (Bates and Dalgamo 1962, Barfield 1980):
l)er
a",(T) =2(2/+
exp ( ; ; ) c-'(mkT)-'" [
(hv)'<T~(v) exp( ~~)d(hv).
(4)
EIII is the binding energy of the captured electron which satisfies
hv = e+ EIII
(5)
e being the electron kinetic energy.
Radiative reeombination in rubidium
3883
We then obtain
an/(T)=(3286.3402)2(21+1)(kT)-3/21
co (e+e",)2u:,(e)exp(~;) de.
(6)
AlI the energies are expressed in Ryd units, u;,( e) and u:,( s ) are in cm2 and a",( T)
is expressed in cm] s-1.
The radiative recombination rate coefficient is then summed over 1 as
11-1
ail ( T) = L a",( T).
(7)
'-0
The total recombination rate coefficient is
CICl
a,( T) = r a.. ( T)
(8)
11-"0
where no corresponds to the lowest unfilled shell or subshell of the recombined atom.
It is of interest to calculate the radiative recombination rate coefficients a",( T) and
a,,( T) for recombination spectra of atomic ions (Burgess 1958, Seaton 1959, Pengelly
1964) and the total recombination rate coefficient al for ionisation equilibrium of
atomic ions (Jordan 1969, 1970).
The required photoionisation cross sections u:,( e) for Rb are calculated by the
method already employed by Aymar et al (1984). In the framework of a non-relativistic
single-electron model a central potential is used and core polarisation efîects are
accounted for. Only the contribution of ejection of the outer ni electron to u:,( e) is
considered in this work. The validity of the calculation of u:,( e) is therefore confined
to the energy range close to the threshold. In this'energy range autoionisation efîects
can be neglected; in effect autoionised lines corresponding to the excitation of the 4p
inner-shell electron have been observed for electron energies larger than 0.8 Ryd above
the threshold (Bearden and Burr 1967).
The radiative recombination coefficient a",( T) is cornputed from equation (6).
The integrand of equation (6) decreases rapidly as e increases: successive increasing
intervals of integration are used until their contributions become negligible. The
corresponding efficient electron energy range increases with temperature T. For low
T this energy range is confined near the threshold. AIl calculations are restricted to
the temperature range 500 t!ii T ~ 6000 K for which the efficient electron energy range
is located within 0.4 Ryd above the threshold.
2.2. Results of the hydrogenic and Kramers' models
For the sake of comparison with radiative recombination rate coefficients for Rb atoms
we recall the results of the hydrogenic and Kramers' models for the rate coefficients.
For hydrogenic ions aIl the radiative recombination rate coefficients May be calcu-
lated exactly since analytic expressions for the photoionisation cross section u:,( e)
are known (Gordon 1929). Accurate results for all,(T) and low n values have been
obtained by Burgess (1964) for hydrogenic ions and by Boardman (1964) for the
hydrogen atom H using exact transition matrix elements in u:,( e).
However, with increasing n the analytic expressions for u:,( e) become complicated
and difficult to evaluate directly. One May then use an approximation to obfain simple
expressions for the radiative rate coefficients. The photoionisation cross section of the
3884
S ~ane
shell n which is defined as
O'~(E) =~ L(21+ l)O'~/(E)
n 1
is approximated in the Kramer's model by the semiclassical expression O'~( E) (Kramers
1923, Sobelman 1972)
Kr
641faa~ Z4
1
0',. (E)= 3v"3 -;;s (E+E,.)3
(9)
where a is the fine-structure constant, ao is the Bohr radius, Z is the charge of the
hydrogenic ion and E,. = Z 2Ry/n 2 is the binding energy of the shell n. Equation (9)
gives good results close to the threshold for any n, but they become less satisfactory
with increasing E. With equation (9) one deduces
14
3
Z 2R)3/2
(Z2 RY)
(Z2 RY)
(10)
a~(Z, T) =(5.197 X 10- cm S-l)Z ( n2k;
exp n2kT El n2kT
where E (x ) = I: exp( -iïr:' dt.
1
Taking directly O'~,( B) = O'~( E) one obtains
Burbidge et al (1963) have performed the summation over n and have given a rather
simple expression for the temperature dependence of the total rate coefficient
Z 2R )1/2
0':V(z,
Y
T) = (5.197 X10-14 cm? S-l)Z ( kT
x [0.8675 +! ln ( Z:;Y) + 0.0833 ( Z:;Y) ]
(11)
for th-e range T / Z 2 :Et 3 X 10' K..
Deviations from exact values of radiative rate coefficients may occur for Kramers'
results. They are particular important for a~( T) and increase with temperature. In
fact as T increases the efficient electron energy range increases and therefore Kramers'
approximation becomes less justified. An important improvement is obtained by
introducing the weil known Kramers' Gaunt factor s, defined as
O'~(E )
g,.(E)=
Kr( )~1
0',. E
which leads to
Z 2Ry)3/2
(Z2 RY)
a,.(Z, T) = (5.197 X 10- 14 cnr' S-l)Z ( n
Sri n
(12)
2kT
2kT
where
Z 2RY)
fcc
(Z2 R
)
Sri ( U
=
0
exp - n2k; u (1 + U)-l g,.(U) du
with u = e/ e,.. With the first three terms in the asymptotic expression of g,. (u) Seaton
(1959) has obtained rate coefficients a,.(Z, T) calculated with deviations from the exact
values which do not exceed 2% for T / Z2 ~ 104 K. The total radiative recombination
Radiative recombination in rubidium
3885
rate coefficient, expressed by Seaton (1959) as
a,(Z, T) = (5.197X10-14 cm)S-I)Z(Z::Y) 1/2
x [0.4288+! ln( Z::Y) +0.4638 (Z::Y) -1/3]
(13)
with deviations from the exact values of less than 0.5% for T/ Z2=s;; 10' K., gives a better
approximation and dependence on T.
Bates and Dalgamo (1962) have conveniently summarised Seaton '5 work and quoted
a ~(T) and a ~(T) for H at different temperatures.
3. Resalts
Detailed results for coefficients of Rb a",( T), a,,( T) and a t( T) have been obtained in
the temperature range 500SSii T lSiO 6000 K and compared with the results of the hydro-
genie and K.ramers' models corresponding to the charge Z = 1 (charge of the ion Rb+
before recombination).
3.1. Results for a",( T) with 11 Et 20, 1=s;; 10
3.1.1. Evolution of a", with n and l for T jixed. The evolution of a", with 11 at a fixed
and rather low temperature T = 500 K is shown in figure 1 for various 1 values and
(QI
H
(bl Rb
d
i
- 10.,4
10., 4
.k
-,
'h
'"
;:g
...li
'f
...-ë:
CI
10.1..
10.1..
d
P
10.16
10-16
s
n
n
10-1'
10.11
4
B
12
16
20
4
8
12
16
20
n
FIpre 1. Radiative recombination rate coefficients a", (in units of cm) S-I) plotted against
the principal quantum number,. for 1- 0-7 (s, p, d, ... ,t), 100n) al temperature T - SOO K
for (a) H and (b) Rb.
3886
S ~ane
compared with a~/. The coefficients a"1 and a~ have the same evolution with n for
any given 1;6 0 and the relative order of a"1 or a ~ for any given n depends upon n
as seen in figure 1.
When T is low the efficient electron energy range for the calculation of a"1 and
a ~I is confined near to the threshold for any n and L Only values of 0'"/( s ) and O'~( s )
in this vicinity are to be considered.
Firstly for H and given 1the coefficients a ~ decrease monotonically with increasing
n for I:s;; 3 but present a maximum for 1>3. This is related to the evolution of O'~( e)
with e which depends on both the n and 1 values. For given 1:Ei 3 and increasing
values of e, O'~( s ) decreases more rapidly the higher n is, as shown in figure 2 for
1:;: 1 curves. This is not the case for given 1>3, as shown in figure 2 for 1:;: 6 curves;
the increase of a ~ for low n is then related to the increase with n of O'~(s ) near the
threshold.
Secondly for any given n, a ~ increases first with increasing l; reaches a maximum
and then decreases, The increase of a~ with 1 follows that of the statistical weight
factor 2(2/+ 1) and that of the threshold photoionisation cross section O'~(O) which
also increases with 1up to a maximum. The decrease of a ~ for large 1values is related
to that of O'~(0) and mainly to the fact that the higher 1is, the faster O'~( s ) decreases
with e (see figure 2). The relative order of a~ depends upon n because the I~ value
for which a~1 reaches a maximum depends upon n.
As far as Rb is concerned, for any n, a"1 is close to a ~I for 1> 3 whereas it is quite
different for 1=si 2, as may be expected. In faet the photoionisation cross sections of
Rb present non-hydrogenic characters only for 1=si 2 (Aymar et al 1984).
The occurrence of the Cooper minimum for 0'ns(s ) leads to 0'ns( e ) « O'~s( s ) and
consequently to a"S < a ~s. This minimum for O'ss( s ) is closer to the threshold than
0.02
0.04
0.06
0.08
0.10
c (Ryd 1
Figure 2. Photoionisation cross sections (in units of Mb, 1 Mb= 10- 18 cm2) C7 (e ) ( - )
n p
and C7ni( e ) (- -) plotted against the energy of the photcelectron (in units of Ryd).
Radiative recombination in rubidium
3887
those of the other O"n.( E) with n > 5. This explains the maximum present in the evolution
of the coefficients ans with n which does not exist for H. For p and d states the
differences between am and a ~ depend upon n. For high n(:li: 20) an' < a ~ because
O"n'(O)« O"~(O), but for low n(:lI: 5) we have instead an' > a~ and the relative order of
an' is completely changed from that of the corresponding a~. Large values are obtained
for a np and and owing to two factors. Firstly the decrease of O"n'( E) for 1Si:2 with E
is slower than in the case of hydrogen. The second and important factor is that the
large values of the ionisation potentials En' for p and d states of Rb give a higher weight
to the factor (E+En,)2 occurring in equation (6).
The evolution of ara' with n and 1 has been discussed in detail for T = 500 K;
however similar behaviour is obtained for any temperature.
3.1.2. Evolution ofara' with T. For given n and l; a n,(T) for Rb decreases monotonically
with increasing temperature, as is apparent from equation (6) and figure 3, which
shows the evolution of as,( T) with T for various 1 values. The important fact here is
that the efficient electron energy range increases with T. The coefficients as, with 1:Ji 0
decrease faster with T the higher 1 is, due to the evolution of O"s,( E) with E and L
Thèse results are similar for any given n. The relative importance of an' correspond.
ing to lower 1:Ji 0 increases with temperature. The relative order of an' for given n
th us changes with T. Values of ara' ( T) are given in table 1.
Let us note that a n,(T) decreases with T slower than a ~,( T) because O"n'( E) decreases
with E slower than O"~,( E ).
3.2. Results for an ( T)
The radiative recombination an (T) on the shell n has been calculated (equation (7»,
for n Si: 10 and n = 15 and compared with a~( T).
10· n
fg~
d'
10.110 h
i ;;
d
P
~f
-p
~
'g
tII
k
...
-. h
!5 10.15
5
0;
tI
10. 16
k
S
500
2000
4000
6000
T(KI
Figure 3. Radiative recombination rate Coefficients a8l( T) for 1=0-7 (5. P. d•...• le) (in
units of cml
1)
5-
plotted asainst the temperature.
w
00
00
00
C'l
~
Table 1. Values of a",( T) (in units of 10- 14 cm) S-I), 1=0-3 (s, p, d, 0 and various ft values at temperatures T =500, 2500 and 5000 K. The numbers in parenthèses
::s
denote the powers of ten,
~
ft
T(K)
1
4
5
6
8
10
12
15
18
20
500
s
7.95 (-2)
12.4(-2)
6.27 (-2)
3.45 (-2)
2.0 (-2)
1.1 (-2)
7.5(-3)
6.2 (-3)
2500
2.30 (-2)
4.02 (-2)
1.91 (-2)
9.60 (-3)
5.3(-3)
2.7 (-3)
1.6(-3)
1.2 (-3)
5000
1.15(-2)
2.07 (-2)
9.60(-)
4.50(-3)
2.5(-3)
1.2 (-3)
7.0 (-4)
5.0 (-4)
500
P
17.02
4.219
8.277 (-1)
2.985 (-1)
1.437 (-1)
6.65 (-2)
3.97 (-2)
3.13 (-2)
2500
8.142
2.138
4.489 (-1)
1.667 (-1)
8.030 (-2)
3.53 (-2)
1.95(-2)
1.40 (-2)
5000
6.103
1.677
3.672 (-1)
1.381 (-1)
6.640(-2)
2.88(-2)
1.39(-2)
9.90 (-3)
500
d
33.72
13.90
6.198
1.955
9.408 (-1)
4.376 (-1)
2.01 (-1)
1.12 (-1)
7.99(-2)
2500
14.42
6.195
2.873
9.428 (-1)
4.510(-1)
2.134 (-1)
1.00 ( -1)
5.48(-2)
3.88 (-2)
5000
9.660
4.306
2.046
6.790(-1)
3.154(-1)
1.582 (-1)
7.45( -2)
4.09 (-2)
2.66 (-2)
500
f
6.309
5.676
4.219
2.300
1.331
9.029 (-1)
4.54 (-1)
2.77 (-1)
2.26(-1)
2500
2.194
1.983
1.476
7.909 (-1)
4.546 (-1)
2.915 (-1)
1.57 (-1)
9.04(-2)
6.45(-2)
5000
1.233
1.121
8.347 (-1)
4.454 (-1)
2.526 (-1)
1.602 (-1)
8.71 (-2)
4.99 (-2)
3.21 (-2)
Radiative recombination in rubidium
3889
For any given n and T values, a"l( T) presents a maximum in its evolution with 1.
Then the ratio X,,, (T) = a",( T)/ a,,( T) also exhibits a maximum xM(n, T) for IM(n, T)
when 1 increases as shown in figure 4 for asti as at T = 500 and 5000 K. lM increases
whereas XM decreases with n at given T and lM de creases whereas XM increases with
T for given n. This means that the contribution to a" of a"l corresponding to low 1
values (non-hydrogenic character) is larger for low-n values and high temperatures.
This is clearly shown in figure 5 which outlines the comparison of a,,( T) with a~( T)
and the evolution of a,,( T)/ a~( T) with T. a,,( T)/ a~( T) increases with T for given
n because a,,( T) decreases with T slower than a,,( T), as does a"l( T) as compared
with a~(T).
0.4
0.3
"
1 \\
1 \\
..
1
\\
t:l
1
\\
-
1
\\
iD
I:S
0.2
1I~"""'"
1
"' \\
~
il
\\ '0
\\
1
\\
1
\\
0.1
1
\\
/1
\\~
\\
1
\\''-
0
2
4
6
B
1
Fipre 4. The ratio as'! as plotted against the orbital quantum number 1for T =Soo ( - )
SOOO K(- - -).
From our results for low n a,,( T) ~ a~( T), the non-hydrogenic charaeters are
enhanced with increasing T, and a" (T) may be 3-4 times larger th an a ~(T). However,
as n increases the relative importance of the non-hydrogenic contributions to a"
corresponding to alll with 1~ 2 decreases and for n ~ 10 we have approximately
a,,(T) =- a~( T).
a" (T) with 11 ~ 10 and a 1'( T) are given in table 2. For low n the evolution of
a,,( T) with T and n is not weil described by K..ramers and Seaton's formulae (equations
(10) and (12), Z::; l ). We have used a least-squares procedure to fit our results for
a" (T) and we have obtained empirically three-term parametric expressions which
agree with the computed values to better than 5%.
The evolution with T for given n, and with n at given T, is obtained from
_
(
b
ln T)
a" ( T) =T 1/2 a + T + c-:;-
(14)
(15)
where a" is expressed in units of 10-14 cm) S-I and a, b, C, a', b', c'are constant
coefficients. As an example, for n = 5 we have a =8.233 x 1<r, b =1.643 x 10' and
3890
S ~ane
3.5
3.0
2.5
1-
:"';, 2.0
ts
:::.
1-
~ 1.5
ts
1.0
0.5
oL....-.,--..--_.,--__-.,---..---,..-
500
2000
4000
6000
T (KI
Figure 5. The ratio a" (T)/ a ~(T) ploned against the temperature for n = 5, 6, 8, 10 and 15.
s
Table 2. Values of
H•S(
r
a4d( T), a4f( T), a,,( T) n ~ 10 a 15( T), a
T) and at • ( T) (in
t ( T), a t
units of 10- 14 cm) S-I) for various values of T.
T(K)
500
1000
2000
3000
4000
5000
6000
a 4d
33.72
23.59
16.30
13.01
11.03
9.660
8.642
a 4r
6.309
4.162
2.594
1.901
1.499
1.233
1.043
a5
39.20
27.46
19.18
15.54
13.38
11.91
10.83
a.
18.72
12.84
8.701
6.900
5.848
5.141
4.625
a7
13.40
9.200
5.800
4.400
3.700
3.100
3.000
as
10.00
6.467
4.037
3.029
2.464
2.097
1.837
Q9
8.400
5.200
3.200
2.400
1.900
1.600
1.400
a10
7.089
4.418
2.604
1.872
1.473
1.220
1.044
a l5
3.636
2.133
1.149
0.781
0.590
0.472
0.396
a
224.4
138.8
85.35
65.88
52.07
44.54
37.78
t
ar.s
165.8
96.40
54.64
39.22
29.46
24.50
20.42
a Kt.S
172.9
100.9
56.98
40.92
30.97
25.22
21.26
t
c =3.078 X 104• For T = 5000 K we have a' =6.256 x 103, b' =1.684 x 103 and c' =
-8.825 X 103•
3.3. Results for a l ( T)
It is usual ta split the total radiative recombination coefficient al for non-hydrogenic
ions and atoms into two parts for its calculation (Aldrovandi and Pequignot 1973).
Radiative recombination in rubidium
3891
One part corresponds to the non-hydrogenic contribution and the other one to the
hydrogenic contribution. As ail =0: a~ for n;;;e: 10 we evaluate al from equation (8) as
9
CID
a l=a4d+ a4r+ L a + L a~
ll
11-5
11-10
with
a~ and att can be obtained from tables given by Bates and Dalgamo (1962). al(T)
calculated for the whole temperature range is given in table 2. The evolution of a t( T)
with T is not weil described by Kramers and Seaton's formulae (equations (11) and
(13), Z =1). We have fitted our results for a t( T) to better than 4% with the three-
parameter analytical formulae found empirically:
a ( T) = (5.197 X 10-14 cm' S-l) (:;) 1/2
l
x [1.1627+0.024(~) -0.0035(:;) In(~) J.
(16)
For comparison of al for Rb with the results of the hydrogenic and Kramers models,
a~ and a:cr must be modified to account for the filled shells and subshells of Rb+.
We have calculated corresponding a~'s and a:cr·s. The coefficients a4d, a4r, al, a~'s
and a:V's are given in table 2.
Figure 6 shows al compared with the results of the hydrogenic and Kramers models.
a~'s and a:cr·s do not differ much, but al differs significantly from them. aJ a~
increases with increasing temperature as expeeted and May be as high as 2. Modelling
the total radiative recombination coefficient by the hydrogenic or Kramers one is not
always reliable.
24
20
";'
16
III
...B
-tS 8
4
oL....,,--.----,--~---r----...---
soo
2000
4000
6000
T (KI
Flpre 6. Total radiative recombination al(T) for Rb (in units of lO-u cm) 5-') plotted
against the temperature (c:urve A). Comparison with the results of the hydrogenic a~.5(T)
(c:urve B) and Kramers models a:,r.5(T) (c:urve C) are also prcsentec:l Results obtained
for a t ( T) of Li by Caves and Dalgamo (1972) are the same as ours for Rb (curve A).
3892
S ~ane
For Rb the radiative recombination coefficients on the lower subsheUs (4<:1, 40 and
shells (n = 5-9) are far from being hydrogenic and a detailed calculation using the
correct photoionisation cross sections is valuable. It would be useful to compare our
results with others obtained for Rb or other alkali atoms, Unfortunately only few
theoretical results have already been obtained for the radiative recombination
coefficients of sorne alkali atoms. Non-hydrogenic features of the radiative recombina-
tion coefficients alti into the lowest states of Cs (Norcross and Stone 1966) and Li
(Caves and Dalgamo 1972) have been outlined.
The total radiative recombination coefficient Clt has been given for Li by Caves and
Dalgamo (1972) who calculated the non-hydrogenic contribution for n =2, 3 by use
of a model potential and adopted hydrogenic values for" ;;,: 4. Their values coincide
practically with ours for Rb as shown in figure 6. This was previously noticed by
Moslcvin (1963) who used the quantum defeet method (Burgess and Seaton 1960) to
evaluate a for the alkali atoms Li-Cs. Precise values cannot, however, be derived for
t
a of Rb from Moskvin's curve and this prevents any comparison with other results.
t
4. Conclusion
This work on the non-hydrogenic behaviour of the radiative recombination coefficients
of Rb adds to the previous studies performed with alkali atoms (Moskvin 1963), Li
(Caves and Dalgamo 1972) and Cs (Norcross and Stone 1966, Weisheit 1972).
The non-hydrogenic features are significant for recombination in ail the "S, np and
nd Rydberg series even for large values of n and for the lowest sheUs (n =5-9). For
ni Rydberg series, however, with 1;;,: 4 and the higher shells (n;;,: 10), the radiative
recombination coefficients are close to the hydrogenic ones.
Il would be interesting to use our method of calculation for studying the systernatics
of radiative recombination of alkali atoms and alkali-like ions. It is expeeted that the
central field model which has been used gives more reliable results than those provided
by the quantum defect theory (Burgess and Seaton 1960) for that systematics.
Il will be also of interest to extend the temperature range and to study the role of
excitation of inner-shell electrons for recombination of alkali atoms and alkali-like
ions. Extension of the results obtained for one-eleetron systems to more complex
atoms and ions is another good challenge.
References
Agnew Land Summers C 1965 Proc. 7th. lnt: Conf. on P1Iysics of lonised Gases, Belgrade pp 574-80
AJdrovandi S M and Pequignot 0 1973 Astron. Astrophys. 15 137-40
Aymar M, Robaux 0 and Wane S 19841. P1Iys. B: AL MDL P1Iys. 17993-1007
Barfield W 0 19801. P1Iys. B: AL MDL Phys. 13931-7
Bates 0 Rand Dalgamo A 1962 Atomic and Molecular Processes ed D R Bates (New York: Academie)
ch 7
Bearden J A and Burr A F 1967 Rev. Mod. PItys. 39 125-42
Boardman W J 1964 Astrophys. 1. SuppL Series 9 185-92
Burbidge G R, Gould R J and Pottasch S R 1963 Asrrophys.1. 138 945-67
Burgess A 1958 Mon. Not. R. Astron. Soc. 118477-95
-
1964 Mon. Nol. R. Astron. Soc. 6fJ 1-20
Burgess A and SeatoD M J 1960 Mon. NOL R. Astron. Soc. 120 121-51
Caves TC and Dalgamo A 1972 1. Qwmt. Spearosc. Radial. Transfer 12 1539-52
Radiative recombtnation in rubidium
3893
Gordon W 1929 Ann. PItys., Lpz. 2 1031
Jordan C 1969 Mon. Not. R. Astron. Soc. 142501-21
- - 1970 Mon. Not. R. Astron. Soc. 148 17-23
Kramers H A 1923 PhiL Mag. 46 836
Massey H S W 1969 EIectronic and Ionie Impact phenomena vol II (Oxford: Clarendon) ch 14
Mohler F L 1933 1 Res. NBS 10771-80
Moskvin Yu V 1963 Opt. S~ctrosc. 15316-8
Norcross 0 W and Stone P M 1966 J. Qw;znt. Spectrosc. Radia: Transfer 6 277-90
Pengelly R M 1964 Mon. Not. R. Astran. Soc. ln 145-63
Rothe 0 E 1969 1 Qw;znt. Spectrosc. RadùJt. Transfer 9 49-62
- - 1911 J. QuanL Spectrosc. Radiat. Transfe, 11 355-65
Seaton M J 1959 Mon. Nol. R. Astron. Soc. 119 81-9
Sobelman 1 1 1972 Ali IlItroduction ta the 11Ieory of Atomic Spectra (Oxford: Pergamon) ch 9
Weisheit J C 1972 J. Qw;zllt. SpectJwc. Radiat. Transfer 12 1241-8
A.N N E X E
I I I
J. Phys. B: At. Mol. Phys. 20 (1987) 2657-2675. Printed in the UK
Excited-state photoionisation and radiative recombination for
ions of the potassium isoelectronic sequence
S Wane and M Aymar
Laboratoire Aimé Cotton, CNRS Il, Bâtiment 505, Campus d'Orsay, 91405 Orsay Cedex,
France
Received 8 August 1986, in final fonn 20 October 1986
Abstnct. Photoionisation cross sections for excited 111 states (11 lIIiii 20, t« 4) of K and positive
K-Iike ions have been computed in the framework of a non-relativisric single-electron
model by the use of a central potentiaI. The evolution of the non-hydrogenic behaviour
of photoionisation cross sections near threshold is studied 810ng a given 111 series and along
the K sequence. This evolution and the occurrence of minima and maxima in photoionisa-
tion cross sections are analysed in terms of the quantum defect theory.
Radiative recombination coefficients for K- Til + , Fe7+ and M0 2l + have been obtained
within the electron temperature range 5001!iii 'î:« 10000 K, by the use of the principle of
detailed balance. The significant non-hydrogenic features are outlined and the systematics
of the recombination of alltali atoms and alkali·like ions are analysed. Comparisons are
made with the results of the hydrogenic model and with ether available theoretical or
expenmental results.
1. Iatroductioa
A knowledge of ground- and excited-state photoionisation cross sections and radiative
recombination coefficients for atoms and positive ions is of primary importance in
radiative transfer in laboratory, astrophysical and thermonuclear plasmas, in addition
to the intrinsic interest for atomic theory.
In connection with recent progress in atomic beam techniques. and the development
of synchrotron radiation sources and laser research methods, there has been increased
attention to the study of photoionisation processes from excited atoms (Wuillemier
1982), mainly from neutral alkalis which have low excitation potentials (Kollath 1980).
For multicharged positive ions laboratory experiments are rather difficult and very
few results have been reported to date (Lucatorto and McIlrath 1976. McIlrath and
Lucatorto 1977). In addition, results for radiative recombination are still very scarce
(Rothe 1969. 1971). Therefore more data are needed for positive ions.
On the theoretical side, some calculations have been performed for mostly ground-
state photoionisation cross sections for ions of the Li sequence (McGinn 1970, Tiwari
et al 1975). Na sequence (Shevelko 1974, Butler et al 1984) or other alkali isoeleetronic
sequences (Black et al 1972, Reilman and Manson 1979. Chichkov and Shevelko 1981).
Systematic trends in excited-state photoionisation have been round recently mainly
for the neutral alkali atoms Li-Cs (Aymar et al 1976, Devdariani and Klyucharev
1977, Lahiri and Manson 1982) and the beginning of the Rb sequence (Aymar et al
1984).
0022-3700/87/122657 + 19502.50
(c) 1987 IOP Publishins Ltd
2657
2658
S Wane and M Aymar
As far as radiative recombination is concemed, some results for the rate coefficients
have been obtained for hydrogenic ions (Seaton 1959, Burgess 1964), alkali atorns
(Moskvin 1963, Caves and Dalgarno 1972, Wane 1985), the Li sequence (Barfield 1979,
Pradhan 1983), Na sequence (Mitai and Narain 1979) and for positive ions of astrophy-
sical interest (Woods et al 1981, Shull and Steenberg 1982).
It is then of interest to study the systematics of excited-state photoionisation and
of radiative recombination for alkali atorns and along alkali isoelectronic sequences.
The K-Iike ions have been less thoroughly studied than Li-Iike or Na-like ions.
However, some ofthem are of astrophysical interest (Ca +, Fe7+), are found in Tokamak
plasmas as impurities (Cr5+, Fe7+, M02J+) or are interesting for diagnostic purposes
(KrJ7+). The K isoelectronic sequence is therefore weil suited for investigation.
In this work we present results on excited-state photoionisation cross sections and
radiative recombination coefficients for K and K-Iike ions. Calculations for photoioni-
sation cross sections within the framework of a non-relativistic single-electron model
are perfonned by the method already employed by Aymar et al (1984). Radiative
recombination coefficients are then deduced by use of the principle of detailed balance,
following the procedure already given by Wane (1985).
The model used for the calculations is recalled in § 2. The results on the outer-shell
photoionisation cross sections along the ni Rydberg series (n ~ 20, 1~ 2) and along
the K sequence are presented in § 4. The systematic trends of the partial photoionisation
cross sections are analysed in tenns of the quantum defect theory, as indicated in § 3.
The results obtained for the radiative recombination coefficients of K-TiJ+, Fe7+ and
M02J+ within the temperature range 500 ~ T ~ 10 000 K are given in § 5. Emphasis is
put on the non-hydrogenic features, and systematic trends of the radiative recombina-
tion of alkali atoms and alkali-like ions are analysed. The hydrogenic model or other
available theoretical or experimental results are finally given for comparison.
2. Model ased to calculate photoionisation cross sections and radiative recombination
rate coeftidents
We recall in this section the fundamental points and basic fonnulae of the theory.
2.1. Central-field models used to eoaluate photoionisation cross sections
Within the framework of a non-relativistic single-particle central-field model, the cross
section (in cm') for photoionisation of an ni state of a one-electron system is given in
the dipole approximation by (Sobel'man 1972)
(1)
where 6", «0) is the binding energy of the electron nl and 6 (>0) is the energy of the
photoelectron. The energy of the incident photon is hl! = e - 6", (ail energies are in Ryd).
For 1'=0, O"",(e) is the sum of two partial cross sections 0",,'.'-1(6) and O"",.,+,(e),
respectively, associated with the photoelectron continua /-1 and l + 1.
Ions of the potassium isoelectronic sequence
2659
The radial matrix elements R"u2:I(E) (expressed in atomic units) are given in the
dipole-length formulation by
(2)
R"'.I'(E) =1
00
P",(r)rPel'(r) dr
where Pe,,(r) is normalised per unit energy range and has the asymptotic fonn
I/4s.m [
l' 11'
P
EI/ 2r-T+ Z
EI/21n(2el12r)+argf ( i Z
1'+1- E
)
]
e,.(r)-l'E-
I/2 +cS,.(E)
(3)
where z = Z - N + 1 is the residual charge on the final ion and cS,.( E) is the phaseshift
with respect to hydrogen-like wavefunctions.
The radial wavefunctions are calculated using two different central potentials
already employed successfully for excited-state photoionisation (Aymar et al 1984).
(i) The central potential has a simple analytic fonn depending on three parameters
which are detennined by comparing the experimental energies with zero-order calcu-
lated ones; this potential has been used for members of the K sequence where
experimental energies are available.
,
(ii) The central potential corresponds to the parametric potential introduced by
Klapisch(l971) which is represented by an analytic function depending on a set of
parameters, each parameter describing the distribution of charges in a shell n of the
atomic core. The optimal potential is detennined by minimising the total energy of
the ground state. This potential has been used for the other ions of the K sequence
where only a few experimental energies are known,
2.2. Radiative recombination rate coefficients
In the radiative recombination process of one-electron systems, an ion X~+ of charge
z in initial state ISO combines with a free incident electron to produce an ion or atom
X(Z-I)+ of charge (z -1) in a specifie final state n/ 2L while a photon of frequency v
is emitted:
(4)
This capture process is the inverse of the photoionisation process. The respective cross
sections u~,( v) and u:,( v) are related through the principle of detailed balance (Massey
1969)
c
(hv/ C)2
p
tr ..,(v) = 2(2/+ 1)
2
u",(v)
(5)
P
where v is the relative velocity of the incident eJectron, p is its momentum and c is
the velocity of light.
The corresponding recombination rate coefficient is given by the velocity (or
thermal) average
a",(T) =(VO'~,(v»=LOO VO'~,(v)f(v) dv
(6)
where f( v) is the Maxwellian distribution function of electron velocities.
The
2660
S Wane and M Aymar
coefficients a,,/( T) can be written as (Bates and Dalgamo 1962, Barfield 1979)
a"/(T)=(3286.3402)2(2/+1HkT)-J/ 2 1:lO (e+l,,/)2u~/(e)exp( - k~) de
(7)
where k is the Boltzmann constant. T is the electron temperature and e is the electron
kinetic energy, which satisfies hll = e + 1,,/ where 1,,/ is the ionisation potential of the
captured electron. Ali the energies are expressed in Ryd, u:/(e) is in cm? and a,,/( T)
is expressed in crrr' çl.
The radiative recombination rate coefficient on shell n is then
,,-\\
a,,( T) = L a,,/( T)
/-0
and the total radiative recombination rate coefficient on ail states is
"·"0
where no corresponds to the lowest untilled shell or subshell of the recombined ion or
atom. The coefficients a,,/( T) are cornputed from u:/( s ) values and then a" (T) and
at ( T) are deduced.
3. Quantum defect tbeory 8n81ysis of excited-srate photoionisation
The behaviour of photoionisation cross sections when the potential V( r) is a Coulombic
one or a much more realistic potential has been described previously (Burgess and
Seaton 1960, Fano and Cooper 1968. Aymar et al 1984). and only fundamental points
will be mentioned.
3.1. Hydrogenic behasiour and scaling factors
The cross section a' (s ) of a hydrogen-like ion of charge z is related to the hydrogen
cross section u H ( s ) by
u%(e) = uH(e/ Z2)/ Z2.
(8)
The comparison of cross sections along the K isoelectronic sequence will be carried
out using scaled energies e' = e] Z2 and scaled cross sections u'(e') = Z2u(Z2 e'), where
z has already been defined (equation (3».
For hydrogen H and hydrogenic ions the radial matrix elements R~/./%\\(e) are
always monotonically decreasing functions of 6. Then the partial photoionisation cross
sections U~I./:1: \\ (e) and the total cross section u~/( s ) are maximum at threshold and
drop to zero as e increases. For 1';160, the ratio u~I./_\\(e)/u~/./+\\(e) is always smaller
than 1 and increases with n. For a given ni series the partial and total cross section
threshold values increase with n.
3.2. Analysis of non-hydrogenic behaviour
For non-hydrogenic atoms or ions the behaviour of partial and total cross sections
can differ strongly from the hydrogen-like one. The most striking non-hydrogenic
feature is the occurrrence as e' increases of zeros in the radial matrix elements R"/./:I:\\( s '),
Ions of the potassium isoelectronic sequence
2661
giving minima in the partial cross section curves U~/.h:l(e'). Various non-hydrogenic
shapes of these curves (see figure 1) involving up to three minima have been obtained
for ground and excited alkali atoms (Aymar et al 1976, 1984, Msezane and Manson
1982, Lahiri and Manson 1982). The general trends of excited-state photionisation
cross sections of alkali atoms (Li-Cs) and Sr+ have been analysed recently by Aymar
et al (l984) in terms of the quantum defect theory of Burgess and Seaton (1960). This
analysis is used further and we recall its fundamental points.
The contribution to the dipole matrix elements R nl,,,( s ') cornes almost entirely from
the large r region where the excited electron moves primarily in the hydrogenic field
due to the core. The additional non-Coulomb forces which prevail within the core
modify the radial wavefunetions in the externat region. Both bound and continuum
orbitais are contracted and shifted towards the nucleus with respect to hydrogen-Iike
orbitais, so that their overlap is modified. The relative shift of the two orbitais with
respect to each other is responsible for the non-hydrogenic charaeter of photoionisation
from excited states.
The phaseshift of a bound orbital ni is measured by 'TTJLnl where JLnl is the quantum
defect of the ni state and the phaseshift of the continuum orbital is 8,,(e') (equation
(3». The quantum defeet method brings out an oscillatory dependence of radial matrix
elements Rnl.I,(e') on JLnl and 8 (8' ) such as cos[ 'TT~",.,,(e')] with
"
~ nl."( s') = - JLnl + 8,,(e')/ 'TT + X//,( n, s")
(9)
where the empirical parameter X is a slowly increasing function of n and e' (Peach
1967). The occurrence of zeros in the radial matrix elements R nl"( s ') is related to
half-integer values of ~nl."(s"),
Near the threshold, an approximate value of ~nl."(e ') can be obtained by using in
equation (9) the Iimiting values obtained for n =co and e' =0:
(l0)
where the asymptotic value X(O) of function X can be extracted from the tables of
Peach (1967). The quantity ~JL//' = JLI' - JJ.I represents the quantum defect difference
for large n values.
A critical quantum defect difference ~JJ.?" for the zero of radial matrix elements
Rnl.l'(t') to occur is defined by the relation
~JL?'.+ X//,(O) = ±0.5.
(ll)
a
Type
Type
Type
Type
Type
lai
(bl
le1
(dl
(e)
E:
Filare 1. Schematic cross section curves for live typical cases.
Table 1. Shape types of O':'I.I'(e') cross sections according to ~IJ.II' values.
o
...
no zero
one zero
two zeros
threezeros
(8), (b)
(c), (d)
(e)
(0
2662
S Wane and M Aymar
The shape types of the partial cross section curves O'~/.r<e') depend on the difference
1~J.LIl'I-I~J.L ~·I (see table 1), the number k of zeros being determined by the inequalities
(12)
4. Results for excited-state pbotoionisation of K and K-like ions
Photoionisation cross sections have been computed for ni series (n ~ 20, 0 ~ 1~ 4) of
K Ca+ SC2+ T'J + -y4+ CrS+ Mn6+ Fe'+ Zn 11+ Kr"+ and M023+ Only the photoioni-
,
,
, 1 "
,
,
"
.
sation of the outer ni electron is considered and autoionisation effects are ignored.
The validity of this treatment is confined to the near-threshold energy range. Neverthe-
less calculations are perfonned for higher photoeleetron energies in order to detect
the various minima occurring in the partial cross sections O'~/.I'(e') and analyse the
systematics of these minima.
The shape type of each O'~/.I'( s') curve is given in table 2 for each ni .. e' l' transition
of K and K·like ions. In the same table, the asymptotic quantum differences ~J.LII'
obtained from our calculations are compared with the critical values ~J.L~' (equations
(10) and (11» derived from the tables of Peach (1967).
For large 1 values (/> 3), the 1~J.L1l'1 are small and partial cross sections O'~I,/'(E')
are not different from those for hydrogen. At the opposite extreme, for 1~ 2, various
cross section curves exhibit extrema, the number of minima being well described by
inequalities (12). Let us note that the presence of minima, related to cancellation
effects in radial matrix elements, lessens the cross sections as compared with those for
hydrogen.
4.1. Evolution of partial cross sections along a Rydberg series
The ~J.LI/' and ~J.L~' quantities involved in inequalities (12) correspond to asymptotic
values. For low-lying levels of a given series, quantum defects J.L", can differ from the
limiting value J.LI for large n. Therefore when I~J.L/l'I ==0 I~J.L~·I + k -1 the critical value
for k zeros is only reached for highly excited states and a change of shape in the
photoionisation curves occurs as n increases. It May be noted (see table 2) that the
O'~d.l{e') curve changes shape type twice along the nd series of Ca", Sc2+ and Ti3+.
Indeed for these elements the quantum defeet difference ~J.L"d.f for low n is quite
different from the corresponding value for large n.
For each series of any element, the minima (or maxima) occurring in O'~/.I'(e')
generally MOye away (or towards) the threshold as n increases and then become
stationary when J.Lnl and XII'(n, e ') in (10) reach their asymptotic values. Therefore the
non-hydrogenic behaviour remains for highly excited ni states.
4.2. Isoelectronic variation of partial cross sections
The evolution of non-hydrogenic behaviour of the cross sections O'~/.r<e') along a
sequence is related to the dependence of the quantum defect J.L",(Z) on Z, the nuclear
charge. The isoeleetronic variation of J.Ln'(Z) for a given ni series depends strongly
on the 1 value (Edlèn 1964). For small 1, J.Ln'(Z) is mainly due to the penetration of
the ni orbital in the core and decreases as Z increases. For large 1, core polarisation
Table 2. For a given ni .... e'I' transition, compilation of t11J.~' and t1p.1I' values, and the shape type of u:,I.,.(e') cross section for each element.
ë'
::s
Elements
Loo
~
...
Transition
K
Ca"
Se2+
TiH
V4+
CrS+
Mn6 +
Fe7+
Zn""
Kr 17+
M02H
t1p.~.
::s-
1'\\
~
ns .... s'p
-0.46
-0.35
-0.30
-0.27
-0.24
-0.22
-0.21
-0.19
-0.15
-0.11
-0.09
-0.37
0
...
s:::a
(e)
(b)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
Loo
Loo
-.
s::
np .... E's
0.46
0.35
0.30
0.27
0.24
0.22
0.21
0.19
0.15
0.11
0.09
0.71
~
(a)
(a)
(a)
<a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
i;;'
0
np .... s'd
-1.47
-0.82
-0.64
-0.54
-0.47
-0.42
-0.38
-0.35
-0.26
-0.19
-0.15
-0.42
III
(d) n.e;; 8
(e)
III
(e)
(b) ri ~ 4
(b) 4.e;;n.e;;6
(b) 4.e;;no;;lJ
(a) 4.e;;n.e;;7
(a)
(a)
(a)
(a)
-~...
(e) n ~9
(e) n ~ 5
(c) ri ~ 7
(e) n~14
(b) n ~ 8
a
::
-.
nd .... e'p
1.47
0.82
0.64
0.54
0.47
0.42
0.38
0.35
0.26
0.19
0.15
0.75
~
Loo
(e)
(a) n.e;; 3
(a)
<a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
III
..Q
(b) 4.e;; n.e;; 5
s::
III
(e) n ~ 6
::
~
III
"d .... ET
-0.22
-0.62
-0.55
-0.49
-0.43
-0.38
-0.34
-0.31
-0.22
-0.16
-0.12
-0.48
(a)
(a) n.e;; 3
(a) n.e;; 3
(a) n.e;; 4
(a) 3.e;;".e;; 7
(a)
(a)
(a)
(a)
(a)
(a)
(b) 4.e;;n.e;;5
(b) 4.e;;n.e;;7
(b) 5.e;;n", Il
(b) n ~ 8
(e) n--6
(e) n ~ 8
(e) n ~ 12
nf.... s'd
0.22
0.62
0.55
0.49
0.43
0.38
0.34
0.31
0.22
0.16
0.12
0.78
<a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
IV
0\\
0-
w
2664
S Wane and M Aymar
effects are responsible for most of the JJ."'; for these non-penetrating orbits, Edlèn
(l964) showed that JJ."J(Z) first increases with Z, then passes through a maximum and
ultimately decreases.
So lâJJ.spl and JâJJ.pdl decrease along the K sequence. nie evolution along the
isoelectronic sequence of the shapes of the O'~s.p(e'), O'~p.s(E'), O'~P.d(E') and O'~d.p(E')
curves is quite regular; the extrema observed for low ionisation stages progressively
move towards the threshold and then into the discrete spectrum when Z increases.
ln contrast, IAJJ.dtl first increases with Z from K to Ca + and then decreases. Thus
for photoionisation of d states non-hydrogenic features including advent of new extrema
are more important for some ions (Ca + ... y4+) than for the neutral K.
4.3. Typical illustrations
Non-hydrogenic behaviour of total cross section O'~,( E') curves will now be illustrated
for s, p and d states.
4.3.1 ns series (4~ n ~ 20). Figure 2(a) shows the evolution of the scaled cross section
curve O'~(E') along the sequence and figure 2(b) the evolution with n of the threshold
values O'~s(O). Except for low ionisation stages (K, Ca") the cross sections move
progressively further to the hydrogen ones along the K sequence. The O'~S(E') curves
of K (type (c)) and of Ca+ (type (b)) strongly differ from the hydrogen one and
1
'=ë
~
1
..
§
_01
CI
..
~
ii
-1 1
10 ~
10-2+-----,---r--...,.--r-----r--r--~_+
0.2
0.4
0.6
0.8
1.0
4
6
8
10
12
14
16
18
20
t' IRydl
n
Figure 2. (a) Scaled total cross sections O'~I (in Mb, 1 Mb "" 10-11 cml ) along the K sequence
plotted against the sealed photoelectron energy e' (in Ryd) for 4s. (b) Scaled total cross
sections at threshold U~/(O} alona the K sequence ploned against Il for ns series.
Ions of the potassium isoelectronic sequence
2665
threshold values are much smaller than that for hydrogen owing to large cancellation
effects in the radial matrix element R"s.p(E'). For the highly ionised ions the cross
sections O'~s(E') are of hydrogen-like type (a) but nevertheless decrease less rapidly
with E' than in the hydrogen case.
4.3.2. np series (4~ n ~ 20). Figure 3(a) shows the evolution of the scaled cross section
curve O'~p( E') along the sequence and figure 3(b) the evolution with n of the threshold
values O'~p(O). The curve O'~P.d(E') presents markedly non-hydrogenic features for the
first members of the sequence (K-. Mn6+). In many cases one has 0'~P.d(6') < O'~p.s(E');
thus the extrema occurring in O'~P.d(E') are not apparent in the total cross section
curves. However for K-TiJ+ the minima of O'~P.d(E') result in the change of slope of
O'~p(E') as is obvious on figure 3(a) for n = 6.
4.3.3. nd series (3E;n=S:;:20). Figure 4(a) shows the evolution with Z of O'~(E') and
figure 4(b) the evolution with n of scaled total and partial threshold cross sections.
The decrease of O'~d( E') is much slower than the hydrogen one; while the curve O'~d( E')
is of hydrogen-like shape type (a) for K., the O'~i E') cross sections of many ions
(Ca+ -. Mn6+) present striking non-hydrogenic traits. For Ca+ and Sc2+ the extrema
of O'~d.r<E') profoundly affect the total photoionisation curve for some particular n
values. For n > 3, the O'~d( E') curve of Ca+ exhibits extrema corresponding to those
of O'~d.r<E') (see O'~(E') on figure 4(a»; for Sc2+ and 3 < n < 8, the curve O'~d(E') is of
type (b) (see O'~d(E') on figure 4(a» as is O'~d.,{E'). For more ionised ions the curve
O'~d( E') is of hydrogen-like type (a) as illustrated on figure 4(a) for Ti3+ and n = 6.
Nevertheless non-hydrogenic features are still important; in particular one has in many
cases O'~d.,{E') < O'~d.p(E') for some n values (see figure 4(b) for Cr'"). The increase
of non-hydrogenic charaeter with n for a given ion which lessens the cross section
values O'~d.r<O) (see figure 4(b) for Sc2+) explains the pronounced minima presented
by the threshold values O'~d(O) for Ca+ to Cr'" (figure 4(b».
10
o
10-2 +--r--,--r-....,..----,.-..--.--~-..-+
o
0.2
0.4
0.6
0.8
1.0
8
12
16
20
E'IRyd)
n
Flpre 3. The same as filure 2 for (a) 6p and (b) np series.
2666
S Wane and M Aymar
--1..__ •.1----1_...1--........1-_1_...1--........1---..1._+
lb)
(a 1
10
1)2
:a
:a
~
s
ë 10
lOl1~
...
....
-:a
Ct
II·
..?""'
_- .
-"
Ct
,
,
1
,
.I.l--
....
10.1
.
l
II
10·2-1---r-..--""T'""--r~.,.....--r-~.....---r-+
10"
fVl
Sel' ..........•..
~ "\\ /~>-_..
1lt'1 \\f
2
6
la
'" 18 12
+-----,r-----r--+-=-..::.-+=-.:;:....;=-+
o
0.2
0.4
0.6
0.8
1.0
2
6
10
14
18
22
E' (Ryd)
n
figure 4. The same as figure 2 for (a) 6d and (b) nd series. For the inset, scaled partial
and total cross sections at threshold for Sc2+ and Cr5+: - - -, (]'~d.P(O); ..... , (]'~d.(O);
- , (]'~d(O).
In summary, significant non-hydrogen-like features have been obtained for partial and
total photoionisation cross sections from ground and excited ni states (n:!6i 20, 1:!6i 2)
of K and K-Iike ions, in conneetion with the relatively large values of the quantum
defects of these states.
4.4. Comparison with previous work
Our predictions are compared with previous work in table 3 for threshold cross sections
0'",(0).
.
(a) For K the only available experimental result concems the ground state (Marr
and Creek 1968. Sandner et al 1981). Our curve 0'45(E) (see figure 2(a» has the same
general shape as the experimental curve but the minimum is farther from the threshold
than the corresponding experimental one. Our near-threshold cross sections are larger
and our values past the minimum smaIler than the corresponding experimental ones.
Similar discrepancies are observed in the other theoretical results (McGinn 1970,
Aymar et al 1976). In fact the cross sections 0'"5( E) are much smaIler than the hydrogen
cnes, and very sensitive to a smaIl change of wavefunctions because of strong cancella-
tions effects occurring in the radial matrix elements.
Our results for excited-state photoionisation cross sections are identical to those
already given by Aymar et al (1976) who used the same kind of central potentiaI.
They compare weIl (table 3) with the results obtained by Moskvin (1963) from the
quantum defect theory (Burgess and Seaton 1960), especiaIly for the np and nd states.
For 0'3d( E ) our values are similar but somewhat higher than those obtained by Msezane
and Manson (1984) with the velocity Hartree-Fock (HF) formulation. The value of
Ions of the potassium isoelectronic sequence
2667
Table 3. Calculated cross sections (in Mb) al threshold; comparison with previous theoreti-
cal results,
Msezane (1984)"
Black
Reilman
Present
Moskvin
McGinn
et al
and Manson
work
( 1963)
H5
L
V
(1970)
(1972)
(1978)
K
5s
0.33
0.52
4p
4.72
4.80
3d
27.14
35.00
31.35
24.83
24.76
Ca+
45
0.198
0.171
0.209
Fe'+
3d
0.698
0.766
• H5, Hartree-Slater; L, length; V, velocity.
U)d(O) compares weil (table 3) with the results obtained by Msezane (1984) with the
Hartree-Slater potential and the multiconfiguration Hartree-Fock (MCHF) method.
(b) For Ca + only theoretical results for the ground state are available. Our values
for 0"4s(e) are a little smaller than values obtained by Black et al (1972) who take
account of core polarisation effects, and a tittle higher than those of McGinn (1970)
who used a pseudopotential method and those of Reilman and Manson (1979) obtained
with a Hartree-Slater potential model.
(c) For the other ions of the K sequence the only available theoretical results
concem the 3d ground state. Our values for O"id( E) of Sc2+- Fe7+ and Zn Il + are in
good agreement with values of Reilman and Manson (1979) within the energy range
considered; and our curve O")d( E) for Fe7+ is practically the same as that obtained by
Reilman and Manson (1978) from a Hartree-Slater central-potential model. Here the
partial cross sections O")d.r( E) are indeed of hydrogen-like shape type (a) and are not
very sensitive to a small change of wavefunctions as are 0""S,p( E) of K and Ca".
Core polarisation effects can be taken into account to improve the photoionisation
cross sections, particularly from the ground state of K (Weisheit 1972) and Ca".
However, only excited ni states (1 E;; 2) where the cross sections are small are mostly
affected (Aymar et al 1984) and core polarisation effects decrease rapidly along a
sequence (Shevelko 1974, Chichkov and Shevelko 1981).
In conclusion, although the overail trends of photoionisation cross sections given
here are expected to be valuable, more theoretical and experimental data are needed
to assess the reliability of our calculations.
5. Radiative recombination rate coefficients for K and K-Iike ions
Radiative recombination rate coefficients have been calculated for the recombining
.
K+ C 2+ S )+ T' 4+ F 8+
d M 24+
h
d
. h
Ions
,
a , c ,
1
,
e
an
0
; t ey are compare
wit
the results of the
hydrogenic model. Autoionisation effects are completely disregarded in the determina-
tionation of the photoionisation process. Consequently, the computation of the radia-
tive rate coefficients is restricted to the temperature range SooEt TEt 10000 K which
confines the effective range of the electron energy closer to threshold the lower the
temperature.
2668
S Wane and M Aymar
5.1. Results of the hydrogenic model
The results for recombination of hydrogen H and hydrogen-Iike ions are first recalled.
For atomic hydrogen and hydrogenic ions ail the radiative recombination rate
coefficients May be calculated exactly (Boardman 1964, Burgess 1964), or approximately
using the Kramers-Gaunt factors (Seaton 1959). The radiative recombination rate
coefficient a=( T) of a hydrogen-like ion of charge z is related to the hydrogen one by
a=(T)=za H(Tlz 2 ) .
(13)
The comparison of the coefficients a,,/( T) along the K sequence will be carried out
using scaled temperatures and scaled radiative recombination coefficients defined by
the relations
T'= Tlz 2
(14)
a'( T') = a(z 2T')1 z
where z is the charge of the recombining ion.
Recently features of hydrogenic recombination have been outlined (Wane 1985).
For given 1 and 'T, the coefficients a ~/ decrease monotonically with increasing n for
1~ 3. For given n and 1 values the coefficient a ~/( T) decreases monotonically with
increasing temperature. Consequently the coefficient a ~(T) decreases with n for given
'T, decreases with T for given n, and therefore the coefficient a:( T) decreases with T.
5.2. Results for the radiative recombination rate coefficients of K and K-like ions
For any n the calculated coefficient a,,/( T) is close to the hydrogen-like one a~/( T)
for 1> 3, but is quite different for 1:!Ié: 2 mainly for K - Te-+-.
5.2.1. a,,/(T), 1:s;.2. We will look at two cases.
(a) Evolution of alti with n for 1 and T fixed.
For the first members K·Ti3+ the
evolution with n of a ~/ (1 ~ 2) at a fixed temperature T' =500 K is shown in figure 5
and compared with a~. Non-hydrogenic characters are obvious, mainly for a~s of
K·Ca+ and a~d of Ca"- Ti 3+. The non-hydrogenic behaviour of the cross section
O'~/(E') near the threshold leads to O'~/(E')« O'~/(E'), and thus to a~/« a~. This is
particularly noticeable for a~s and a~d (n close to 6) of Ca+; the evolution with n of
a~/ is closely related to that of the O'~/(O) values shown in figure 2. The curve a~s
presents a maximum for K; indeed the minimum for O'~(E') is very close to threshold,
resulting in a small value of a ~s for n =4 associated with a maximum at n =5. The
a~p of Ca" are greater than the a~p; in fact the decrease of O'~p(E') with E' is slower
than in the case of hydrogen. Moreover the great values of the ionisation potentials
I"p give a higher weight to the factor (E + I"p)2 occurring in equation (7).
(b) Evolution of a,,/( T) with T for n and 1fixed. In this work ail the coefficients
a,,/( T) of any element have been calculated up to a temperature not higher than
10 000 K in order to study the effects of non-hydrogenic behaviour of cross sections
near threshold. The comparison of a ~/( T') with a ~/( T) along the K sequence requires
high temperatures for the ions and consequently values of the cross sections correspond-
ing to large eleetron energies. Therefore here and in the following sections the coefficient
a( T) should be considered and compared with the corresponding a=( T).
For given n and l, the coefficient a"/( T) generally decreases monotonically with
increasing temperature T. Departures from this behaviour for K and Ca + are illustrated
Ions of the potassium isoelectronic sequence
2669
1b 1
10.15
9
10
-1
...
III
1
III
'" 10'·'
•
...
"'. 10'14
~
..
Q,
-e
_c
f3
10.17
10.15
..
10.11
10.16
,.
8
12
16
20
4
8
12
16
20
n
n
( c 1
-...1 14
<il
10
'"Il
......C-f3 10.15
Alure 5. Scaled radiative recombination coefficients
a~1 (in units of cm? S-I) for K- Ti2+ plotted against
4
8
12
16
20
n at a scaled temperature T' =SOO K for (a) /lS series,
n
(b) np series and (c) nd series.
in figure 6; the unusual T dependence of a 4S( T) for K and of a"d( T) (n = 5-9) for
Ca + is related to the evolution of the corresponding a ",( E) with E. Indeed the efficient
electron energy range increases with T; when a sufficiently pronounced maximum of
a ",( E) occurs within this range, than a",( T) does not decrease monotonically with T
and may even increase with T from a minimum. In particular the ratio of the maximum
2670
S Wane and M Aymar
of O'"s(E) to O'"s(O) for K is large for n =4 and decreases rapidly with increasing n;
the same behaviour holds for O'"d( E) of Ca + where the corresponding ratio is very high
for n = 6. The increase of a4S(T) and a"d( T) with T implies the disappearance of the
extrema observed in figure 5 at temperatures higher than the relatively low temperature
considered there. The coefficients a"/( T) which increase with T from a given tem-
perature will ultimately reach a maximum at a temperature beyond the temperature
range studied here, and then decrease with Tt as may be expeeted from equation (7).
The coefficient a"/( T) which decreases with T decreases slower than a ~/( T) because
0'"/( E) decreases with E slower than O'~/( E). For lower n values high ionisation potentials
of the ni states (1 ~ 2) enhance a"/( T) relative to a ~/( T). For a given n, the coefficients
a"/( T) decrease with T faster the higher L So the relative importance of the a"/( T)
corresponding to lower 1 values increases with temperature.
5.2.2. a" (T). The radiative recombination coefficients a" (T) on the shell n for K,
Fe7+ and M0 23+ (n~ 10) and for Ca+ (n~20) are given in tables 4-7; the coefficient
a" (T) decreases with n for given T and with T for given n, as for the corresponding
hydrogen-like coefficient a~( T). The ratio a"( T)I a~( T) (figure 7) generally increases
with T and is higher the lower n becomes. In fact, a"/( T) decreases with T more
slowly than a ~/( T). The non-hydrogenic character is enhanced with increasing T due
to the relative importance of a"/( T) with low 1 values.
The increase of a"( T)I a~( T) with T is particularly important for K because the
E dependence of 0'"/(E) (1 ~ 2) exhibits weIl marked non-hydrogenic behaviour.
10" 1 !
lb 1
Ca'
r
1
10
1
'15
1
10-12 ~
1 (a)
1
i
;
1
1
1
10 '16 "'t
10''''
!
-7'
'"
'"
,
,..
,..
e
...
e
1
-10 '17 _
..c:r;,
J10'''1
i
1
10'18 J
10.j
1
10.19 .
10-'6
1
i
i
i
i
0
2000
4000
6000
8000
1000
0
2000
4000
6000
8000
10000
T ( KI
T (KI
Fiaure 6. Radiative recombination coefficients plotted against temperature T (in K):
(a)a".(T) for K and (b) a"d{T) for Ca+.
Ions of the potassium isoelectronic sequence
2671
2.0
1.8
1.6
(b 1
CaO
1.2
.... 1.4
....
CI
CI
-
4
-
e
"'J 1.0
CI
20
1.2
-
0.8
10 \\ \\
\\
8 \\
1.0
6
5
0.6
0.8,
0
2000
4000
6000
8000
1000
0
2000
4000
6000
8000
10000
T IKI
T IK 1
Figure 7. Ratio ".( T)I,,~( T) plotted against temperature for variaus n values and for (a)
K (z = l) and (b) Ca" (z =2).
For Ca+, a"(T)/a~(T)decreases with T for n~6 in relation with the n and T
dependences of a"d( T).
The coefficient a"( T) differs from a~( T) for K, Fe7+ and M023+ (n < 10) and for
Ca+ (n:l!i: 20), and a"( T) may be up to 1.5 and 2 times largerthan a~( T) for respeetively
M023+ (n =4) and K (n =4), or up to 1.2 times smaller for Ca+ (n =6). However as
n increases the relative importance of the non-hydrogenic contributions to a"( T)
corresponding to a",( T) with 1~ 2 decreases so that for n;;1: 10 approximately a"( T) =
a~(T) for K, Fe7+ and M023+. For Ca+ a"(T)=a~(T) only for n>20, due to the n
and T dependences of atui ( T).
5.2.J. Results for a,( T). The total radiative recombination coefficient a t( T) has been
calculated for K, Ca+, Fe7+ and M023+ by a procedure already given (Wane 1985).
The coefficient a t( T) is split into one part corresponding to the non-hydrogenic
contribution and into another corresponding to the hydrogenic contribution as follows:
" l
" l
a t ( T) = a3d(T) + L a"( T) + a:( T) - L a~( T)
"-4
"-1
where nL =9 for K, Fe7+ and M023+ and nL =20 for Ca ". The coefficients a~( T) and
a:( T) are obtained from Seaton (1959).
For comparison of a t( T) with the results of the hydrogenic model, a:( T) must be
modified to accouru for the filled shells and subshells of XZ+. We have therefore
calculated the corresponding a:·5( T). The coefficients a3d(T) and a t( T) and the ratio
a t ( T)/ at5( T) are given in tables 4-7. The ratio a t( T)/ a:'S( T) is always higher than
1 and increases with 'T. rapidly for K and Ca\\ but much less so for Fe7+ and M023+.
Modelling the total radiative recombination coefficient by the hydrogen-Iike one is
therefore not always reliable,
2672
5 Wane and M Aymar
14
Table 4. Values of aJ<.!( T). a ( T) (n.s; 10) and a ,( T) (in units of 10-
cm! S-I) for K and
n
of a,( T)/ a;"( T) (z = 1). for various values of T.
T(K) = 500
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
aJd
21.90
15.22
10.38
8.20
6.89
5.99
5.33
4.82
4.40
4.06
3.77
a 4
24.61
17.44
12.32
10.11
8.83
7.97
7.34
6.86
6.46
6.14
5.86
a,
15.51
10.69
7.19
5.68
4.80
4.22
3.80
3.48
3.23
3.02
2.84
a 6
12.02
8.07
5.21
3.98
3.28
2.83
2.50
2.25
2.06
1.90
1.77
a,
9.58
6.60
4.10
3.10
2.5
2.2
1.80
1.70
1.50
1.40
1.2
a g
8.48
5.44
3.28
2.39
1.90
1.59
1.37
1.20
1.08
0.98
0.90
aq
7.4
4.6
.2.6
1.9
1.5
1.3
1.1
1.0
0.80
0.75
0.70
a 10
6.43
3.99
2.27
1.60
1.25
1.01
0.86
0.75
0.66
0.59
0.54
a,
193.6
115.8
69.1
51.1
41.2
35.0
30.5
27.4
24.8
22.8
21.1
a,/ a;.s
1.04
1.07
1.11
1.15
1.19
1.23
1.27
1.31
1.35
1.39
1.42
Table 5. Values of aJd(T). an(T) (n.s;20) and a,(T) (in units of 1O-' 4cmJs- ') for Ca"
and of a,( T)/ a,:"( T) (z =2) for various values of T.
T(K) = 500
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
aJd
241.40
171.44
122.23
100.60
87.81
79.15
72.80
67.89
63.97
60.74
58.02
a 4
82.31
58.62
41.01
33.16
28.47
25.27
22.90
21.07
19.59
18.38
17.35
a,
56.41
39.83
27.31
21.69
18.31
16.00
14.30
12.98
11.92
11.04
10.31
a 6
47.39
33.19
22.37
17.50
14.59
12.59
11.13
10.00
9.09
8.35
7.72
as
37.26
25.65
16.77
12.76
10.08
8.85
7.69
6.81
6.11
5.54
5.06
a 10
30.87
20.96
13.29
9.90
7.92
6.61
5.67
4.96
4.40
3.96
3.59
a l2
25.18
16.38
10.19
7.52
5.95
4.95
4.23
3.68
3.26
2.92
2.64
a l6
18.10
11.37
6.74
4.82
3.75
3.06
2.57
2.22
1.94
1.73
1.62
a20
13.64
8.24
4.69
3.28
2.51
2.03
1.69
1.41
1.26
1.11
0.97
a,
1128.14
711.00
441.89
334.76 276.10
236.77
207.90
187.04
170.34
157.39
145.98
a,/a;"
1.145
1.165
1.192
1.221
1.254
1.279
1.297
1.321
1.341
1.365
1.382
Table 6. The same as table 4 (in units of 10-12 cmJ S-I) for Fe'· with z =8.
T(K) =500
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
aJd
47.40
34.00
24.04
19.62
16.99
15.19
13.87
12.84
12.00
11.32
10.73
a 4
20.45
14.67
10.37
8.47
7.33
6.56
5.98
5.54
5.18
4.88
4.63
a,
12.88
9.23
6.53
5.33
4.61
4.12
3.76
3.48
3.25
3.07
2.91
a 6
9.69
6.95
4.91
4.01
3.47
3.11
2.83
2.62
2.45
2.31
2.19
a,
8.00
5.80
4.00
3.20
2.80
2.55
2.40
2.20
2.10
2.00
1.90
as
6.80
4.89
3.47
2.84
2.46
2.21
2.02
1.87
1.75
1.66
1.57
a q
6.10
4.40
3.10
2.50
2.10
1.90
1.70
1.60
1.50
1.40
'1.30
a 10
5.04
3.88
2.76
2.27
1.97
1.77
1.63
1.51
1.42
1.39
1.27
a,
286
189
124
96
80
70
62
57
52
48
45
a,/ a;.s
1.20
1.23
1.25
1.27
1.28
1.29
1.30
1.31
1.32
1.33
1.34
Ions of the potassium isoelectronic sequence
2673
Table 7. The same as table 4 (in units of 10- 12 cm)
1)
5-
for Mo:3 + with z = 24.
T(K) =500
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
ald
183.60
135.34
95.77
78.19
67.71
60.55
55.27
5U7
47.86
45.12
42.80
a 4
186.32
131.03
92.70
75.69
65.53
58.61
53.51
49.53
46.33
43.67
41.43
as
126.04
90.40
63.91
52.17
45.19
40.41
36.88
34.14
31.93
30.09
28.55
a"
95.86
69.44
49.11
40.08
34.71
31.02
28.32
26.21
24.52
23.11
21.91
a7
80
57
41
34
29
26
24
22
21
19
18
a.
66.61
48.07
33.98
21.73
24
21.46
19.58
18.12
16.94
15.96
15.13
a9
58
42
29
25
21
19
17
16
15
14
13
alO
51.80
37.30
26.36
21.47
18.61
16.63
15.17
14.03
13.11
12.35
11.71
al
2946
1964
1297
1018
853
745
666
606
559
519
485
ai a~"
1.083
1.094
1.101
1.107
1.11
1.11
1.12
1.12
1.12
U2
1.12
It would be useful to compare our results with others obtained for" K and K-like
ions or for other alkali-like atoms and ions. Unfortunately only a few theoretical
results have been reported for the temperature range studied. It is of interest to compare
our results for K with those previously obtained for Li (Caves and Dalgarno 1972)
and Rb (Wane 1985) where model potentials taking account of core polarisation effects
have been used. The two coefficients a l ( T) for Li and Rb are practically the same
and always higher than a l( T) for K~ the ratio a l ( T)I a~'S( T), which equals 1.82 for
Rb and 1.23 for K at T = 5000 K, is always much higher for Rb than for K.
Calculations have been made for a l ( T) of astrophysically abundant light elements.
The value al (10000 K) = 6.78 X 10- 13 cnr' S-I obtained by Shull and Steenberg (1982)
for Ca" from interpolation along isosequences is twice as small as our al (10000 K) =
14.60x 10- 13 cm? çl. This suggests great care in the calculation of at(T) for Ca" and
the need of other results for comparison.
Woods et al (1981) have obtained a l ( T) for Fe ions using photoionisation cross
sections calculated with a Hartree-Slater central-potential modeI. Their value of a t
(10000 K) =6.05 X 10- 11 cnr' S-I for Fe7+ compares weil with our a (10000 K) =
t
4.52 X 10- 11 cm? S-I. The difference may come from the highly excited states they have
considered to be hydrogen like.
The results available for a t ( T) of ions like Li (Barfield 1979), Na (Mitai and Narain
1979) and K (Kim and Pratt 1983) concern temperatures much higher than those
considered here, and have been obtained mostly taking into account relativistic efîects.
6. Conclusions
This work on excited-state photoionisation cross sections and radiative recombination
coefficients for K and positive K-like ions extends the previous studies performed for
Rb-Sr+ (Aymar et al 1984, Wane 1985). The results given add to the ones obtained
for alkali atoms (Moskvin 1963, Caves and Dalgamo 1972, Aymar et al 1976) and
alkali-like ions (McGinn 1970, Pradhan 1983, Butler et al 1984). Markedly non-
hydrogenic features have been outlined for photoionisation cross sections and radiative
recombination coefficients, particularly for K- rt". It would he of interest to extend
the temperature range and therefore to study the role of excitation of inner-shell
electrons in recombination of alkali atoms and alkali-like ions. ft is also worth while
2674
S Wane and M Aymar
to extend the present results to other one-electron systems or more complex atoms
and ions. Finally, core polarisation and relativistic efîects could be taken into account
in the photoionisation cross section calculations.
Acknowledgments
A critical reading of the manuscript and helpful discussions with Mrs E Luc and 0
Robaux are highly appreciated and gratefully acknowledged.
References
Aymar M, Luc-Koenig E and Combet-Fameux F 1976 J. Phys. B: At. Mol. Phys.9 1179-91
Aymar M, Robaux 0 and Wane S 1984 J. Phys. B: At. Mol. Phys. 17993-1007
Barfield W 0 1979 Astrophys. J. 129 856-66
Bates 0 Rand Oalgamo A 1962 Atomic and Molecular Processes ed 0 R Bates (New York: Academie
Press) ch 7
Black J H, Weisheit J C and Laviana E 1972 Astrophys. J. 177567-72
Boardman W J 1964 Astrophys. J., Suppl. Ser.9 185-92
Burgess A 1964 Mon. Not. R. Astron. Soc. 69 1-20
Burgess A and Seaton M J 1960 Mon. Not. R. Astrort. Soc. 120 121-51
Butler K, Mendoza C and Zeippen C J 1984 J. Phys. B: At. Mol. Phys. 172039-48
Caves TC and Dalgamo A 1972 J. Quant. Spectrosc. Radiat. Transfer 12 1539-52
Chichkov B N and Shevelko V P 1981 Phys. Scr.23 1055-65
Devdariani A Z and Klyucharev A N 1977 Opt. Spectrosc. 42 694-95
Edlèn B 1964 Handbuch der Physik vol 27 Spectroscopy (Berlin: Springer) pp 80-220
Fano U and Cooper J W 1968 Rev. Mad. Phys.40 441-507
Kim Y S and Pratt R H 1983 Phys. Reu: A 27 2913-24
Klapisch M 1971 Comput. Phys. Commun. 1 239-60
KoUath K J 1980 J. Phys. B: At. Mol. Pnys. 13 2901-19
Lahiri J and Manson S T 1982 Phys. Rev. Leu. 48 614-16
Lucatorto T Band McIlrath T J 1976 Phys. Re». Lett. 37 428-31
Marr G V and Creek D M 1968 Proc. R. Soc. A 304 233-44
Massey H S W 1969 Electronic and Ionie Impact Pnenomena vol II (Oxford: Clarendon) ch 14
McGinn G 1970 J. Chem: Phys. 53 3635-40
McIlrath T J and Lucatorto T B 1977 Phys. Rev. Lett. 38 1390-3
Mitai H P and Narain U 1979 Physica 91C 305-8
Moskvin Yu V 1963 Opt. Spectrosc: 15316-18
Msezane A Z 1984 Phys. Rev. A 29 3431-3
Msezane A Z and Manson S T 1982 Phys. Rev. Lett. 48 47:3-5
- - 1984 Phys. Rev. A 30 1795-9
Peach G 1967 Mem. R. Astron. Soc. 71 13-27
Pradhan A K 1983 Astrophys. J. 270 339-41
Reilman RF and Manson ST 1978 Phys. Ret: A 182124-30
- - 1979 Astrophys. J., Suppl. Ser. 40 815-80
Rothe D E 1969 J. Qua"t. Spectrosc. Radiat. Transfer 6 277-90
- - 1971 1. Quant. Spectrosc. Radiai. Transfer 11 355-65
Sandner W, GalJagher TF, Sanfinya K A and Gounand F 1981 Phys. Rev. A 23 2732-5
Seaton M J 1959 Mon. Not. R. Astron. Soc. 11981-9
Shevelko V P 1974 Opt. Spectrosc. 36 7-9
Shull J M and Steenberg M V 1982 Astrophys. J., Suppl. Ser. 48 95-107
Sobel'man 1 1 1972 An Introduction to the Theory of Atomic Spectra (Oxford: Pergamon)
Tiwari p. Hashim M A and Ojha S P 1975 Can. J. PItys. !~ 1524-27
Ions of the potassium isoelectronic sequence
2675
Wane S 1985 J. Plrys. 8: AI. Mol. Plrys. 183881-93
Weisheit J C 1972 Plrys. Rev. A 5 1621-30
Woods 0 T, Shull J M and Sarazin C L 1981 Astrophys. J. 249399-401
Wuillemier F J 1982 X-Ray and Alomic Inner·Sheli Pnysics (AIP Conf. Proe.) ed B Crasemann, pp 615-32
A N N E X E
IV
J. Phys. B: At. Mol. Phys. 20 (987) 4425-4440. Printed in the UK
Photoionisation and radiative recombination for the rubidium,
copper and silver isoeleetronic sequences
S Wane and M Aymar
Laboratoire Aimé Cotton, CNRS Il, Bâtiment SOS, Campus d'Orsay, 91405 Orsay Cedex,
France
Received 26 February 1987 .
Abstraet. In the framework of a non-relativistic single-electron model, photoionisation
cross sections from 111 states (ft lIIii20, alIIii/ lIIii4) have been computed for the Rb, Cu and Ag
sequences. The evolution of non-hydrogenic behaviour of photoionisation near threshold
is studied along the sequences, and emphasis is put on the occurrence of minima in the
photoionisation cross section curves. Systematic trends along a sequence and the com-
parison of the behaviour along the different K, Rb, Cu and Ag sequences are analysed in
terms of the quanturn-defect theory. Through the principle of detailed balance, scaled
radiative recombination coefficients a~/( T) for Sr'"- y2+, Cu-Ga~+ and Ag_Snl+ have been
obtained within the scaled electron temperature range 500os;; T' '!iÏ 5000 K, and compared
with the corresponding hydrogen resulta. Markedly nen-hydrogenic features and system-
atics of recombination along isoelectronic sequences have been outiined.
1. Introduction
l'hele is a general need for ground- and excited-state photoionisation cross sections
and radiative recombination coefficients in atmospheric and astrophysics, plasma
physics and fusion technology.
In connection with the development of synchrotron radiation sources, laser tech-
nology and various applications of resonance ionisation spectroscopy (Hurst et al
1979), there is a continuing interest in the study of photoionisation processes from
excited atoms, mainly from neutral alkalis (Gilbert et al 1984, Preses et al 1985,
Msezane et al 1986). l'hele are to date very few results on photoionisation of multi-
charged ions owing to the high temperatures necessary to produce these ions in quantity,
and the intensity limitations of a crossed-beam experiment. In addition, experimental
results on radiative recombination are still very scarce. More spectroscopie data for
stripped ions are therefore needed.
On the theoretical side, calculations on excited-state photoionisation havF been
performed mainly for neutral alkali atoms (Lahiri and Manson 1982, 1986, Aymar et .
al 1984), for the transition elements Cu and Ag (Msezane and Lee 1985) and for
Rb-Sr" (Aymar et al 1984). Calculations on radiative recombination have been made
for the alkali atoms Li (Caves and Dalgarno 1972) and Rb (Wane 1985). General
systematic trends of excited-state photoionisation and radiative recombination along
the K sequence have been obtained in a recent paper (Wane and Aymar 1987), hereafter
referred to as I.
Il is highly desirable to extend these previous studies, and outline systematic trends
of excited-state photoionisation and radiative recombination along isoelectronic
0022-HOO/R7/174425+16S02.50
(ê) 1987 IOP Publishinz Ltd
4425
4426
S Wane and M Aymar
sequences of homologous single-valence-electron systems. The atoms Cu and Ag have
a simple ground-state electronic structure: (n -l)dlons 2S I/ 2 (n =4 for Cu and n = 5
for Ag), and a wide range of practical applications in which excited states participate.
In addition, many stripped ions of isoelectronic sequences are found in tokamak
plasmas (Hinnov 1976). Therefore, the isoelectronic sequences of Cu and Ag are weil
suited for investigation.
In this work we present results on excited-state photoionisation cross sections and
radiative recombination coefficients for Cu- and Ag-like ions. In addition, the previous
study on Rb-Sr+ has been completed for other ions of the Rb sequence, in parallel to
the results given for the K sequence in I. Calculations for photoionisation cross sections
within the framework of a non-relativistic single-electron model are perforrned by the
method already employed by Aymar et al (1984). Radiative recombination coefficients
are then deduced by use of the principle of detailed balance, following the procedure
already given by Wane (1985).
The method of calculations is recalled in § 2. The results on the outer-shell
photoionisation cross sections along the ni Rydberg series (n:=s;; 20, 1Ei 3) and along
the sequences are presented in § 4. The systematic trends of the partial photoionisation
cross sections and the evolution of non-hydrogenic behaviour of photoionisation near
threshold are analysed in terms of the quantum-defect theory of Burgess and Seaton
(1960), as indicated in § 3. The results obtained for the radiative recombination
coefficients of Sr+_y2+, Cu-Ga2+ and Ag_In2+ within the scaJed temperature range
500 ~ T' ~ 5000 K are given in § S. Emphasis is put on the non-hydrogenic features,
and systematic trends of radiative recombination along isoelectronic sequences of
single-valence-electron systems are analysed.
2. Methods of calculation of the photoionisation cross sections and radiative
recombination coefficients
The fundamental points and basic theoretical formulae have been given in 1, and the
computational procedures for photoionisarion cross sections and radiative recombina-
tion coefficients recalled. Similar calculations are performed in this work.
Within the framework of a non..relativistic single-particle central-field model the
cross section (in" cm2) for photoionisation of an ni state of a one-electron system is
given in the dipole approximation by (Sobel'man 1972)
-18
(1
2
1+ 1 2
)
(1)
O"nl(E) = 0.855 x 10
(E - Eni)
21 + 1 Rnl,I-I( E) + 21 + 1 Rnl,l+1 (E)
where Eni «0) is the binding energy of the ni electron and E (>0) is the energy of the
photoelectron. The energy of the incident photon is hll = E - Eni (all the energies are
in rydbergs).
The total cross section O"",(E) is the sum oftwo partial cross sections O"nl,l-l(e) and
(J' nl,l+l (E)
respectively associated with the photoelectron continua 1- 1 and 1+ 1 for
l 'F 0, and reduces to (J' nl,/+ 1(s ) for 1=: O.
The radial matrix elements R nl•I :iI; l ( e ) (expressed in atomic units) are given in the
dipole-length formulation by
,R"I,I'(e) = lc:cl Pnl(r)Q(r)P.I'{r) dr
(2)
Pnototonisation and radiative recombination for Rb, Cu and Ag
4427
where Q(r) is the dipole operator; PII/(r) is normalised ta unity and P~I'(r) per unit
energy range.
The radial wavefunctions are calculated using two different central potentials.
(i) Core polarisation efîects are taken into account in the calculations for Cu-Ga2+
and Ag_In2+, according to a method previously given for Rb-Sr+ (Aymar et al 1984).
The central potential used is Ver) = Vo(r) + Vpol(r) where Vo(r) has a simple analytical
fonn depending on three parameters, and the effective polarisation potential Vpol(r)
depends on the static dipole polarisability of the core and a parameter-the effective
core-radius eut-off, The parameters are determined by comparing the experimental
energies with zero-order calculated values. In addition, the radial matrix elements
(equation (2» are calculated using a modified dipole operator Q(r) which includes
the effects of core polarisation.
(ii) For the other ions of the sequences where only few experimental energies are
available, the central potential used corresponds to the parametric potential introduced
by KJapisch (1971). This potential already used in 1 is represented by an analytical
function depending on a set of parameters determined by minimising the total energy
of the ground state. Without core polarisation effects, Q( r) reduces to the usual r
operator (equation (2».
The radiative recombination rate coefficient all/( T) is obtained through the principle
of detailed balance (Bates and Dalgamo 1962, Barfield 1979) by
all/( T) = (3286.3402)2(21 + 1)(kT)-3/2 t'Xl (e + 111/)2u III,( e) exp( e] kT) de
r -
(3)
where k is the Boltzmann constant and T the electronic temperature; e is the electron
kinetic energy which satisfies h,,:= e + III" where 1111 is the ionisation potential of the
captured electron and h" the energy of the emitted photon in the process of radiative
recombinatien. Ali the energies are expressed in Ryd and all/(T) is expressed in cm' s-1.
3. Quaotum-defect theory aoalysfs of excited-state photoiooisation
Systematic trends of partial photoionisation cross sections for non-hydrogenic atoms
or ions have been analysed recently in l, in terms of the quantum-defect theory of
Burgess and Seaton (1960). A detailed discussion on the behaviour of cross sections
along a sequence compared with the hydrogen one has been given. This comparison
was carried out using scaled energies e' = si Z2 and scaled cross sections u'(s') =
u(Z2
Z2
e' ) where Z =Z - N + 1 is the residual charge of the final ion. Only some points
of the analysis will be mentioned.
For hydrogen the radial matrix elements R ~I,I'( e') are always monotonically decreas-
ing functions of e'. Then the photoionisation cross sections <7'~I,I'(s') and U~(E') are
maximum at threshold and drop to zero as e' increases. For 1" 0, the ratio
<7'~I,I-l(e')/<7'~I,I+l(e') is always smaller than 1 and increases with n. For a given nl
series, threshold values 0"~1,1I1'(0) and u~(O) increase with n.
For non-hydrogenic atoms or ions the behaviour of cross sections can differ strongly
from that for hydrogen. Zeros in radial matrix elements RIII,I·(e') may occur as e'
increases, giving up to three minima in <7'~I,,.(e') curves, In fact, both bound and
continuum orbitais are contracted and shifted towards the nucleus with respect to
hydrogen-Iike orbitais, owing ta the non-Coulomb forces that prevail within the core.
4428
S Wane and M Aymar
The relative shift of the two orbitais with respect to each other is responsible for the
non-hydrogenic character of photoionisation.
The quantum-defect method brings out an oscillatory dependence of Rn/,,,(e') on
""ni and 8,,( E') such as cos[ 1TÂ n/,,,( E')] with
ÂnI,I·(e') = -""ni + 81'(e')/ 1T+XII'(n, e')
(4)
where "",t! is the quantum defect of the ni state, and 8,,(e') the phaseshift of the
continuum orbital with respect to hydrogen-like wavefunctions. The empirical para-
meter X is a slowly increasing function of n and e' (Peach 1967). The occurrence of
zeros in R"/.,,(e') is related to half-integer values of Ân/,,,(e').
Near the threshold, an approximate value of Ân/,,,(e') can be obtained by using in
equation (4) the limiting values obtained for n =00 and e'=O:
Â"I.,,(e') =- ÂJ.'II·+XII'(O)
(5)
where the asymptotic value X(O) of X can be extracted from the tables of Peach (1967).
The quantity ÂJ.'II' = J.''' - J.'I represents the quantum-defect difference for large n values.
A eritieal quantum-defeet differenee ÂJ.'~' for the zero of R nl,/( s ') to oecur is defined
by the relation
Â",,~.+ Xw(O) = ±0.5.
(6)
The shape types (a) ~ (e) of (J'~t.r( s ') depend on the difference 1ÂJ.'II'I-I ÂIJ. ~·I (figure
1), the number k of zeros being determined by the inequalities
IÂJ.'~·I + k -1 < IÂJ.'wl < IÂIJ.?,.I + k.
(7)
o
1l1\\lI/'1
1
1
1l1\\l1/11
o
Flpre 1. Schematic cross section curves for live typical cases and number of minima
according to relative values of ~IJ./I"
4. Results for excited-state pbotoionisation cross sections of Rb-, Cu- and Ag-like ions
Photoionisation eross sections have been eomputed for ni series (n =si 20, 0 ~ 1:EO 4) of
Cu-Mo IH , Ag-Xe7+ and y2+_Xe I7+ in addition to the results already given for Rb-Sr+.
Only the photoionisation of the outer ni electron is considered and autoionisation
effects are ignored. The validity of this treatment is confined to the near-threshold
energy. Nevertheless caleulations are performed for higher photoelectron energies in
order to deteet the various minima occurring in (J'~/,/·(e') curves, and analyse the
systematics of these minima.
4.1. Isoelectronic variations of quantum defects
The asymptotic quantum differences ÂJ.'II' are given for eaeh ni ~ e'l' transition in table
1 for Cu-like ions, in table 2 for Rb-Iike ions and in table 3 for Ag-like ions.
Phototontsation and radiative recombination for Rb. Cu and Ag
4429
Table 1. For a given ni .. E' l' transition, compilation of t"JJ. 1,. and t"JJ.1I' values, and the
shape type of O'~,.,.( E') cross section curve for each element of the Cu sequence.
Elements
Transition
Cu
Zn+
Ga 2+
Ge3+
As4+
SeH
8r6+
Kr7+
ns" E'p
-0.54 -0.39
-0.33
-0.30
-0.27 -0.25
-0.23
-0.22
(c)
(b)n"'8
(b)n"'4
(a)
(a)
(a)
(a)
(a)
(c) n'-9
(a) Il.-5
np~ E'S
0.54
0.39
0.33
0.30
0.27
0.25
0.23
0.22
(a)
(a)
(a)
(a)
'(a)
(a)
(a)
(a)
np~ a'd
-1.02 -0.87
-0.74
-0.62
-0.56 -0.51
-0.47
-0.43
(c)
(c)
(c)
(c)
(c)
(b)n'lllii4
(b)nll!iii5
(b)n"'10
(c)n"'5
(c) n'-6
(c)lI;;,l1
nd .. s'p
1.02
0.87
0.74
0.62
0.56
0.51
0.47
0.43
(c)
(c)
(a)n'lllii13
(a)
(a)
(a)
(a)
(a)
(b)14'l11iin"'16
(c)II;;,17
nd .. e T
-1.05 -0.92
-0.86
-0.78
-0.72 -0.66
-0.61
-0.56
(c)
(c)
(cl
(c)
(c)
(b)n1l5O;4
(b)n'lllii5
(b)n1l5O;7
(cln"'5
(c) n;;,6
(c) n;;,8
nf .. e 'd
1.05
0.92
0.86
0.78
0.72
0.66
0.61
0.56
(c)
(c)
(b) n"'5
(a)n"'9
(a)
(a)
(a)
(a)
(c) n =-6
(b)10'llliin1l5O;13
(c)II'-14
nf .. E'g
-0.01 -0.01
-0.02
-0.02
-0.03 -0.05
-0.06
-0.07
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
Elements
Transition
Rb8+
Sr9+
ylO+
Zrll+
Nbl2+
Mo13+
t"JJ. ~.
ns" e 'p
-0.20
-0.19
-0.18
-0.18
-0.17
-0.16
-0.37
(a)
(a)
(a)
(a)
(a)
(a)
np~ E'S
0.20
0.19
0.18
0.18
0.17
0.16
0.71
(a)
(a)
(a)
(a)
(a)
(a)
np~ e'd
-0.41
-0.38
-0.36
-0.34
-0.32
-0.31
-0.42
(b)n1l5O;16
(a) Il 1150; 7
(a)
(a)
(a)
(a)
(c)n;;,17
(b)8 ... n1l5O;19
(c) n;;a20
nd~ e'p
0.41
0.38
0.36
0.34
0.32
0.31
0.75
(a)
(a)
(a)
(a)
(a)
(a)
nd~ ef
-0.52
-0.48
-0.45
-0.42
-0.39
-0.37
-0.48
(b) n"9
(a)n'lllii4
(a)n"'5
(a)n"'8
(a)
(a)
(c)n"'10
(b) 5.. n1l5O; 12
(b) 6 'l11ii n "' 18
(b) n;;,9
(c)n=-13
(c)n"'19
nf .. E'd
0.52
0.48
0.45
0.42
0.39
0.37
0.78
(a)
(a)
(a)
(a)
(a)
(a)
nf- E'g
-0.08
-0.09
-0.10
-0.11
-0.11
-0.11
(a)
(a)
(a)
(a)
(a)
(a)
t~o
Table 2. The same as table 1 for the Rb sequence.
C'l
~
Elements
::s
111
Q
Transition
Rb
Sr+
yH
Z~+
Mo H
Tc6+
Rh8+
AgIO+
In 12+
Sb l 4+
Te l H
Xe l 7+
A~~.
::s
~
~
ns'" e'p
-0.48
-0.37
-0.32
-0.29
-0.25
-0.23
-0.21
-0.19
-0.17
-0.16
-0.15
-0.14
-0.37
(c)
(b)nE;12
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
~
'<
(c) n-= 13
:J
Q
.,
np'" e's
0.48
0.37
0.32
0.29
0.25
0.23
0.21
0.19
0.17
0.16
0.15
0.14
0.71
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
np'" s'd
-1.34
-0.88
-0.70
-0.61
-0.51
-0.47
-0.41
-0.37
-0.33
-0.31
-0.29
-0.28
-0.42
(c)
(c)
(c)
(c)
(c)
(b)n0>;6
(b)nO>;I4
(a)nO>;I1
(a)
(a)
(a)
(a)
(c)n~7
(c)n~15
(b)n~12
nd ... s'p
1.34
0.88
0.70
0.61
0.51
0.47
0.41
0.37
0.33
0.31
0.29
0.28
0.75
(c)
(b)nE;4
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(c)n Si05
nd ... e'f
-1.29
-1.33
-1.23
-1.03
-0.80
-0.72
-0.59
-0.52
-0.45
-0.41
-0.39
-0.35
-0.48
(c)
(c)
(c)
(c)
( c)
(b) n0>;4
(b)n""6
(h) n 0>;9
(a)n0>;4
(a) no>; Il
(a)
(a)
[c] n;;.,5
(c) n~7
(c)n~IO (b)50>;no>;I6
(b)n;;"12
(c)n~17
n(... e'd
1.29
1.33
1.23
1.03
0.80
0.72
0.59
0.52
0.45
0.41
0.39
0.35
0.78
(c)
(c)
. (c)
(c)
(b)nO>;IO
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(c)n~11
nf... e'g
-0.02
-0.10
-0.15
-0.25
-0.29
-0.30
-0.29
-0.27
-0.26
-0.24
-0.23
-0.22
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
T"" J. The same as lable 1 for Ihe AS sequence.
)e
-e
Elements
o'
:1
tj.
Transilion
AI
Cd+
InH
Sn)+
Sb4+
TeH
16+
Xe1+
~#oi~.
I:l
-
O'
:1
"S~s'P
-0.53
-0.37
-0.32
-0.29
-0.27
-0.25
-0.24
-0.22
-0.37
I:l
(c)
(b) Il E; 14
(a)
(a)
(a)
(a)
(a)
(a)
:1
~
(c)II~15
è3
IIp~S'S
0.53
0.37
0.32
0.29
0.27
0.25
0.24
0.22
0.71
~
(a)
(a)
(a)
(a)
(a)
(a)
(a)
(a)
i:i'
-.
"p~s'd
-1.01
-0.85
-0.74
-0.62
-0.56
-0052
-0.48
-0.45
-0.42
-
e~
(c)
(c)
(c)
(c)
(c)
(b)IIE;5
(b)nE;6
(b)nE;8
~
(c)n~6
(c) n;;JI7
(c) n ~9
l")
e
"d~s'p
1.01
0.85
0.74
0.62
056
0.52
0.48
0.45
0.75
:J
(c)
(b)nE;5
(a) 5E; nE; 14
(a)
(a)
(a)
(a)
(a)
0-
-.
:1
(c)n;;JI6
(b) ISEi Il tE; 18
I:l
-.
(c)II~19
-
e
IId~ s'f
-2.04
-L79
-1.57
-U5
-1.09
-0.90
-0.80
-0.72
-0.48
:1
(e)
(e)
(d)IIE;8
(c)
(c)
(c)
(c)
(c)
'0>
...
(e)II"'9
:lO
IIf~ E'd
2.04
1.79
i.S7
US
1.09
0.90
O.SO
0.72
0.78
~O-
(e)
(c)nE;7
(c)
(c)
(c)
(c)
(b) Il tE; 10
(a)
Q
(d)8E;nE;1l
(c) n;;JIll
I:l
(e) n"'12
:1
~
IIf~ s's
-0.01
-0.06
-0.13
-0.27
-0.43
-0.54
-0.55
-0.55
~
(a)
(a)
(a)
(a)
(a)nE;12
(a) nE; 6
(a)IIEi6
(a)nE;S
OQ
(b)n~13
(b)7 Ei Il tE; 12
(b)7E;n~12
(b)6E;n""12
(c)II;;J113
(c)II;;J113
(c) Il ~ 13
s
-
4432
S Wane and M Aymar
The isoelectronic variation of the ÂIJ./I' quantities is related to the evolution of the
IJ.I quantum defeets. The dependence of calculated asymptotic quantum defects IJ.s.
J.'p, J.'d and J.'( (J.'nh n ~ 00) on z and on the sequence (K, Rb, Cu and Ag) is displayed
in figure 2. The isoelectronic variation depends strongly on the 1 value (Edlèn 1964).
For small 1 (s, p), the quantum defect J.'n' mainly due to the penetration of the ni
orbital in the core decreases as z inereases. Core polarisation effeets are responsible
for most of the qua~1tum defeet J.'n' for large 1 (f); for those non-penetrating orbitais
J.',tI tirst increases with z, then passes through a maximum and ultimately decreases.
As discussed by Manson (1969) the quantum defect of nd states depends strongly on
the element, due to the existence of potential barriers in the effective potential seen
by the d electron of particular elements. As visible on figure 2 the isoelectronic variation
of J.'d for K and Rb differs ~t low z from that observed for Cu and Ag. fxcept in the
low z range, the continuous decrease with z results from the penetration of the orbital
in the core. The evolution with z of the asymptotic quantum-defeet differences is
drawn in figure 3. The three sets of curves IJ.s. J.'p and J.'d (z ~ 3) are very similar (figure
2), the gaps between successive curves of a given set being close to the gaps between
the curves of another set. Thus ÂlJ.sp and to a lesser extent ÂlJ.dp do not depend much
on the sequence. Let us note that the curves corresponding to the Rb. Cu and Ag
sequences are almost superimposed. Similar behaviour does not remain for ÂlJ.dr and
ÂlJ.rg due to the very different evolutions of J.'d and IJ.f with z.
2.2 1"'"1- - - - - - - - - - . ,
2.01 - ,
::1 ~\\
~I ~\\,,'
"Il
~d /-'~A9
1
1
~
1&.
""
1
2.0
'
.
"
l
' , A g
2.0""
' , A g
,
...
"
1:1~
-,-.
...................
l "-......
................
Rb
1.0 i
(dl i
..••...•....••••
'--_~~~ 1.0
......•..•.•••.•..•..••••~=}~
10
I!t
~~~----~b
1
1
...............- ••~
0.3 1'---_ _- - _ - _ - '
01 ~......
Cu 1
0.6o
5
10
15
0
5
10
15
5
10
15
z
z
Fleure 1. Asymptotic quantum de{eet !J.l along a sequence ploned against the residual
charge z for (a) !J.•• (b) !J.p • (C)!J.d and (d) !J.r-
These general remarks will allow us to analyse the systematics of photoionisation
along a given sequence, and to compare the new results obtained for the Rb, Cu and
Ag sequences with those already given for the K sequence in I. It will be shown that
for low 1(s, p) the isoeleetronic variation of the (T~I,I·(E') cross sections is quite regular.
Moreover similar behaviour holds for the four sequences K, Rb, Cu and Ag. In
contrast, for f states non-hydrogenic features appear only for highly ionised ions of
the Ag sequence. Photoionisation from d states corresponds to an intermediate situation
detailed later in § 4.2.3.
4.2. Systematics ofphotoionisation cross sections of excited states of Rb, Cu and Ag-like
ions
The shape type of each (T~I,I'(e') curve is given for each nl ... s'l' transition in tables
1-3 for Cu-, Rb- and Ag-like ions. In the same tables, the asymptotic quantum
Photoiontsation and radiative recombination for Rb, Cu and Ag
4433
1.6
,
(al
0.8....-----..l.-----....J-------&.-,
\\
Shape(c)
IcI
~ 1.0
...
:1.
<l
Cu,Rb,Ag
0
-----"-'--._------~----------
K
2.0
lbl
Shape (el
o
5
10
15
IA~fl+1
z
Shape tc)
.......-••,-
---h (
-------------_..â..ape al
o
s
10
1S
z
Figure 3. Asymptotic quantum-defect difference ~p.". along a sequence plotted against the
residual charge z for (a) ~P.dp. (b) 1.1loLdr/. (c) 1~IoL.pl and (d) ;~loLr.l. The elements with
O'~d.I'(E') of shape type (c) are denoted by full circles and those with O'~d.r(E') of shape
type (e) by crosses in (a) and (b).
differences Â#-,I/' are compared with the critical asymptotic values Â#-,?,' (equations (5)
and (6) derived from the tables of Peach (1967). These Â#-' ?" vaiues accurately describe
the occurrence of minima in the photoionisation cross sections of Cu-, Rb- and Ag-like
ions. This point is illustrated in figures 3(a) and (b ) corresponding to the nd-+ e'p
and nd -+ s'f transitions. Indeed, the horizontallines in figure 3(b) separate three zones
ccrresponding respectively to shapes (a), (c) and (e) (see figure 1). Simiiarly one has
two zones in figure 3(a).
The elements with U~d.l'( s') of type (c) (for large n) are denoted by fun circles and
those with U~d.f(S') of type (e) (for large n) by crosses. The circles and crosses are
located in the right zones of figures 3( a) and (b).
These figures only iIlustrate the shape of u~,,r(e') for large n values. The Â#-,u' and
Â#-,?,' quantities involved in inequalities (7) correspond to asymptotic values.
For
low-lying levels the #-'"' can be different from the limiting value for n =oc; moreover
the XII·(n, s') function (equation (4» is also different from its asymptotic value. When
IÂpolI,1 :lie IÂpo~,1 + k --1 the critical value for k zeros is only reached for highly excited
states, and a change of shape in the U~I,I'( e') curves occurs for a given series as n
increases. Let us note that the changes from u~ol,,'(s') oftype (b) (or (d» to u("o+I)I,"(s')
of type (c) (or (e) correspond to a displacement of the minimum from below to above
the ionisation limit. The corresponding values at threshold U~I,I'(O) and u("o+I)I,"(O)
are generally particularly small.
The systematics of excited-state photoionisation will now be illustrated for s, p, d
and f states.
4.2.1. ns series (n:fié 20J. Figure 4 shows the evolution with n of the threshold values
O'~.(O) along the three sequences. Since for a given z the Âpoep is almost independent
of the sequence, the three sets of curves are very similar. The O'~.(O) values of neutral
,------------------------
4434
S Wane and M Aymar
10
1
1
l
'
10-3
r
j
1
1
1
1
1
L i~
_ _ '
4
6
8
10 12 14 16 18 20
4
6
8
10 12 14 16 18 20
4
6
8
10 12 14 16
18 20
n
n
n
Filure 4. Scaled total cross sections at threshold (]'~.(O) (in Mb, 1 Mb =10-18 cm~) plotted
against n along the (a) Cu sequence, (b) Rb sequence and (c) Ag sequence.
atoms (type (e» and those of the first ions of the sequences (types (b), (c) differ from
hydrogen ones, owing to large cancellation effects in the radial matrix elements
R"s.p(E'). The pronounced minima observed for Zn+, Sr" and Cd+ correspond to the
change of shape from (b) to (c) along their respective ns series. For highly ionised
ions (z ;a: 3) the cross sections move progressively to hydrogen ones along the sequences.
The evolution ofsimilar C1'~1(0) along the K sequence (see 1figure 2(4» is very similar,
but the C1'~s(O) curve of Ca+does not exhibit any minimum (in the range n 1ER 20) because
aIl the C1'~s(E') curves are there of type (b).
4.2.2. np series (n 1ER 20). Figure 5 shows the evolution with n of the threshold values
C1'~p(O) along the Ag sequence. which are of the same order of magnitude as hydrogen
values, for the lower members. The value of C1'~p( E') depends upon the relative weight
of C1'~p••(E') and C1'~P.d(E') which depends strongly upon n and the element considered.
In many cases one has C1'~p.d(E') < C1'~p,.(E'); thus the cross sections do not move
progressively to the hydrogen values along the sequence. Analogous behaviour holds
for K (see 1, figure 3(a». Rb and Cu sequences due to the similarity between the Ap.p,
and Ap.pd values for the four sequences.
4.2.3. nd series (n E; 20). A new feature, compared with the K sequence. is the presence
of minima in the partial cross section curve C1'~d.f(e') for highly ionised ions (z =13
for Rb sequence); moreover the C1'~d.f(E') of the first members of the Ag sequence have
two minima (type (e». This is clearly related to the large AP.df values obtained for
heavy elements (see figure 3(b».
Figure 6 displays the evolution with n of threshold values C1'~d(O) along the three
sequences (Rb. Cu and Ag) and clearly shows the large difference between the
sequences. The occurrence of new minima in the C1'~d.f( E') curve of In2+ (change from
Photoionisation and radiative recombination for Rb, Cu and Ag
4435
Ag-like
10'
:a
z:
ô
lL
~c::
a
10
4
6
8
10
12
14
16
18
. 20
n
Fllare 5. Scaled total cross sections at threshold O'~p(O) plotted aginst " along the Ag
sequence.
103 r----~--~--.....,
:a
J:
ê 10 'l"I--~'
...
-c::
a
4
6
8
10 12 14 16 18 20
4
6
8
10 12 14 16 ·18 20 4
6
8
10 12 14 16 18 20
n
n
n
Flpre 6. The same as figure 4 for (7'~d(O).
shape (d) to shape (e) for n =8) explains the minimum visible on figure 6(c). For
Rb and Cu sequences the minima occurring for highly ionised ions correspond to the
change of shape (b) to (c). Let us recall that the homologous minima occurring in
the K sequence concern the Ca+- y4+ ions.
The relative weight of O'~d.p(E/) and O'~d,r(E/) depends strongly upon n and. the
element considered; thus the evolution towards the hydrogen values of O'~d(e') is not
regular for any sequence. Furthermore the O'~d(e') curves exhibit minima corresponding
to those of O'~d.r(e') curves, particularly for the lower members of the sequences, e.g,
for Rb-Zr.3+ and Ag_Sn3+.
4.2.4. ni series (n .. 20). The A~~. value corresponding to the occurrence of one
minimum in the O'~r..(B') curve cannot be obtained from the tables of Peach (1967),
which are restricted to transitions between small 1values, 1~ 3. However from tables
4436
S Wane and M Aymar
1-3 and figure 3(d) one can assume that 1~J.&.~81 =- 0.55, because minima occur only for
highly ionised ions of the Ag sequence. The total cross section O'~r( E') depends mainly
on the partial cross section O'~r.a<E') and the zero occurring in O'~r.d(E') does not mueh
affect O'~f( s'). So for the K (sec 1), Rb and Cu sequences the O'~f( s') values are not
very ditIerent from the hydrogen values. Non-hydrogenic features observed in the Ag
sequence are illustrated by figure 7, which shows the evolution of O'~'r(E') along the
Ag sequence (figure 7(a», and the evolution with n of the threshold values O'~r(O)
(figure 7(b». The curve 0'~5r(B') is of type (c) as is O'~'r.a<E') for higher members
Tes+-Xe7+, but only of hydrogen-like type (a) for lower members Ag-Sb4+. The minima
shown in O'~r(O) for n =12 correspond to the change of shape (b) to (c) along the nf
series of elements.
For comparison with previous work the only available results concem the ground
state of Cu-Zn+ and Ag obtained with the pseudopotential method (McGinn 1970),
and the lower excited nd states Cu 4d-5d and Ag 5d obtained with the Hartree-Fock
fonnulation (Msezane and Lee 1985). Near-threshold values given by McGinn for
Cu 45 and Ag 5s are much larger than ours and his predicted minima much farther
from the threshold, whereas we both find cross section values of the same order for
Zn+ 45. The threshold values given by Msezane and Lee, 0'4<1(0) = 16.62 Mb and
O'Sd(O) = 33.47 Mb for Cu, and O'Sd(O) ::: 14.97 Mb for Ag from the Hartree-Fock length
formulation are less than but of the same order as ours (respectively 20.84 and 39.48
for Cu, and 20.19 for Ag). Moreover, we predict the same number of minima although
our predicted ones are much farther from the threshold th an their minima. When
caneellation occurs in radial transition matrix elements, resulting in minima in the
photoionisation curves, theoretical results are extremely sensitive to the details of the
laI
10'
10
10
~
:z:
~
§
... ~
-;:
Q
Q
o
0.02
0.04
0.06
0.08
4
6
8
10
12
14
16
18
20
C' IRydl
n
Flpre 7. (a) Sca1ed total cross sections Q'~,r<e') aloDg the Ag sequence ploaed a,ainst
the scaled pbotoelectron energy .' (in Ryd). (h) Scaled total cross sections at thresbold
Q'~r<O) along the Ag sequence ploued apinst n.
Photoionisation and radiative recombmatton for Rb, Cu and Ag
4437
initial- and final-state wavefunctions. In such cases, more sophisticated models are
often required to obtain accurate predictions. These models are however not suited
for extensive ca1culations whereas the central potential model, which reproduces weil
the qualitative features of the photoionisation process, is weil adapted for an extended
analysis of systematic trends.
5. Radiative feCOlDbiutioa rate coefticieats for the Rb, Cu aad Ag isoeledroaic
seqaeaces
Radiative recombination rate coefficients a",( T) have been calculated for the recombin-
ing ions Cu+-Ga.l+, Ag+-Irr'" and S~+- y3+ in addition to the results already given
for Rb+ (Wane 1985). The scaled coefficients a ~,( T') =artI( :2T)J z (with T' = TJ:2,
z being the charge of the recombining ion) are compared with those for hydrogen.
The autoionisation effeets are disregarded in the calculation of photoionisation cross
sections. Consequently, the computation of the radiative rate coefficients is restrieted
to the scaled temperature range 5oo:Et T':Et Sooo K which confines the efficientelectron
energy range closer to the threshold the lower the temperature.
.5.1. Evolution of a ~,( T') with n for given 1and T'
The evolution with n of sorne particular a~,( T'). 'r~ 2, at the fixed- temperature
T' =SOO K is shown in figure 8 and compared to the corresponding one for hydrogen.
Three typical non-hydrogenic features, already encountered in the K sequence (l), are
visible on the figure.
Firstly, the curves a ~I of the three neutral elements as weIl as a ~d of Cd" present
a maximum for no =5 or 6. In aIl cases, this maximum is due to the very small value
of O"~_l.'(O) compared with O'~,(O) (see figures 4 and 6(c».
..······..Rb-like
'--- Cu-lilce
_._.- Ag-Iike
10.12
10.12
lbl Ag-like
(cl Ag-like
Ag
10.1)
10-1l~
",,/
H
i
Cd·
1
,
1
SnJt
'",
..
ut
!
In2+
~ W14
"'s 10-1I.J
, t
es
~ 11
1
10-15
10-15 ,
11
10-16
10-16
4 6
8 10 12 14 16 18 20
n
" 6 8 10 12 14 16 18 20
n
n
Flpn Il. Scaled radiative recombination coefficients a~, (in units of cm3 s-') ploned
Il.
alainU /1 at a scaled temperature T. '00 K for. (CI)
series alons the Cu. Rb and AI
sequences; (b) "p series &Ions the AI sequence; (c) "d series alonl the AI sequence.
4438
S Wane and M Aymar
Secondly, the a~s coefficient of Zn+ and the a~d of In2+ present a minimum for
no = 10 followed by a maximum. This irregular n dependence is closely related to that
of the (7'~/(0) values shown in figures 4(a) and 6(c). Let us note that a similar minimum
and maximum occur for a~s of Sr" and Cd" for temperatures less than T' =500 K.
The third characteristic non-hydrogenic trait of a~, coefficients is displayed by the
a ~P coefficients of the first members of the Ag sequence. While the a ~s and a ~d
coefficients shown in figure 8 are much smaller than the a~, the a ~P are greater than
a ~P' In fact in the former case, near the threshold (7'~,( e') « (7'~( s ') whereas in the
latter case O'~p( e') ~ O'~p( s '). Moreover the decrease of O'~p( e') with e' is slower than
in the hydrogen case, and the large values of the ionisation potentials !"p give a higher
weight to the factor (e + l"p)2 occurring in equation (3). The a~d of Ag has the same
behaviour as the a ~p.
A last remark results from figure 8(a). The curves corresponding to the a ~s of
neutral atoms are grouped for large n values; similar groups occur for singly and
doubly ionised ions, stressing once more the great analogy between the O'~s( s') of the
three sequences corresponding to a given z value.
5.2. Evolution of a ~,( T) with T for n and 1fixed
For given n and l, the coefficient a ~,( Tf) generally decreases monotonically with
increasing temperature T' as a~( T'). Departures from this behaviour are illustrated
in figure 9 for a~s(T) of Zn+ and a~d(T') of In2+. The unusual evolution with T'of
the a~s (n;a= 12) of Zn+ and aiOd of In2+ is related to the evolution with e' of the
corresponding O'~/(e'). Indeed the efficient energy range increases with T; when a
5
6
10-17
In2+
10-19
10-1
0
1000
2000
3000
4000
5000
0
1000
2000
3000
4000
SOOO
ri (KI
r (KI
Fipre 9. Scaled radiative recombination coefficients ploncd against the scaled temperature
t: (in K): (a) a~.(r) for Zn+; (b) a~d(T) for In2+.
Pnototonisation and radiative recombination for Rb, Cu and Ag
4439
sufficiently pronounced maximum of (]'~/(e') occurs within this range the coefficient
a ~/( T') presents a maximum. The ratio of the maximum of (]'~/(s") to either (]'~/(0) or
the non-zero minimum of (]'~/(e') is strongly n-dependent and thus sorne a~ values
are affected much more than ethers. Let us note that at high termperatures, eventually
out of the range represented here, the a~/( T') finally decreases with increasing T'.
Similar behaviour holds for a ~s( T') of Sr+ and Cd+, and for a~,{ T') of high members
of the Ag sequence (Z;lr 6). Let us note that departures from a monotonie decrease
with T' have been observed in the K sequence (1), but there the a~/(T) curve was
less tortuous than in figure 9.
6. ConciusioDS
In this work, we have performed calculations of excited-state photoionisation cross
sections and radiative recombination coefficients along the Rb, Cu and Ag sequences.
The results are compared with those previously obtained for the K sequence (Wane
and Aymar 1987) and the systematics of photoionisation are analysed in terms of the
quantum-defect theory. Near-invariance is found for the isoelectronic variation of
photoionisation from ns and np states along the four sequences. At the opposite
extrerne, the isoelectronic behaviour ofphotoionisation from nd and nf states is strongly
dependent on the sequence. New markedly non-hydrogenic features appear with
increasing Z
Thus more minima occur in the partial cross section curves of heavy
elements, e.g. one minimum for the (]'~f,,<e/) and two minima for the (]'~d.r<e') occur
for some ions of the Ag sequence only. Moreover, minima occur for relatively highly
ionised ions, and even appear for the higher members while absent for the lower
members along the Ag sequence. In addition, some of the radiative recombination
coefficients exhibit marked minima and maxima in the evolution with temperature
within the range considered, due to sufficiently high maxima in the corresponding
photoionisation cross section curves. The very irregular and tortuous shapes they have
herein was not observed in the K sequence.
Acknowledgment
The authors wish to thank Ors E Luc and 0 Robaux for fruitful discussions.
References
Aymar M, Robaux 0 and Wane S 1984 J. Play$. B: At. MoL Plays. 17993-1007
Barfield W D 1979 Astrophys. J. 229 856-66
Bates D Rand DaJsamo A 1962 Atomic and Mo/ecu/ar Processes cd 0 R Bates (New York.: Academie) ch 7
Burgess A and Seaton M J 1960 Mon. Not. R. Astrolt Soc. 120 121-51
Caves T C and Dalgamo A 1972 J. Quant. SpeClroSC. Radial. Transler Il 1539-52
EdJèn B 1964 HlUldbuch der Playsik vol 27 SpectrOscoPY (Berlin: Springer) pp 80-220
Gilbert S L. Noec:ker M C and Wieman C E 1984 Plays. Rev. A 19 31.50-3
Hinnov E 1976 PfJys. Rev. A 1. 1533-41
Hurst G S, Payne M 0, Kramer S D and VounS J P 1979 Rev. Mod. Plays. 51 767-819
KJapisch M 1971 Comput Plays. Commult 2 239-60
4440
S Wane and M Aymar
Lahiri J and Manson S T 1982 Phys. Rtv. urt. 48 614-6
-
1986 Phys. Rtv. A 33 3151-65
Manson S T 1969 Phys. Re»: 18197-103
~,
__<
McGinn G 1970 J. Chem. Phys.53 3635-40.
--
v.\\Cil,/ \\IEer/~
Msezane A Z, Lahiri J and Manson S T .
A ,~
Msezane A Z and Lee J 1985 J. Pitys.
~1.
oL Pitys. 1 3
Peach G 1967 Mm&. R. ASII'On. Soc. 71
- 7CAM E
Pressca J M, Burkhardt C E, Corey R ~ E.lmmn'"f)-1:::--9ftol
A Z and Manson ST 1985 Phys.
....,
321264-6
Sobel'man 1 1 1912 An Introduclion 10
~>
Wane S 1985 J. Phy!. B: At. Mol. Phys. 18
Wane S and Aymar M 1987 J. Pitys. B: AI.
-,
....
APPENDICE
à la THESE présentée pour l'obtention du grade de
DOCTEUR ES SCIENCES
par
Sada Tamimpu WANE
ORSAY
1988
DEFAUTS QUANTIQUES, ELEMENTS DE MATRICE DIPOLAIRES
ET SECTIONS EFFICACES DE PHOTOIONISATION
Appendice 1
séquence de K
Appendice 2
séquence de Rb
Appendice 3
séquence de Cu
Appendice 4
séquence de Ag
Pour chaque é1ement, les états n1 sont classés par valeur croissante de 1
et pour chaque 1 par valeur croissante de n.
Pour chaque état n1, la première ligne précise
Ncm de l'é1ement.
NL
état initial nl.
EO
valeur théorique du potentiel d'ionisation -E:nl "
*
N*
nolllbre quantique effectif n
de l'état ei •
MU
valeur théorique du défaut quantique Pn1.
Les valeurs tabu1ées concernent :
E
énergie E: du photoé1ectron en Rydberg ou eV.
E PHOT
énergie du photon incident en eV.
0
LAMBDA
longueur d'onde du photon incident en A.
.
(L/R/L/ ± 1)
éléments de matrice dipolaires de transition ~1, 1 ± 1 (e:) en u , a.
SIGMA L ± 1 : sections efficaces partielles de photoionisation a
, 1 ± 1 (E:) en
n1
Mb (1Mb. 10- 18 cm2).
SIGMA
sec t ion eff icace totale de photo ionisation 0'nl, (E:) en Mb·.
1
j
1
,
- ------.....
K
45
EO· 3.0370E-Ol
IAYD)
N·· 1.8148
MU·
2. 18114
E IAYD)
E lEV)
E PHOT lEV.
LAMBDA
lA)
(L/R/L-l)
(L/R/L"')
SIGMA L - 1
SIQMA L"1
SIQMA
(MB)
.0000
.000
4.132
3000.54
.000
-3. 72!5E -0 1
.000
3.802E-02
3.1I02E-02
.0200
.272
4.404
2815.15
.000
- 1 . 750E -01
.000
8.472E-03
8.472E-03
.0400
.144
4.11711
211111.34
.000
-2.1I00E-02
.000
1 .118 7E - 04
1.887E-04
.0800
.818
4.848
2105.114
.000
8.703E-02
.000
2.31IlE-03
2.3151-03
.0800
1.088
5.221
2374.84
.000
1.731E-Ol
.000
8.834E-03
8. 834E -03
.1000
1.3111
5.483
22117.2&
.000
2.388E-Ol
.000
1.11118E -02
1.1188E-02
.3000
4.082
8.214
150tl. 47
.000
4.178E-Ol
.000
Il.008E-02
8.0081-02
.4000
5.442
8.1175
1284.88
.000
4.032E-Ol
.000
8.781E-02
8. 78U -02
.5000
Il.803
10.1135
1133.84
.000
3.7117E-Ol
.000
8.750E-02
Il.750E-02
1.0000
13.1108
17.738
.8'.88
.000
2.538E-Ol
.000
7.188E-02
7. 188E-02
K
55
EO·
1. 2442E-Ol
«AYD)
N·· 2.8350
MU-
2.11150
E (AYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L"')
SIQMA L- 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
1.883
7324.211
.000
-1.7111E"00
.000
3.301E-Ol
3.301E-Ol
.0200
.272
1 .81115
113011.84
.000
-a.1I18E-Ol
.000
Il.172E-02
Il.172E-02
.0400
.544
2.237
sa42.38
.000
-3.448E-Ol
.000
1.1172E-02
1 .1I72E -02
.0800
.8111
2.508
4841.32
.000
-3. 487E -02
.000
1.1128E-04
I.UBE-04
.0800
1.088
2.781
4457.87
.000
1.557E-Ol
.000
4.237E-03
4.237E-03
.1000
1.3111
3.013
40110.1111
.000
2.74I1E-Ol
.000
1.44I1E-02
1.448E-02
.2000
2.721
4.414
2808.83
.000
4.3111E-Ol
.000
5.348E-02
1.348E-02
.3000
4.082
5.775
2147.10
.000
4.085E-Ol
.000
Il.084E-02
Il. 084E -02
.4000
5.44;
7.1311
1737.118
.000
3.1l70E-Ol
.000
5.713E-02
5.7131-02
1.0000
13.1108
15.288
"0.44
.000
i . 1I88E -0 1
.000
2.774E-02
2.774E-02
2.5000
34.015
35.70B
347.23
.000
Il.528E-02
.000
8.5112E-03
8.5112&-03
K
liS
ED· Il.7780E-02
CRYD)
N·· 3.8411
MU·
2.11188
E (RYD)
E (EV)
E PHOT lEV.
LAMBDA
(A)
(L/RIL - 1)
(L/R/L"I)
SIGMA L-l
SIQMA L"1
SIGMA
(MB)
.0000
.000
.822
13444.58
.000
-4.037E"00
.000
8.445E-Ol
Il.445E-Ol
.0200
.272
1.184
10381.32
.000
- 1 . 112 1 E.. 00
.000
1.873E-Ol
1.1173E-Ol
.0400
.544
1 .41111
84114.82
.000
-5.1154E-Ol
.000
3.2111E-02
3.2117E-02
.0800
.8111
1.738
713 1 .1111
.000
- 1. 040E -0 1
.000
1.18H-03
1.182E-03
.0800
1.088
2.011
1111111.40
.000
1.478E-Ol
.000
2.7113E-03
2.7113E-03
.1000
1 .3111
2.283
5431 .34
.000
2.811E-Ol
.000
f.134E-02
1.134E-02
.2000
2.721
3.1143
3403.05
.000
3.880E-Ol
.000
3.84IlE-02
3.1145E-02
.3000
4.0&2
5.004
2477.78
.000
3 .• '4E-Ol
.000
3.IIBIE-02
3.11115E-02
.4000
5 .• 42
Il.385
1848.07
.000
2.820E-Ol
.000
3.18U-02
3.181E-02
1.0000
13.11011
14.528
853.42
.000
1.188E-Ol
.000
1.288E-02
1 . 28BE -02
1.5000
20.408
21.331
1181.25
.000
7.1I13E-02
.000
7.7118E-03
7.7118E-03
K
8S
EO· 2.8270E-02
IRYD)
N·· Il.84111
MU.
2.111411
E (RYD'
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/A/L-l)
(L/A/L+l)
SIQMA L-l
SIQMA L"1
SIGMA
(MB)
.0000
.000
.388
31133. III
.000
-1.108E"01
.000
3.07I1E"00
3.07I1E"00
.0100
. 1311
.534
232015. 111
.000
-Il. 170E"00
.000
8.1175E-Ol
8.117U-Ol
.0200
.272
.1170
18485.38
.000
-2.117I1E"00
.000
3.01I1E-Ol
3.01I1E-Ol
.0400
.544
.1142
1311111.30
.000
-7.1I30E-Ol
.000
3.448E-02
3.448E-02
.01100
.8111
1. 215
10208.00
.000
-'.211E-Ol
.000
1.118E-03
1.11I1E-03
.0800
1.088
1.487
83311.110
.000
1.347E-Ol
.000
1 .1I811E -03
1 . 1I118E -03
.1000
1.3111
1 . 758
70411.34
.000
2.437E-Ol
.000
B.5112E-03
Il.5112E-03
.2000
2.721
3. 1 1SI
31174.115
.000
2.811I1E-Ol
.000
r , 1I08E -02
1.1I08E-02
.3000
4.082
4.480
27111.54
.000
2.253E-Ol
.000
1.42I1E-02
1.42I1E-02
.5000
Il.803
7.201
1721.74
.000
1.437E-Ol
.000
Il.342E-03
Il. 342E -03
K
lOS
10. 1 .112431-02 (AYD 1
N·· 7.84114
MU·
2.15311
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-O
(L/IlIL"1 )
SIGMA L-l
SIGMA L+l
SIGMA
IMBI
.0000
.000
.221
IIIS 102 . l1li
.000
-2.131E+Ol
.000
Il.30BPOO
Il.308E+00
.0200
.272
.483
211143.44
.000
-3.00IlE+00
.000
2.808E-Ol
2.808E-Ol
.0400
.544
.7115
18202.40
.000
-7.08IlE-Ol
.000
2.414E-02
2.414E-02
.01100
.8111
1.037
11852.111
.000
-8.712E-02
.000
Il.14I1E-04
8.14I1E-04
.0800
1.088
, .3011
114118.43
.000
1.1421-01
.000
1. 073E -03
1.073E-03
.1000
1 .3111
1.1182
7838.311
.000
1.1140E-Ol
.000
3.741E-03
3.741E-03
.2000
2.721
2.1142
4214.10
.000
2.0114E-Ol
.000
7. 8aOE -03
7.880E-03
.3000
4.082
4.303
2881 .1111
.000
1. 511BE-0'
.000
Il. 54IlE-03
Il.114IlE-03
K
125
EO-
1.0313E-02 (AYD)
N·· Il.8470
MU'
2.1530
1
IRYD)
E (EV)
E PHOT UV)
LAMBDA
lA)
(L/R/L-O
(L/R/L"O
SIGMA L-l
SIGMA L"1
SIGMA
(MB)
.0000
.000
.140
8831l1l.85
.000
-3.45IlE+Ol
.000
1.01l3E+Ol
1.053E+Ol
.0025
.034
.174
711111.114
.000
-2.1811+01
.000
5.210E+00
5.210E+00
.0200
.272
.412
300111.78
.000
-2. Sl281+00
.000
2.222E-Ol
2.2221-01
.0400
.k4
.8811
18111.111
.000
-8.0114E-Ol
.000
1.582E-02
1.182E-02
.01100
.8111
.1I1l7
121180. 13
.000
-7.511E-02
.000
3.3I1U-04
3.a8U-04
.0800
1.088
1.2211
100110.011
.000
Il.410E-02
.000
Il.837E-04
Il.837E-04
.1000
1-.3111
1.501
8280.73
.000
1. 53I1E -01
.000
2.2331-03
2.2331-03
.2000
2.721
2.8112
4332.81
.000
1.11111-01
.000
4.325E-03
4.32IE-03
.3000
4.082
4.222
211311.111
.000
1.151E-Ol
.000
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2.1I07E+00
7.123E+00
3'131E-02
7.181E+00
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73583.70
3.484E+Ol
- 1. 4211E+00
4.238E+00
1.442E-02
4.2111E+00
.0100
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81210.40
2.55IE+Ol
-3.110E+00
2.778E+00
8.58"'E-02
2 .182E+00
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.272
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38815.53
1. 01l7E+0 1
-4.41IE+00
1.538E-Ol
2. 770E-0 1
1.13IE+00
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4.183E+00
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2.211E-Ol
2.11114E-Ol
5.21 1E -0 1
.0800
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14043.12
2.274E+00
-2.5118E+00
8.580E-02
2.48SE-OI
3.452E-Ol
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1.381
1.427
1881.011
1.038E+00
- 1. 852E+00
3.208E-02
1 .831 E -0 1
1.852E-Ol
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2.721
2.788
4441.85
3.412E-Ol
-7.11IE-Ol
7.03I1E-03
8.034E-02
8.137E-02
.4000
5.442
5.508
2250.17
1.153E-Ol
-2.224E-Ol
1.534E-03
1.142E-02
1.2115E-02
.8000
8.184
8.230
1508.51
8.048E-02
-1I.378E-02
8. 30llE -04
3.03IE-03
3.882E-03
.8000
10.185
10.851
1132.17
3.138E-02
-4.838E-02
3.380E-04
8.173E-04
1.325E-03
1.0000
13.808
13.872
808.84
2.701E-02
-2.480E-02
2. 0811E-0"
3.553E-0"
5.841E-0.
1.11000
20.408
20.475
805.54
1 .•• 4E-02
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8.1147E-05
2.584E-05
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2.0000
27.:112
27.271
454.52
8.313E-03
1.118IE-04
4.8118E-05
3.28IE-OI
4.1180E-05
2.5000
34.0111
34.081
383.80
8.854E-03
2.128t-03
3. 181E -011
8.473E-08
3.80IE-OII
3.0000
40.811
40.814
303.28
5.052E-03
2.87I1E-03
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1.41I1E-05
3.805E-05
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2.5311i+02
8.834E+01
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1.328E+01
8.777E+Ol
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1.102E+Ol
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1.015E+00
1.428E+Ol
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7.3111E-04
5.500E-03
8.238E-03
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10.185
10.1125
1134.115
2.880E-02
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4.7211i-04
8.340E-04
1.0000
13.808
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2.720E-04
1.5000
20.408
20.448
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1.2441-05
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2.0000
27.212
27.252
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2.358E-05
1.588E-08
2. 35I1E-OII
2.11000
34.015
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4.810E-03
1.482E-03
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12.502
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8.007E-Ol
1.328E-04
1.70IE-Ol
1.702E-Ol
1.0000
13.808
15.224
814.43
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4.5801-01
4.188E-08
1.208E-Ol
1.209E-01
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2.138E-01
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2.234E-04
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34.0111
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81.227
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7.314E·00
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4.774E-02
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1 . 407E .00
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1.177E-03
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2.310E-Ol
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11.804
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5 .1I43E -01
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1.411E-Ol
1.0000
13.11011
14.525
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1.5118E-OII
1.1I40E-02
1.140E-02
1.5000
20.4011
21.328
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1 . 403E -02
2.58I1E-Ol
1.055E-04
5.3110E-02
5.400E-02
2.0000
27.212
28.131
440.74
1 .511 E-02
1.815E-Ol
1.710E-04
3.414E-02
3.512E-02
2.5000
34.015
34.134
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1.133E-04
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2.4115E-02
3.0000
40.818
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217.011
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1.800E-02
4.5000
111.227
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5.784E-02
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8.741
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Il.833E-Ol
Il.005E-04
1.540E-Ol
1.54IE-Ol
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10.885
11.471
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4.1I110E-Ol
1.245E-04
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1.404E-02
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13.11011
14.112
873.85
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3.41I1E-Ol
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20.401
20.111
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1.13lE-02
2. 1OllE-0 1
Il.755E-05
3.512E-02
3.518E-02
2.0000
27.212
27.718
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1.210E-02
1.470E-Ol
1 . 1113E -04
2.2115E-02
2.277E-02
2.5000
34.015
34.1101
358.34
1.202E-02
1. 101 E-Ol
1.257E-04
1. 58 lE -02
1.513E-02
3.0000
40.818
41.404
211.411
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8.582E-02
1.18I1E-04
r , 150E -02
1 . 1112 E-02
3.5000
47.1121
48.207
257.20
Il.355E-03
Il.871E-02
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a.!582E-03
8 .1I88E -03
4.0000
114.424
55.010
225.311
8.114E-03
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Il. 283E-0!5
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7.2114E·00
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2.1177E·00
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3.785E-03
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10.885
11.281
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3.713E-Ol
8.834E-05
Il.125E-02
Il.133E-02
1.0000
13.11011
14.010
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4.24.8E-02
4.248E-02
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1.088E-03
1.700E-Ol
4.321E-0!5
2.2118E-02
2.272E-02
2.0000
27.212
27.11111
448.17
1.03IE-02
1. 184E -0 1
7.4115E-.0!5
1.4!5I1E-02
1.411I1E-02
2.5000
34.015
34.4111
3110.23
Il.1180E-03
8.851E-02
8.107E-05
1.017E-02
1.02!5E-02
3.0000
40.818.
41.222
300.78
8.!587E-03
Il.8114E-02
7.841E-05
7.38I1E-03
7.4112E-03
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1 .1I488E -02
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7.017E·Ol
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2.721
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1 .1I40E .00
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1.147E-03
1. 027E-Ol
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8. 1114
8.388
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3.873E-Ol
3.188E-04
4.7431-02
4.775&-02
.8000
10.88!5
11.101
11111.08
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2.1I10E-Ol
4.4113E-0!5
2.853E-02
2.858E-02
1.0000
13.11011
13.830
8111.48
-1.782E-03
1.144l!-01
1.104E-OII
1.117lE-02
1. 117 lE-02
1.5000
20.4011
20.1133
1100.11
Il.173E-03
1.1110E-Ol
1.87I1E-0!5
1. 04 liE -02
1.048E-02
2.0000
27.212
27.4311
451.11
7.07'E-03
8.0!55E-02
3.4!58E-0!5
Il. 712E -03
Il.747E-03
2.5000
34.01!5
34.2311
3"2.12
8.!588E-03
Il.014E-02
3.733E-0!5
4.88IE-03
4.707E-03
3.0000
40.818
41.042
302.10
5.841E-03
4.880E-02
3.5I1E-0!5
3.38IE-03
3.424E-03
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1.0454E-02 (AVD)
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LAMBDA (A)
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1 .11I3l!.0 1
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4.148E·Ol
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2.'18E+Ol
1.8131·00
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1.38!5E+Ol
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4.8<l2E+00
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1.381
1.503
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4.041E+00
8.473E-02
1.254E-Ol
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2.721
2.883
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1. 455E .00
1.05U-02
2.288E-Ol
2.311E-Ol
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5.585
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1.083E-03
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5.817E-02
.8000
8.1114
8.3011
14112.77
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2.8411-01
1.754E-04
2.!528E-02
2.545E-02
.8000
10.885
11.027
1124.31
-1.417E-03
1.10IE-Ol
2.458E-0!5
1.!515E-02
1.!518E-02
1.0000
13.808
13.7.8
101.14
-1.388E-03
1.420E-Ol
Il.484E-07
1.045E-02
1.045E-02
1. !l000
20.401
20.5151
803.31
4.48IE-03
8.44IE-02
1.04lE-05
5. !531 E-03
5.!54 U -03
2.0000
27.212
27.354
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1.823E-0!5
3.843E-03
3.5111E-03
2.5000
34.015
34.1157
382.1111
4.714E-03
4.373E-02
1.1173E-0!5
2.483E-03
2.483E-03
3.0000
40.818
40.180
302.70
4.248E-03
3.402E-02
1.85SE-0!5
1.787E-03
1. 80llE -03
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1. 580E +02
2.847E+Ol
II. 008E+0 1
1.18I5E+02
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74831.88
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7.853E+Ol
8.345E+00
3.888E+Ol
4.503E+Ol
.0200
.272
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2.4113E+Ol
1.284E+00
8.873E+00
Il.1I37E+00
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1.4110E-02
1.500E-02
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10.885
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5.1137E-08
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1.381
13.177
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8.578E-02
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CA 11
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3.873I1E-Ol
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2.2880E-Ol
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1.8188
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1.527E+00
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27.482
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1 .80811
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2.5118E+00
3.1111E+00
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2.721
11.4115
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3.30lE-Ol
Il.323E-Ol
1.282E+00
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5.442
14.218
872.15
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2.083E-Ol
3.744E-Ol
5.827E-Ol
.8000
10.885
111.8511
830.70
5. 02lE-0 1
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1. 038E··0 1
8.513E-02
1.8110E-Ol
1.0000
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22.380
554.01
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7.873E-02
2.4118E-02
1.037E-Ol
2.0000
27.212
35.1188
344.54
1.1155E-Ol
4.312E-02
2.882E-02
2.803E-03
3.183E-02
3.0000
40.818
411.5112
250.01
1. 1110E-0 1
7.783E-02
1.471 E- 02
1.252E-02
2.723E-02
4.0000
54.424
83.1117
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8.178E-02
7.11115E-02
8.84I1E-03
1.8112E-02
2.577E-02
5.0000
88.030
78.803
181.43
8.042E-02
7. 455E - 02
5.873E-03
1.788E-02
2.375&-02
8.0000
81.835
110.4011
137.14
4.887E-02
8.753E-02
4. 1511E-03
1.727E-02
2.143E-02
CA Il
5P
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1.4801
E (AYD)
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SIGMA L-l
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.0000
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4.3113
2822.55
3.545E+00
-5.170E+00
1. 158E+00
4.1118E+00
8.075E+00
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4.1137
2511.40
2.1128E+00
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8.887E-Ol
3.488E+00
4.354E+00
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5.442
Il.835
1280.85
Il.522E-Ol
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1.888E-Ol
3.311IlE-Ol
5.227E-Ol
.8000
10.885
15.277
811.58
4.888E-Ol
-2.878E-Ol
8.1172E-02
4.583E-02
I.l!l5E-Ol
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13.808
17.111111
888.87
3.585E-Ol
-1.4113E-Ol
4.845E-02
1.882E-02
8.527E-02
2.0000
27.212
31.805
3112.31
1.45I1E-Ol
2.731E-02
1.410E-02
Il.872E-04
1.50IlE-02
3.0000
40.818
45.210
274.24
8.2115E-02
5.087E-02
8.517E-03
4.1I02E-03
1.142E-02
CA Il
8P
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1.1148111-01
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N·· 4.5304
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1.48118
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA
lAI
(L/A/L-l)
(L/A/L+I)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
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2.852
4875.112
5.7114E+00
-8.312E+00
I.884E+00
7.874E+00
Il.538E+00
.0800
1.088
3.740
3315.011
3.285E+00
-4.345E+00
8.457E-Ol
2.115I1E+00
3.804E+00
.4000
5.442
8.0114
1531.84
Il.227E-Ol
-8.88I1E-Ol
1.443E-01
2.580E-01
4.003E-Ol
.8000
8.184
10.815
1148.41
5.738E-Ol
-4.284E-Ol
7.45I1E-02
8.318E-02
1.578E-Ol
.8000
10.885
13.538
1115.115
3.1177E-Ol
-2.288E-Ol
4.484E-02
2.1183E-02
7.448E-02
1.0000
13.808
18.258
782.84
2.1152E-Ol
-1.242E-01
2.1187E-02
1. 05 le -02
4.018&-02
2.0000
27.212
211.883
415.18
l.l07E-Ol
1.1138E-02
7.870E-03
4.700E-04
8.140E-03
3.0000
40.818
43.4811
285.23
8.0115E-02
3.848E-02
3.383E-03
2.42IE-03
5.804&-03
4.0000
54.424
57.075
217.23
3.1188E-02
3.853E-02
1.880E-03
3.1111 E-03
5.07lE-03
5.0000
88.030
70.881
175.42
.2.832E-02
3. 334E -02
1. 188E-03
3.2112E-03
4.480E-03
8.0000
81.835
84.287
147.10
2 .. 148E-02
2.1174E-02
8.133E-04
3.124E-03
3.1137E-03
OA
Il
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(AYO)
N.· 8.5384
MU'
1_ 48 11l
E (AYO)
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LAMBDA
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(L/A/L-t)
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SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
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1.273
11739.41
1.17IE+Ol
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3.854E+00
1.428E+Ol
1.7111 E+O 1
.0200
.272
1.545
8024.20
8.48I1E+00
-1.185E+01
2.332E+00
8.787E+00
1.112E+OI
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1.088
2.382
5250.30
4.201E+00
-5.448E+00
li. 72I1E-OI
2.1138E+00
3.80IlE+00
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2.721
3.11114
3104.14
1.757E+00
-2.022E+00
2.584& -0 1
8.838E-01
Il.422E-Ol
.4000
5.442
Il.715
1848.30
7.430E-Ol
-8.1127E-Ol
7.785E-02
1.350E-01
2.128E-Ol
.8000
8.184
Il.437
1313.811
4.234E-01
-3.143E-Ol
3.543E-02
3.1I05E-02
7.448E-02
1.0000
13.808
14.8711
833.30
2.002E-01
-8.4831-02
1.248E-02
4.484E-03
1 .•1I5E-02
2.0000
27.212
28.485
435.27
8.1188E-02
1.158E-02
2.8115E-03
1.5118E-04
3.0511E-03
3.0000
40.818
42.0111
2114.57
3.729E-02
2.187E-02
1.2281-03
1I.438E-04
2.070E-03
4.0000
54.424
55.81l7
222.81
2.31111-02
2. 173E -02
Il.871S-04
1 . 102E -03
1.78I1E-03
5.0000
88.030
811.303
178.111
1.8113E-02
1.1l72i-02
4.180E-04
1.129E-03
1.545E-03
8.0000
1I1.835
82.11011
1411.55
i . 275E -02
1. 752E -02
2.825E-04
1.088E-03
1.348E-03
OA
Il
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(AYD)
N·· 8.5414
MU'
1.4588
E ( RYD)
E (EV)
E PHOT (EV)
LAMBDA
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<L/R/L-1l
(i./A/L+ 1 ).....
$lGMA L-I
SIGMA L+I
SIGMA (MB)
.0000
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18820.50
1.1141E+Ol
-2.85111+01
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2.210E+Ol
2.7118E+Ol
.0400
.544
1.2110
118011.70
7.8071+00
-1.0371+01
1.. 847E+00
5.817E+00
7.484E+00
.0800
1.088
1.834
8758.75
4.34I1E+00
-5.57.1+00
7.288E-Ol
2.381ll+00
3.118E+00
.2000
2.721
3.487
3578.01
1.50IlE+00
-1.722E+00
1 .•54E-Ol
4.307E-01
5.1180E-Ol
.4000
5.442
8.188
2003.54
5.780E-Ol
-5.342E-Ol
4.300E-02
7.311I1E-02
1.170E-Ol
.8000
8.184
8.1110
13111.81
3.1471-01
-2.321lE-Ol
1. 848E -02
2.024E-02
3.872E-02
.8000
10.885
11.831
1088.02
2.02!5E-Ol
-1.1I5IE-Ol
Il.1I113E-03
8.5881-03
1.8581-02
1.0000
13.808
14.352
883.110
1.432E-Ol
-8.0821-02
8.188E-03
2.201lE-03
8.378E-03
2.0000
27.212
27.1158
443.48
4.8301-02
7.858E-03
1.388E-03
7.232E-05
1.43I1E-03
3.0000
40.8111
41.584
2118.30
2.558E-02
1.48I1E-02
5. 8811E-04
3.85I1E-04
Il.548E-04
4.0000
54.424
55.170
22_.74
1.830E-02
1.472E-02
3.070E-04
5.010E-04
8.080E-04
5.0000
88.030
88.778
180.211
1.150E-02
1.3331 -02
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2.782E+00
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1.254E-01
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2.5181-03
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1.488E-04
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10.885
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3.388E-02
2.535E-Ol
3.258E-0"
2.73I1E-02
2.772E-02
1.0000
13.15015
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2.134E-02
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9.788E-02
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2.0000
27.212
33.3811
371.34
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1.418E-Ol
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4.220E-02
4.220E-02
SC III
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1.1416
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8.184
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1117.07
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3.11I1E-Ol
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Il.500E-02
Il.100E-02
1.0000
13.108
18.142
7411.14
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2.174E-Ol
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4.1113E-02
4.1113E-02
3.0000
40.818
43.713
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1.835E-02
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9.382E-03
Il.382E-03
SC III
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1.13113
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SIGMA 1MB)
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2.854E+00
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7.571E-Ol
7.571E-Ol
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2.721
4.432
27117.13
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8.805E-Ol
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2.012E-Ol
2.082E-Ol
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5.442
7.153
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4.818E-Ol
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9.578E-02
9.578E-02
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10.885
12.5115
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3.8113E-02
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13.108
15.311
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2.838E-02
2.838E-02
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8.1124E-02
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8.713E-03
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54.424
58.134
220.87
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2.803E-02
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2.7721-03
2.772E-03
SC III
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10.4817
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3.805E+00
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Il.135E-Ol
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1.815E+00
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3.817E-Ol
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5.442
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3.884E-Ol
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15.221E-02
8.221&-02
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13.801
14.725
842.03
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1.288E-Ol
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1 .153IE -02
1.538E-02
2.0000
27.212
28.331
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5.21I1E-02
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4.810E-03
SC III
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1.5373
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1 . 234E +00
1.234E+00
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1"458.211
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3.184E+00
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7.235E-Ol
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1.311
1.1148
8371.28
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1.274E+00
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1.1184E-Ol
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2.721
3.307
37411.85
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8.258E-Ol
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8.138E-02
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1.5319
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8.338E+00
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1.51I1E+00
1.5eIlE+00
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.272
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111138.83
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4.114E+00
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8.713E-Ol
1.713E-Ol
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1.088
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1 .388E+00
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8.184
8.523
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1. 1I8E -01
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i.8111E-03
7.8111E-03
1.0000
13.101
13.1115
887.83
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1.022E-02
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3. 183E-03
3.183E-03
SC III
4P
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3.242E-Ol
1.5t17E-Ol
4.83I1E-Ol
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1.311
18.037
887.41
8.4111E-Ol
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8.1178E-02
3.122E-Ol
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5.442
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1.734E-Ol
1. 011E-02
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8.184
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5.080E-Ol
-1.873E-02
1.3431-01
3.152E-04
1.348E-Ol
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10.885
27.581
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4.300E-Ol
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1. 088E -01
1.478E-03
1.082E-Ol
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13.108
30.282
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3.811111-01
7.108E-02
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6.404E-03
Il.318E-02
2.0000
27.212
43.888
282.51
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1.273E-Ol
3.845E-02
2.1181 E-02
1.828E-02
3.0000
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57.4114
215.15
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1.245E-Ol
2.134E-02
3.733E-02
5.887E-02
4.0000
14.424
71.100
174.38
Il.505E-02
1.120E-Ol
1. 345E -02
3.735E-02
5.081&-02
5.0000
18.030
84.701
141.37
7.204E-02
Il.1101&-02
9.208E-03
3.478E-02
oI.311I1ê-02
13
SC III
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2.022E-Ol
3.0117E-02
2.332E-Ol
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7.171E-02
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7.328E-02
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8.717E-02
3.1I1I1E-02
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27.212
35.1171
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Il. 780E-02
2.~37E-02
1.~38i-02
3.873E-02
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3".015
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1.357E-0;
Il.85aE-02
1 .8"IIE -02
1 .872E -02
3.320E-02
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1.I84E-02
1.748E-02
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8.88I1E-02
8.578E·02
8.878E-03
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2.522E-02
5.335E-02
5.071E-0"
5.38I5E-02
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27.212
32.8311
3711.87
1.500E-Ol
7.855E-02
1.53I1E-02
8.012E-03
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1.8"7E-02
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207.18
5.581E-02
5.1180E-02
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1 . 823E +00
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1.807E+00
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3.535E-02
1.778E-Ol
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8.18"
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5 .545E-Ol
-1.1"3E-Ol
7.23I1E-02
5.1138E-03
7.833E-02
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10.885
13.588
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3.883E-Ol
-2. 83I1E.-02
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".582E-0~
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1.0000
13.808
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781.27
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2.802E-02
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27.212
211.883
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5.033E-02
8.770E-03
3.172E·03
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5.5110E-02
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8.512E-03
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217.12
3.575E-02
3.758E·02
1 . 5211E-03
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2.522E-02
3. 158E-02
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3.8117E-03
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7.058E+00
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3.170E-03
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2."80E-02
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8.1I01E-03
1. 538E -02
3.033E-OS
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2.0000
27.212
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3.1578E-02
3.~35E-03
1.15.. 3E-03
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3.0000
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3.1170E-02
3.1"!5E-02
1 . "00E-03
1 . 758E -03
3.158E-03
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2.511 E-02
2.813E-02
7.3118E-0~
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5.0000
88.030
811.825
178.08
1. 7511E-02
2.188E-02
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1 .311"E-03
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Il.123E-03
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1.310E-02
1.823E-02
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1.011E-03
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2.0000
27.212
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1.174E+00
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1.082E+00
1.151E+00
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115.154
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1.887E-Ol
7.130E-Ol
1 . 785E -02
3.825E-Ol
4.004E-Ol
2.0000
27.212
33.5150
3158.45
8.728E-02
3.832E-OI
15.427E-03
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47.1521
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1.310E-02
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31.417
384.815
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3.041E-Ol
4.185E-03
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1.137E-Ol
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1.837
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7.1281-02
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1.282E-OI
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15.271
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2.0000
27.212
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2.285E-02
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8.0.U-02
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1.330E-Ol
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2.508E-Ol
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1.0000
13.15011
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3 .• 1I!U-03
2.221E-02
2.51171-02
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27.212
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2.585E+00
5.808E-Ol
3.17I1E+00
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.272
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7.110E+00
-1.524E+00
1.078E+00
7.431E-02
1.152E+00
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5.802E-Ol
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1.383
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3. 174E+00
1.328E-Ol
3.52I1E-Ol
8.257E-04
3.535E-Ol
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2.375E+00
3.483E-Ol
2.380E-Ol
7.528E-03
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1 .3111
1.837
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1.857E+00
4.448E-Ol
1.1180E-Ol
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7.830E-Ol
4.808E-Ol
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2.874E-02
7.858E-02
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5.442
8.018
20110.03
2.940E-Ol
3.331E-Ol
1.308E-02
2.517E-02
3.825E-02
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8.1114
8.740
1418.113
1,587E-Ol
2.407E-Ol
5.1I0IlE-03
1.808E-02
2.4118E-02
1.0000
13.808
14.182
874.24
7.204 E-02
1.470E-Ol
1.850E-03
1.155E-02
t • 340E -02
2.0000
27.212
27.788
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2. 357E -02
Il.824E-02
3.878E-04
4.587E-03
4.885E-03
4.0000
54.424
55.000
225.43
7.480E-03
2.58I1E-02
7. 7315E-05
1.388E-03
1.475E-03
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1.02021+00 CAlDI
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13.881
'83.21
3.843E-Ol
1.7118E+00
4.9112E-02
1 . 558E +00
1.1I07E+00
.2000
2.721
18.1102
748.81
2.582E-Ol
1.182E+00
2.882E-02
8.323E-Ol
8.8211-01
.8000
8.1154
22.044
582.44
1.488E-Ol
8.188E-Ol
1. 28lE-02
3.031E-Ol
3.1581-01
.8000
10.885
24.71111
500.84
1.15eE-Ol
4.734E-Ol
8.921E-03
1.883E-Ol
2.082E-Ol
1.0000
13.1108
27.487
451.08
8.288E-02
3.721E-Ot
8.388E-03
1.387E-Ol
1. 431 E -0 1
2.0000
27.212
41.083
301.72
3.852E-02
1.484E-Ol
1 . 842E -03
3.1113E-02
3.327E-02
2.5000
34.015
47.8.11
2!l8.87
2. 708E -02
1.02I1E-Ol
8.458E-04
1 . 808E -02
1.8041-02
3.5000
47.1121
81.502
201.110
1.483E-02
5.742E-02
3. 880E-04
7.281E-03
7.1150E-03
TI
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SIGMA L-l
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7.870E-Ol
3. 133E+00
1.485E-Ol
3. 137E+00
3.2851+00
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2.721
Il.1122
1088.80
4.809E-Ol
1.850E+00
7.237E-02
1.428E+00
1 .50 lE +00
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5.4"2
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8154.41
3.225E-Ol
1.205E+00
4.018E-02
7.482E-Ol
7.884E-Ol
1.0000
13.8011
22.507
550.88
1.318E-Ol
4.854E-Ol
1 . OUI -02
1.750E-Ol
1.858E-Ol
2.0000
27.212
38.113
343.33
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1. 852E -0 1
2.247E-03
3. 538E -02
3.783E-02
3.0000
40.818
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2.3181-02
8.083E-02
7.20lE-04
1.1118E-02
1.241E-02
3.5000
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218.311
1.7121-02
8.088E-02
4.483E-04
7.474E-03
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4. 53BE -00
2.853E-Ol
4. 581lE +00
4.850E+00
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1.388E-00
5. 333E -02
8.155E-Ol
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10.885
17 .058
728.81
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8.488E-Ol
1.778E-02
2.587E-Ol
2.7154E-Ol
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13.11011
19.780
828.82
1.482E-Ol
4.7113E-Ol
1.138E-02
1.832E-01
1.74I1E-Ol
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33.38.
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48.882
2153.85
2.253E-02
7.480E-02
Il.425E-04
Il.-4&8E -03
1.011E-02
4.0000
54.424
80.5.8
204.81
1.235E-02
4.28l1E-02
2.4881-04
3.885E-03
4.214E-03
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2.831E+00
7.577E+00
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7.134E+00
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2.721
8.182
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Il.481E-Ol
2.847E+00
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1.788E+00
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1.481E+00
5.734E-02
7.010E-Ol
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10.885
14.348
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1.1181 E-Ol
8.003E-Ol
1 . 518E - 02
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4.282E-Ol
8. 111 E-03
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1.2051-01
2.0000
27.212
30.873
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4. 180E-02
1.280E-Ol
1.443E-03
1.804E-02
1.848E-02
2.5000
34.015
37.478
330.84
2.8e2E-02
8.384E-02
7.315E-04
Il.415E-03
1.015E-02
3.5000
47.821
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242.72
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4.28111-02
2.418E-04
3.374E-03
3.1118E-03
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8.544E+00
1. 01141 +0 1
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2.481
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3.51111+00
8.134E+00
8.258E-Ol
7.432E+00
8.258E+00
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2.721
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2.8871+00
1.508E-Ol
1 .55111 +00
1.710E+00
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4.835E-Ol
1.381E+00
4.8171-02
5.2401-01
5.722E-Ol
1.0000
13.808
15.815
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1.220E-Ol
3.5531-01
8.338E-03
7.188E-02
7.802E-02
2.0000
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28.421
421.43
3.402E-02
1.013E-Ol
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1 . 084E -02
1. 178E -02
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34.015
38.224
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2.180E-02
8.548E-02
4.552E-04
5.574E-03
8.028E-03
4.0000
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7.735E-03
2.510E-02
8.124E-05
1.28lE-03
1. 372E -03
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8.255E'+00
1.473E+Ol
1.813E+00
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4.7411+00
1.143E+Ol
1.00lE+00
8.457E+00
Il.54I1E+00
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5875.71
3. 733E+00
Il.173E+00
7.788E-Ol
8.28I1E+00
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2.721
4.252
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1.0801+00
2.8741+00
1. 338E-Ol
1.2I1lE+00
1.385E+00
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Il.873
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4.4110E-Ol
1.23lE+oo
3.7351-02
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10.885
12.415
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1.518E-Ol
4.288E-Ol
7.705E-03
8.240E-02
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1.0000
13.11011
15.1311
8111.12
1.033E-Ol
2.11"31-01
4.347E-03
4.7081-02
5.1421-02
2.0000
27.212
28.742
431.37
2.7751-02
8.138E-02
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7.432E-03
3.5000
47.1121
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9.2110E-05
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2.223E+00
5.33I1E+00
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2.271E+00
2.588E+00
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2.721
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Il.725E-Ol
2."85E+00
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7.812E-Ol
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3.580E-Ol
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2.151E-02
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2.252E-Ol
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2. 177E-03
2.258E-02
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511.424
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2.043E-01
7.3113E-02
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1 .781 E -02
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2.1188E-02
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1.820E-02
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8.880E-02
1.112E+00
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1.727E+00
2.408E-01
3.487E-01
1.35I1E-02
3.1123E-01
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8.811IE-01
2.183E-01
1.3115E-01
1.872E-02
1.533E-01
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8.1114
11.024
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5.484E-01
1.838E-01
8.8118E-02
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8.530E-02
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18.41111
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1.325E-Ol
2.117BE-02
1. 211 E-02
3.888E-02
2.0000
27.212
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412.30
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7.342E-02
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8.7IOE-03
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7.81I1E-04
2.342E-03
3.142E-03
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111.707
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8.251E-03
2.188E+00
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2.424
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1.11351+00
1.482E-03
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4.712E+00
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1.275E+00
2.107E-OII
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4.047E+00
7. 2~5E-02
1.018E+00
Il.817E-04
1.0lI1E+00
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1.248E-01
8.280E-01
2.118E-03
8.311E-01
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2.721
4.873
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2.184E-01
3.178E-01
8.82I1E-03
3.275E-01
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5.442
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8.3ll4E-Ol
1.874E-01
1.1131-01
1.240E-02
1.237E-01
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8.164
10.315
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4.888E-Ol
1.821E-01
5.377E-02
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1.345E-Ol
3.077E-02·
8.8 ~E-03
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15.758
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2.435E-01
1.138E-01
1 . 858E -02
8.5118E-03
2.812E-02
2.0000
27.212
28.3114
422.24
8.44I1E-02
8.141E-02
4.38IE-03
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8.030E-03
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2.884E-02
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1.412E-02
1.8113E-02
3.500E-04
1.2I8E-03
1.588E-03
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2.531E-01
2.0000
27.212
58.t72
210.25
... t37E-02
2.158E-Ol
3.872E-03
9.853E-02
1.025E-Ol
3.0000
.. 0.818
72.578
170.83
3.12BE-02
1.3531-01
1.813E-03
".788E-02
".t5tE-02
".5000
151.227
t2.t87
133.3"
1.777E-02
7.703E-02
7.tl0E-0"
1 . t81 E-02
2.080E-02
8.0000
81.1535
113.388
IOt.3 ..
1.112E-02
".885E·02
3. 777E-0"
9.715E-03
1.0091-02
Cl.gggll
lC1B.a.7
"0.001
18. ,.
8.IOIE-03
2.gl~E-a2
t. B~!l~-O~
... dll~-6S
".801&-03
30
CR VI
51'
EO·
1.4848E+00
(RYD)
N.· 4.8074
MU'
.08211
t
( RYD)
t
(EV)
E PHOT (EV)
LAMIDA
(A)
(L/R/L-l )
(L/R/L+ 1 )
SIGMA L-l
SIGMA L+l
SIGMA
(MIl
.0000
.000
20.338
1108.111
3.871E-Ol
1 . 455E + 00
8.210E-02
1.547E+00
1.1128E+00
.5000
Il.803
27.142
4511.81
2.233E-Ol
8.372E-Ol
3.114I1E-02
Il.831E-Ol
7.18I1E-Ol
1.0000
13.5011
33.8.5
3115.211
1.43BE-Ol
5.374E-Ol
1.880E-02
3.520E-Ol
3.708E-Ol
2.0000
27.212
47.510
2110.75
7.213E-02
2.118I1E-Ol
Il.1I113E-03
1,241E'01
1.308E-Ol
3.0000
40.818
111 . 1511
202.74
4.211E-02
1. 587E -0 1
2.820E-03
5.5281-02
5.821E-02
!S.0000
118.030
88.3118
140.31
1.844E-02
7.1110E-02
8.088E-04
1.1127E·02
1.70BE-02
Il.0000
81 .1135
101.87.
12 1 .58
1.320E-02
5.221E-02
4.785E-04
8.880E-03
1.04I1E-02
8.0000
108.847
128. 1811
85.88
7.4811~-03
3.074E·02
1 .851 E - 04
4.382E-03
4.578E-03
CR VI
81'
EO'
1.0348E+00
(RYD)
N.· 5.8883
MU'
.1017
E (RYD)
E lEV)
E PHOT (EV)
LAeDA
lAI
1 L/R/L-l )
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA
lM11
.0000
.000
14.0111
BIIO.1I3
Il.537E-Ol
2.070E+00
1 .1I20E-0 1
2.1117E+00
2.32I1E+00
. 11000
Il.803
20.112
583.74
3.141E-Ol
1.028E+00
Il.51l0E-02
7.1120E-Ol
8.475E-Ol
1.0000
13.11011
27. III Il
447.14
1.12IlE-Ol
Il.0731'01
2.483E-02
3.11117E-Ol
3.815E-Ol
2.0000
27.212
41 .281
300.27
8.175E-02
2.78IlE-Ol
7.431E-03
1. 150E-0 1
1. 224E-0 1
3.0000
40.818
1l4.887
2211.81l
4.488E-02
1. 1l112E-0 1
2.978E-03
4. 81lE -02
5.108E-02
5.0000
118.030
82.108
151. 00
1.840E-02
Il.70IlE-02
7.488E-04
1. 3211E -02
1.400E-02
Il.0000
81.11311
115.715
128.54
1.2112E·02
4.818E-02
4.301E-04
7.1178E-03
8.408E-03
CR VI
81'
EO· 5.7821E·01
lRYDI
N·· 7.8801
MU'
· 1088
E i RYD)
E
1 EV 1
E PHOT
1 EV)
LAMIDA
lA)
lL/R/L-l)
lL/R/L+l)
SIGMA L - 1
SIGMA L+ 1
SIGMA
lM1I1
.0000
.000
7.888
11175.84
1.344E+00
3.382E+00
3.828E-Ol
3.231E+00
3.1114E+00
.1l000
Il.803
14.1111
845.12
4.358E-Ol
1.212E+00
7.1I03E-02
7.744E-Ol
8.484E-Ol
1.0000
13.11011
21.474
571.38
2.127E-Ol
Il.211 E-O 1
2.1I1I1E-02
2.1175E-Ol
3.23I1E-Ol
2.0000
27.212
35.010
353.44
8.085E-02
2.48I1E-Ol
Il.17I1E-03
7.&40E-02
8.4118E-02
4.0000
54.424
112.292
1119.04
2.412E·02
7.818E·02
9.757E-04
1. 427E -02
1.525E-02
5.0000
118.030
711.Bt8
1113.311
1.5114E-02
5.308E·02
4.938E-04
7.1180E-03
8.173E-03
1.0000
108.8"7
1111.7111
108.23
5.712E·03
2.118E·02
1.02I1E-04
1.178E-03
1.812E·03
CR VI
lOF
EO' 3.8830E-Ol
(RYD)
N.· 8.88117
MU'
.1133
E 1 RYDI
E 1 EV)
E PHOT (EV)
LAMIIDA
lA)
(L/R/L-l )
(L/R/L+ 1 )
SIGMA L-l
SIGMA L+l
SIGMA
lMIl)
.0000
.000
5.011
2474.24
2.232E+00
4.831E+00
Il.72I1E·01
".200E+00
".873E+00
.5000
Il.803
1 1 . 814
1048.48
".8.. 4E·01
1 . 233E+00
7.4114E·02
Il ..... BE-Ol
7. 1811E-Ol
1.0000
13.11011
18.1117
11115.88
2.07I1E·01
5.11118E·01
2. 1111 E'02
2.1"BE-Ol
2.3114E-Ol
1.5000
20."08
25."20
"87.75
1.138E·01
3.2"5E·01
8.878E-03
8.1I10E-02
1.050E·01
3.0000
"0.818
411.128
270.5"
3 ..... 8E·02
1.01l2E·01
1.4117E-03
1.157E-02
2.004E·02
4.0000
5 ..... 2 ..
1l8.435
208.111
1.877E-02
Il.328E-02
Il. 251lE-04
8. 5 .. n
-03
8.172E-03
Il.0000
81.1135
811. Il'' 7
143.08
8.1l0"E-03
2.80U-02
1.1188E-0"
2.1131E·03
2.800E-03
7.0000
81l.2'"
100.21l2
123.117
8.0111E-03
2. 13!5E -02
9. IIUIE' 05
1.841E·03
1.7"OE-03
CR VI
121'
EO'
2.1l .. 87E·01
lRYDI
N·· Il.8848
MU'
· 11 112
E ( RYD)
E lEV)
E PHOT lEV)
LAMIDA
lA)
(L/R/L'11
lL/R/L+l )
SIGMA L-l
SIGMA L+l
SIGMA
IMIl)
.0000
.000
3.4118
3575 .....
3.308E+00
Il.427E+00
1.022E+00
5.1"4E+00
Il.1118E+00
.1l000
Il.803
10.271
1207.18
4.8112E·01
1.173E+00
Il.5''OE-02
Il.07.. E·01
Il.728E-Ol
1.0000
13.11011
17.07..
7211.18
1. 887E -0 1
4.8811-01
1.1155E·02
1.521 E·Ol
1 . 1117E-0 1
1. 11000
20 ... 08
23.877
5111. 28
8.1170E,02
2.752E·01
Il.3112E·03
Il.4114E-02
7. 134E-02
3.0000
40.818
44.285
278.17
2.811I1E·02
8.1138E·02
8.784E-04
1.1I7E-02
1.285E-02
".0000
54.424
57.881
21".17
1.1118E·02
!l.08I1E-02
4.085E-0"
!1. 37BE-03
5. 7811E-03
7.0000
81l.2'"
118.708
125.81
4.881E·03
1.1188E-02
Il. 212E -05
1.010E-03
1.073E·03
CR VI
1111'
10·
1.42701-01
IRYD)
N.· 15.8831
MU'
· 1 1118
E (RYD)
E 1 EV 1
E PHOT (EV)
LAMIIDA
(A)
lL/R/L-l)
1 L/R/L+ 1 )
SIGMA L'I'
SIGMA L+l
SIGMA
(Mil)
.0000
.000
1 .8.. 2
8385.77
5.818E+00
1 . OOIlE+O 1
1.875E+00
7.0!52E+00
8.1127E+00
.5000
Il.103
8.745
1417.17
4.318E·01
9.827E·01
4.3801'02
3.0321'01
3.471E-Ol
1.0000
13.11011
15.11"8
787.47
1 ... 87E·0 1
3.773E-Ol
8.3831'03
7.8"8E-02
8.888E-02
1.5000
20."08
22.350
51l".74
7.487E·02
2.001E·01
3.374E-03
3.212E-02
3.550E·02
3.0000
40.118
42.758
288.88
2.0331-02
5.lIlJllE-02
4.7110E-04
5.520E·03
5.1It1I1E·03
5.0000
118.030
1111.871
177.20
7.0311'03
2.2!l4E-02
8.318E-OII
1. 2711E '03
1 . 3118E -03
CR VI
201'
EO' 8. 101181- 02
IRYD)
N.· 111.8823
MU'
.1177
E ( RYD)
E
lEV)
E PHOT (EV)
LANIIDA lA)
lL/R/L'1l
IL/R/L+1l
SlaMA L-l
SlaMA \\,+ 1
SIGMA
IMIII
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1.2311
100011.37
8.341E+00
1. 4211E+0 1
2.812E+00
8.043E+00
1. 188E+Ol
.2000
2.721
3.880
3130.711
1.272E+00
2.44I1E+00
1.725E-Ol
8.510E·01
1.023E+00
.4000
5.442
Il.1181
181l5.18
5.05I1E·01
1.07I1E+00
4.1I01E-02
2.782E·01
3.252E-Ol
1.0000
13.11011
14 .8"5
831l.21
1.17IE·01
2.810E-Ol
5.1144E·03
4.515E·02
5.01lIlE-02
2.0000
27.212
28.451
435.78
3.357E·02
8.220E-02
8. 1135E '04
8.118I1E-03
Il. 5"1IE -03
3.0000
40.818
42.057
284.81
1.51IlE-02
4.4231-02
2.1I00E·04
2.t!55E-03
3.215E-03
31
Mil VII
4S
EO. 5.7518E+00 (RYD)
N·· 2.11187
MU'
1.0813
E 4RYD)
E (EV)
E PHOT lEV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+I'
SlCMA
L- 1
SICMA L+l
SICMA
(MB)
.0000
.000
78.258
1!l8.43
.000
2.012E-01
.000
1.1I111E-Ol
1.1I111E-01
1.0000
13.505
111.8&4
134.117
.000
1 . 554E -01
.000
1.!l7I1E-Ol
1. !l711E -01
4.0000
54.424
132.U2
113.45
.000
1.035E-Ol
.000
8.114!lE-02
8.114!lE-02
IIQII VIl
55
EO' 3.I!l85E+00 (RYD)
N·· 3.11387
MU·
1.0513
E (RYD)
E (EV)
E PHOT (IVI
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l)
SICMA L-I
SICMA L+l
SICMA
(MB)
.0000
.000
42.1175
288.50
.000
3.177E-Ol
.000
2. 12!lE-01
2.725E-01
1.0000
13.505
!l5.581
2111. 13
.000
2.224E-Ol
.000
1.758E-Ol
1. 758E -0 1
3.0000
40.818
83.7113
147.117
.000
1.313E-Ol
.000
Il.084E-02
Il.084E-02
7.0000
115.241
138.217
811.70
.000
5.1112E-02
.000
3.7117E-02
3.7117E-02
Mil VII
5S
10· 2.002I1E+00
(RYD)
N·· 4.114111
MU·
1 .05311
E (RYD)
E (EV)
E PHOT (IV)
LAMBDA
(A)
IL/R/L-l)
(L/R/L+ 1 )
SlCMA
L-l
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L+l
SICMA
(MB)
.0000
.000
27.252
4!l4.117
.000
4.5110E-OI
.000
3.5111E-Ol
3.551E-Ol
1.0000
13.1105
40.8118
303.45
.000
2.548E-OI
.000
1.801E-Ol
1.801E-Ol
3.0000
40.818
118.070
182.15
.000
1.305E-Ol
.000
7.28I1E-02
7.28I1E-02
8.0000
108.847
1311.01111
III . 10
.000
4.1I1I1E-02
.000
2.070E-02
2.070E-02
Mil VII
85
10·
1.013I1E+00 (RYD)
N·· Il.11520
MU·
1.0480
E ( RYD)
E (EV)
E PHOT
(EV)
LAMeDA (A)
(L/R/L-l)
(L/R/L+l)
SICMA L-I
SICMA L+I
SIGMA
(MB)
.0000
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13.7114
8118.82
.000
7.lIllE-Ol
.000
5.425E-01
5.425E-Ol
1.0000
13.505
27.400
452.50
.000
3.030E-Ol
.000
1 . 118lE -01
1 .1l81 E-Ol
2.0000
27.212
41.0011
302.311
.000
1.701E-01
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7.41l3E-02
7.453E-02
Il. 0000
58.030
81.824
151.53
.000
5.272E-02
.000
2.023E-02
2.023E-02
8.0000
108.847
122. &42
101.10
.000
3.5001-02
.000
Il.443E-03
Il ....43E -03
IIQII VII
lOS
10· Il.1113E-01
(RYD)
N·· 8.11543
MU·
1 . 04 Il 7
E (RYD)
E (EV)
E PHOT
IlV)
LAMBDA
(A)
(L/R/L-l)
( L/R/L+\\)
SICMA
L-I
SIQMA L+l
SIGMA
(MB)
.0000
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8.311l
14111.13
.000
1. '.111+00
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7.50IlE-01
7.50IlE~01
1.0000
13.5011
21 .• 21
Illl!!. 51
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;l.1I87E-01
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1.22I1E-Ol
2.0000
27.212
35.1l27
348 .•'
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1.47I1E-Ol
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4.811IE-02
4. 811lE -02
Il.0000
81.535
• 811 .•50
137.84
.000
3.7I1IE-02
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8.12I1E-03
8. I2I1E-03
Mil VII
12S
EÔ. 4.082I1E-01
(RYDI
N.· 10 .•555
MU·
1.0445
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-I)
IL/R/L+l )
SICMA L-l
SIGMA L+l
SIQMA
(MB)
.0000
.000
5.555
2232.011
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1.1I75E+00
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9.788E-Ol
Il.788E-01
1.0000
13.5011
Ill. 151
847.011
.000
2.71l7E-Ol
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9.150E-02
Il.150E-02
2.0000
27.212
32.757
378.311
.000
1.248E-Ol
.000
3.20IlE-02
3.205E-02
4.0000
54.424
511.1178
2011.72
.000
5.1121-02
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9.850E-03
Il.850E-03
Il.0000
81.535
87.1110
142.20
.000
2.1152E-02
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4.773E-03
IIQII VII
155
10' 2.11I05E-01
(RYD)
N.· 14 . lISII5
MU·
1.0435
E (RYD)
1
(EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-\\)
(L/R/L+ 1 )
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SlCMA
L+l
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(MB)
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2.1180
4150.15
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2.8221 +00
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1.4I1IE+00
1. 411lE +00
.4000
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8.423
1472.05
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Il.01l0E-Ol
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1.1I38E-Ol
1.0000
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15.5811
147.1l3
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2.11I5E-01
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5.027E-02
5.027E-02
3.0000
40.818
43.7118
283.011
.000
Il.155E-02
.000
7.317E-03
7.3I7E-03
• 5.0000-·,
81.835
14.51'
145.53
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1 . 114!lE - 02
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2.013E-03
2.013E-03
Mil VII
,20S
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1.3U5E-01
(RYD)
Il·· 18.1I1l70
MU·
1.0430
E (RYD)
E (EV)
1
PHOT (EV)
LAMBDA
(A)
(L/R/L-I)
(L/R/L+l)
SICMA L-I
SIQMA L+I
SIQMA (MB)
.0000
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1.855
5583.21l
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4.2171+00
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2.074E+00
2.074E+00
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5.442
7.2118
1111111.01
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5.373E-Ol
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1.324E-01
1.3241-01
1.0000
13.11011
11l.4111
801.'2
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1.7311-01
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2.1I10E-02
2.1I10E-02
2.0000
27.212
211.0117
4211.55
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Il.7021 -02
.000
8.20IlE-03
8.20IlE-03
4.0000
84.424
55.2711
220.31
.000
2.'00E-02
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2.210E-03
2.210E-03
Mil VII
4P
EO· 5.05115E+00 (RYD)
".. 3. 101111
MU'
.81101
1 (RYD)
1
lEV)
1 PHOT (IV)
LAMBDA
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(L/R/L+I)
SIQMA L-I
SICMA L+I
SICMA
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.0000
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118.'34
1711.811
2.247E-01
2.170E-Ol
7.2110E-02
1.350E-Ol
2.08I1E-01
1.0000
13.1105
82.540
150.21
1.5771-01
1 .s05E - 0 1
4.811IE-02
1.255E-01
1.742E-01
3.0000
40.818
1011.752
112.117
1.054E-01
1.472E-01
2.5831-02
Il.1152E-02
1 . 25 lE - 0 1
8.0000
108.847
177.782
1111.74
4.7841-02
8.11511-02
8.5221-03
5 ..5871-0~.
Il.43.E-02
Mil VIl
5P
EO. 2.85113E+00 (RYDI
N·· 4. 13411
MU·
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38.111111
317 .s2
4.0111-01
2.12IE-01
1.3141-01
1.2101-01
2.524E-Ol
1.0000
13.11011
1l2.1105
235.5'
2.445E-Ol
2.185E-Ol
5.585E-02
1.052E-01
1.7I1E-01
2.0000
27.212
1111 . 21 1
187.25
1.IIUE-Ol
1.771E-OI
3.850E-02
8.5115E-02
1.255E-Ol
Il.0000
81 . 1135
120.535
102.78
Il.133E-02
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Il.505E-03
4.324~-02
15.274E-02
,...
M:' VII
5P
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1 .85 IllE +00
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5. 1443
MU·
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E (RYD)
E (EV)
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5.2431-01
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2.01l7E-Ol
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1.544E-Ol
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40.818
115.010
187.13
1.247E-Ol
1.375E-Ol
2. 1411E-02
5.235E-02
7.38IlE-02
15.0000
58.030
113.222
133.00
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Il.308E-02
Il.483E-03
3.384E-02
4.332E-02
8.0000
108.847
134.040
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32
MN VII
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8151.33
1.203E·00
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3.U8E-Ol
Il.271E-02
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10.815
23.818
518.38
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2.827E-Ol
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8.1114E-02
1.842E-Ol
1.0000
13.808
28.1138
4815.43
3.833E-Ol
2.373E-Ol
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8.285E-02
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53.851
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8.1181E-02
8.025E-03
2.120E-02
2.822E-02
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81.082
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5.514E-02
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8.288E-02
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27.212
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4.382E-02
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8.877E-02
8.557E-03
1.ll47E-02
2.8021-02
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118.030
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7.077E-03
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8.883E-Ol
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7.5118E-Ol
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8.0831-01
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8.872E-Ol
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1.508E-Ol
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1.574E-02
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2.308E-02
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8.32U-Ol
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8.007E-02
8.500E-02
12.0000
183.271
185.887
83.28
1.583E-02
5.588E-02
1.2031-03
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1.77lE-Ol
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8.032E-02
2.025E-03
3.178E-02
3.381E-02
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183.271
185.083
88.88
1.313E-02
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5.833E-04
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81.40
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3.1132E-Ol
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27.212
55.011
225.311
7.448E-02
2.833E-OI
8.21I1E-03
1.585E-Ol
1.1I117E-Ol
3.0000
40.818
118.1117
180. IlIl
4. 11711E -02
1.7114E-01
4.045E-03
7.1l271-02
8.332E-02
5.0000
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8.81I1E-02
1.305E-03
2. 1175E-02
2.805E-02
Il.0000
81 .1135
101l.434
113.30
1. 11113E -02
Il.1I0IlE-02
8.1521-04
1 . 71 5E -02
1.711I1E-02
MN VII
IIF
ED'
1.4132E+00 (RYDI
N••
5.8885
MU'
· 1 1 15
E CRYD)
E (EV)
E PHOT (EV)
LAMIIDA lA)
(L/R/L-I)
CL/R/L+I)
SIGMA L- 1
SlaMA L+l
SlaMA
CMB)
.0000
.000
111.227
1144.84
4.8113E-Ol
1.52I1E+00
1.228E-OI
1.1I0IlE+00
1.73IE+00
1.0000
13.11011
32.833
317.112
1.71181-01
5.8117E-OI
2.7114E-02
4.05IlE-Ol
4.335E-Ol
2.0000
27.212
411.431l
21111.1111
8.87I1E-02
3.033E-OI
Il.854E-03
1.!l34E-Ol
1.1I32E-Ol
3.0000
40.818
110.0<45
2011.411
5.218E-02
1.824E-OI
4.404E-03
7.172E-02
7. 1112E- 02
MN VII
8F
ED'
7.8811I1E-Ol
CRYD)
N-.
7.8808
MU'
· 1 1112
E CRYOI
E CEV)
E PHOT 1EV)
LAMBDA (A)
CL/R/L-l)
CL/R/L+l)
SICMA L-1
SlaMA
L+l
SlCMA (MB)
.0000
.000
10.735
1155.02
1.00IlE+00
2.483E+00
2.1128E-OI
2.377E+00
2.1170E+00
1.0000
13.11011
24.340
5011.38
2.235E-Ol
Il.378E-Ol
3.274E-02
3.555E-Ol
3.883&-01
2.0000
27.212
37.11411
3211.74
Il.418E-02
2.8113E-OI
Il. 01151- 03
1. 117E-Ol
1.20BE-OI
3.0000
40.818
51.552
2~0.51
5.05I1E-02
1.5021-01
3.54I1E-03
4.75lE-02
5. 1OllE - 02
5.0000
118.030
78.1114
157.41
2.052E-02
Il.1I08E-02
8.1128E-04
1. 350E -02
1.43I1E-02
MN VII
lOF
ID" 5.0222E-OI
(RYD)
N'"
Il.87711
MU'
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E (RYD)
E (EV)
E PHOT (EV)
LAMBDA (AI
CL/R/L-I)
(L/R/L+I)
SlaMA
L-I
SlaMA
L+ 1
SlaMA
(MB)
.0000
.000
8.833
1814.47
1.1180E+00
3.540E+00
5.1115E-Ol
3.074E"00
3. 5.4E+ 00
1.0000
13.11011
20.431l
1I0e.1I1
2.3IU-Ol
Il.088E-OI
2.113I1E-02
2.720E-Ol
3.014E-Ol
2.0000
27.212
34.045
3114.18
8.1147E-02
2.480E-OI
Il. 85I1E-03
7.517E-02
8.203E-02
4.0000
54.424
111.257
202.40
2.1I03E-02
8. 1711E-02
1. 118E -03
1.471 E-02
1. 583E - 02
5.0000
118.030
74.8113
1115.112
1.11112E-02
5.4114E-02
5.774E-04
8.114E-03
8.11111 E-03
MN VIl
12F
10' 3.4743E-Ol
CRYD)
N,••
1'.8751l
MU'
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E (RYO;
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E PHOT (EV)
LAMBOA (A)
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(L/R/L+I)
SlaMA L,-1
SlaMA
L+ 1
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CMB)
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.000
4.727
21122.91
2.500E+00
4.702E+00
7.1158E-Ol
3.753E+00
4.84I1E"00
1.0000
13.11011
18.333
11711.30
2.1118E-OI
5.524E-OI
2.385E-02
2.008E-Ol
2.247E-OI
2.0000
27.212
31.1139
388.20
7.588E-02
2.108E-OI
4.953E-03
5.082E-02
5.577E-02
4.0000
54.424
59. 151
2011.111
2.IIIIIE-02
Il.1151E-02
7.471E-04
Il. 3117E -03
1. 01~E-02
34
lIN VII
llF
10' 1.8445E-Ol
(RVD)
N'"
15.8743
MU'
. 1257
1
(UO)
Il UV)
E PHOT (IV)
LA.IDA
lAI
(L/R/L-ll
IL/R/L+l)
SIGMA L-l
SI GIlIA L+l
SIGMA (MI)
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.000
2.141
4181.38
4.5571+00
7.345E+00
1.479E+00
5. 125E+00
8.104E+00
1.0000
13.101
18.252
712.92
1.820E-Ol
4.351 E-Ol
1.450E-02
1.101S1-Ol
1. 21S0E-Ol
2.0000
27.212
29.857
415.28
5.713E-02
1.532E-Ol
2.124E-03
2.515E-02
2. 77IE -02
3.0000
40.818
43.413
281.27
2.702E-02
7.738E-02
8.544E-04
11.338E-03
1.01U-02
MN VII
20F
EO'
1.240I5E-Ol
(RVD)
N'"
111.8738
MU'
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E PHOT (EV)
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SIGMA L - 1
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.000
1.1S88
7341.111
7.143E+00
1.040E+Ol
2.319E+00
8.554E+00
8.874E+00
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8.803
8.491
1480.22
4.2114E-Ol
8. 851E -01
4.215E-02
2.388E-Ol
2 .• ,0E-0'
1.0000
13.801
15.294
810.88
1.470E-Ol
3.428E-Ol
8.88IE-03
8.41S11-02
7.3441-02
2.0000
27.212
28.800
428.02
4.385E-02
1.1571-01
1.488E-03
1.3881-02
1.5381-02
3.0000
40.818
42.508
291. 811
2.0341-02
5.753E-02
4. 73IE -04
5.051E-03
5.52IE-03
35
FE VIII
.5
EO'
7.1330E+00 (RYD)
N·· 2.885.
MU'
1.00.11
E ( RYD)
E (EV)
E PHOT
(EV)
LAMBDA
(A)
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CL/R/L+I)
SIGMA L- 1
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.000
117.051
127.75
.000
1.11118E-Ol
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1 . 751lE - 0 1
1.75I1E-Ol
1.0000
13.1l01l
110.1157
112.05
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1 .••• E-Ol
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5 •.• 2 •
151 .• 75
81.85
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Il.1111 E-02
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8.7113E-02
8.7lil3E-02
FE VIII
55
EO. 3.1171I1E+00 (RYD)
N·· •. 0,.,
MU'
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E (RYD)
E (EV)
E PHOT
lEV)
LAMBDA lA)
(L/R/L-l)
CL/R/L+I)
SIGMA L- 1
SIGMA L·,
SIGMA (Mill
.0000
.000
5•. 0.2
2211 .•3
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2.11112E-Ol
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2 .• 07E-Ol
2 .• 07E-Ol
1.0000
13.1l0e
117.11.8
183.28
.000
1.1180E-Ol
.000
1.1l1l7E-Ol
1.1I1l7E-Ol
3.0000
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Il•. 81l0
130.71
.000
1.253E-Ol
.000
Il.31l2E-02
Il.31l2E-02
FE VIII
ilS
EO. 2.538.E+00 (RYD)
N·· 5.0212
MU'
.lil788
E (RYD)
E (EV)
E PHOT
(EV)
LAMIlDA
(A)
(L/R/L-l)
(L/R/L.,)
SIGMA L- 1
SIGMA L·,
SIGMA (Mil)
.0000
.000
3•. 538
358.1111
.000
3.807E-Ol
.000
3.1.IlE-Ol
3.1.IIE-Ol
'1.0000
13.1108
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257.53
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2 .• 2.E-Ol
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1. 777E-0 1
1.777E-Ol
3.0000
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75.3511
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1.2117E-OI
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7.1I1l2E-02
7.lilIl2E-02
7.0000
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1211.7711
115.5.
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Il.001E-02
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2.1137E-02
2.lil37E-02
FE VIII
Ils
EO.
1.2111l2E+00 (RYD)
N·· 7.02811
MU'
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E (RYD)
E (EV)
E PHal
(EV)
LAIIlII DA (A)
(L/R/L-l )
IL/R/L+II
SIGMA L-l
SIGMA L·'
SIGMA (Mil)
.0000
.000
17.1l315
703.01l
.000
Il.585E-Ol
.000
•. 8015E-Ol
•. 805E-Ol
1.0000
13.1I01l
3'.2.,
31111.87
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2.1135E-Ol
.000
1.lIlil2E-Ol
1.11112E-Ol
2.0000
27.212
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1.7.3E-Ol
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8.151l7E-02
8.587E-02
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172.01l
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8.75I1E-02
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3.471E-02
3 .• 71E-02
FE VIII
'10S
EO.
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(RYDI
N·· Il.02lill
MU'
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E IRYD>
E (EV)
E PHOl
lEV)
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10.1l81
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Il.1I117E-Ol
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Il.8IleE-Ol
Il.lle8E-Ol
1.0000
13.1l08
24.287
510.110
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3.038E·01
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2.0000
27.212
37.8lil3
327.20
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1.1l80E-Ol
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5.lil.7E-02
5.1I.7E-02
7.0000
lil5.24.'
105.1123
117.05
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3 .• 77E-02
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8.0.5E-03
8.0.5E-03
FE VIII
12S
EO. 5.21103E-01
IRYD)
N·· 11.0302
MU-
.lil8lil8
E (RYDI
E (EV)
E PHOT (EV)
LAMIIDA
(A)
(L/R/L-l)
IL/R/L·')
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1732.35
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1.3112E+00
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8.711lE-OI
8.71I1E-Ol
1.0000
13.1I01l
20.7113
5117.15
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2.1112E-Ol
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1.1 OIlE-O 1
1.108E·01
2.0000
27.212
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380.75
.000
1.37I1E-Ol
.000
•. 0111 E-02
•. 0111 E-02
5.0000
1l8.030
75.187
1114.110
.000
•. 300E-02
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8.737E-03
8.737E-03
FE VIII
IIlS
EO'
2.832I1E-Ol
( RYDI
N·· 15.0313
MU'
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E (RYD)
E (EV)
E PHOT
(EV)
LAMIIDA (A)
(L/R/L-l)
IL/R/L+I)
SIGMA L- 1
SIGMA L+l
SIGMA (Mil)
.0000
.000
3.85.
3217.04
.000
2.3.7"+00
. 000
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1.33.E+00
1.0000
13. 110 Il
17 .• 110
710.12
.000
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Il.523E-02
Il.523E-02
3.0000
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277.55
.000
5.1138E·02
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Il.8lillE-03
Il.8111E-03
5.0000
1l8.030
71.88.
172.48
.000
2.1115E-02
.000
3.838E-03
3.838E-03
FE VIII
20S
EO.
1 . 71170E-0 1 (RYD)
N·· 111.0317
MU'
.lil883
E (RYD)
E (EV)
E PHOT
(EV)
LAMIlDA
(A)
(L/R/L-I)
(L/R/L"')
SIGMA L- 1
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3.510E+00
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1.81l1E+00
1.8111E+00
1.0000
13.808
11l.010
77 •.•3
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1.1177E-OI
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3.1132E-02
3.1132E-02
3.0000
.0.818
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281l.811
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5.2118E-03
5.288E-03
FE VIII
.P
EO'
Il.351l3E+00 (RYD)
N·· 3.1731
MU'
. 821llil
E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA (A)
(L/R/L-I)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA
(Mil)
.0000
.000
81l.483
1.3.38
1.71l8E-Ol
2.000E-Ol
5.811.E-02
1 .••lilE·Ol
2.01I1E-Ol
1.0000
13.1I01l
100.0811
123.88
1. 3lil.E-0 1
1.7110E-Ol
•. 073E-02
1.300E-Ol
1.707E·01
•. 0000
5 •.• 2 •
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87.lIlil
7.lil88E-02
1.2.2E·01
1.87.E-02
Il.110E-02
1. Olil8E·Ol
8.0000
108.8.7
1115.331
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4. 1158E-02
8.501E·02
8.878E·03
5.1113E-02
Il.aOIE-02
FE VIII
5P
EO' 3.113.2E+00 (RYD)
N· . •. 111115
MU'
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E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA (A)
(L/R/L'I)
(L/R/L+I)
SIGMA L- 1
SIGMA L+l
SIGMA (Mil)
.0000
.000
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250.75
3.132E·01
2.1I11"-01
1.01IlE-Ol
1.412E·Ol
2 .• 28E-01
1.0000
13.1l01l
83.053
llilll.54
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2.101E-Ol
5.7112E·02
1. 1811E-0 1
1.7.5E-Ol
2.0000
27.212
711.1l5lil
181.7.
1.513E-Ol
1.721l"-01
3.1l77E-02
Il.51l5E-02
1.32.E-Ol
FE VIII
IlP
EO'
2.31117E+00 (RYD)
N·· 5.2057
MU'
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E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (M8)
.0000
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32.133
3815.88
•. 853E-Ol
3.233i-Ol
1.118IlE-Ol
1 .• 07E-Ol
2.lillil3E-OI
1.0000
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271.08
2.1l115E-Ol
2.338E-Ol
l'-lil57E -02
1.0.7E-Ol
1.7.3E-Ol
2.0000
27.212
511.3••
208.113
1.7.2E-Ol
i , 780E -01
3.771E-02
7.87IlE·02
t.lIlIlE-Ol
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81.11311
113.71l8
108.lil8
5.812E-02
8.33I1E-02
8.051E-03
3.311 E-02
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FE VIII
8P
EO.
1.2300E+00 (RYD)
H·· 7.2133
MU'
. 78117
E (AYD)
E (EV)
E PHOT
(EV)
LAMBDA (A)
(L/R/L-l)
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(MI)
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Il.308E-Ol
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30.341
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3.437E-Ol
2.52.E-Ol
7.507E-02
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1.221E-Ol
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3.5lilIlE-02
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118.371
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FE VIII
'OP
EO. 7.5345E-0' (RYDI
Na.
Il.2'114
MU·
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E (AYDI
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15.70IlE-Ol
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1.3118E-Ol
Il.257E-Ol
1.0000
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3.1148E-Ol
2.45I1E-Ol
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3.0000
40.818
51 .01111
242.78
1.003E-OI
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2.177E-02
3.254E-02
4.0000
54.4-24
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7.545E-02
Il.08I1E-03
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134.113
3.117I1E-02
4.84I1E-02
2.1I01E-03
Il. 053E -03
1.1115E-02
FE VIII
12P
EO· 5.0857E-Ol
(RYDI
Na.
11.2'80
MU'
.7820
E (RYD)
E (EV)
E PHOT (EVI
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(MB)
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1.388E-Ol
8.41'E-Ol
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20.5211
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3.547E-Ol
2.271E-Ol
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4.43I1E-02
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2511.73
8. 4411E -02
8.301E-02
7.138E-03
1.380E-02
2.OIl4E-02
4.0000
54.424
111.343
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15.503E-02
Il.083E-02
3.8111E-03
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1.340E-02
7.0000
115.241
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2.211I1E-02
3.175E-02
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4.313E-03
5.441E-03
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115.7117
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8.321E-04
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4.3113E-03
FE VIII
'IIP
EO· 2.71130E·Ol
(RYDI
Na.
15.21114
MU'
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E (RYD)
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SICMA L-'
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(Mil)
.0000
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3.7511
32118.01
3.1150E+00
Il.28I1E-Ol
1.22I1E+00
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1.3114E+00
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8. 21l4E-03
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Il. 772E -03
Il.0000
81 . 11315
85.3115
145. '11
1.1188E-02
2.552E-02
7.011111-04
2.330E-03
3.037E-03
FE VIII
20P
EO· 1.73251-0' (RYD)
Na.
111.2200
. MU·
.7800
E (RYD)
E (EVI
E PHOT (EV)
LAMBDA
(A)
(L/R/L -!)
(L/R/L+l)
SICMA L- 1
SICMA L+l
SIOMA
(Mil)
.0000
.000
2.357
521511.811
Il.153E+00
1.158E+00
1 . 81lllE+00
1.324E-Ol
2.0021+00
1.0000
13.11011
15.11113
7711.70
2.4118E-Ol
1.4115E-Ol
2.03I1E-02
1.435E-02
3.471E-02
2.0000
27.212
211.51111
4111.31
8.114SE-02
Il.1I08E-02
4.112I1E-03
15.1112E-03
1 . 014E -02
4.0000
54.424
511.781
2'8.311
2.830E-02
3.0dE-02
Il.524E-04
2.210E-03
3.1IlU-03
Il.0000
81.1135
83.1Ii13
147.112
1.444E-02
1.844E-02
3.1170E-04
1.1117E-03
1.5114E-03
7.0000
115.2.'
117.51111
127.04
1.1' IlE-02
1.517E-02
2_1545E-04
Il.405E-04
1.1115E-03
FE VIIl
3D
EO'
1.0854E+Ol
(RYD)
Na.
2.4283
MU'
.5717
E (RYDI
E (EV)
E PHOT (EV)
LAMBDA (A)
(L/R/L-l)
IL/R/L+ll
SICMA L- 1
SIOMA- L+l
SIOMA
(Mil)
.0000
.000
147.1173
83.1111
Il.83I1E-02
3.4117E-Ol
1.73I1E-02
Il.80U-Ol
Il.1183E-01
1.0000
13.11011
11l1.27i1
711.88
5.1111 E- 02
3.012E-Ol
1.41111-02
5.517E-Ol
5.115111-0\\
3.0000
40.8'8
'88.4110
115.78
4.555E-02
2.2112E-0'
Il.82I1E-03
3.734E-Ol
3.832E-Ol
8.0000
108.847
2511.520
48.33
2.1l1l0E-02
1.2118E-Ol
4.11115E-03
1.1131 E-Ol
1.1177E-Ol
FE VIII
4D
EO. 5.1241E+00 (RYD)
Na.
3.534'
MU'
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E (RYD)
E (EV)
E PHOT (EV)
LAMIIDA
(A)
CL/R/L-ll
IL/R/L+11
SIGMA L- 1
SIGMA L+ 1
SIGMA
(M8)
.0000
.000
1111.718
177.84
1.511I1E-Ol
4.70IlE-Ol
4.480E-02
5.828E-Ol
Il.27IlE-Ol
1.0000
'3.11011
83.324
148.80
1.178E-Ol
3.71I1E-Ol
2.1I0IlE-02
4.337E-Ol
4.1128E-Ol
5.0000
118.030
137.747
110.0'
4.1I08E-02
1.753E-Ol
8.33U-03
1.5117E-Ol
1.1180E-0'
8.0000
108.847
178.5115
811.43
3.0113E-02
1. '44E-Ol
4.211.E-03
8.8'IIE-02
Il. 2.5E -02
FE VI Il
50
EO' 3.011111+00 (RYD)
Na.
•. 5502
MU'
.44118
E (RYD)
E (EVI
E PHOT (EVI
LAMIDA lA)
(L/R/L-l)
(L/R/L+I)
SIQMA L-l
SIGMA L+ 1
SIGMA (Mill
.0000
.000
42.057
211•. 80
2.8771-01
Il.13I1E-Ol
8.748E-02
5.1175E-Ol
Il.850E-Ol
1.0000
13.11011
15.IIU
222.74
1.775E-Ol
4.343E-Ol
4.4'OE-02
3.115I1E-Ol
•. 400E-Ol
5.0000
118.030
110.087
112.113
5. 3158E-02
1.1148E-0'
7.1145E-03
1.127E-Ol
'.20llE-Ol
Il.0000
81.1135
123.11113
'00.2.
4.350E-02
1.375E-Ol
5.882E-03
8.812E-02
Il .• 00E-02
FE VIII
110
EO. 2.07301+00 (RYD)
Na.
5.55113
MU·
.• 437
E (RYD)
E (EVI
E PHOT (EV)
LAMIDA
(A)
(L/R/L-l)
(L/A/L+')
SIGMA L- 1
SIGMA L+l
SIOMA (MB)
.0000
.000
28.2011
4311.58
4.47I1E-Ol
7.1115E-Ol
1.4231-01
Il.11l7E-Ol
7.5110E-Ol
1.0000
'3.11011
41.812
21111.5.
2.277E-Ol
4.7.4E-0'
5 .•47E-02
3.548E-Ol
4.0112E-Ol
4.0000
5•. 424
82.1I211
150.015
Il.8110E-02
1.8112E-Ol
Il.815I1E-03
1.080E-Ol
1.17IlE-Ol
5.0000
18.030
1111.235
128.84
5.247E-02
1.483E-Ol
Il.H1E-03
7.1183E-02
8. 11411E -02
FE VIII
80
EO· 1.1'1I4E+00 (RYD)
Na.
7.51112
MU'
.4388
E (AYDI
E (EV)
E PHOT (EVI
LAMIDA
( A)
( L/R/L-I)
CL/A/L+I)
SIGMA L-'
SIGMA L+'
SIGMA (MIl
.0000
.000
15.231
8'4.05
8.5i10E-Ol
1.0118E+00
2. USE-Ol
Il.55l5E-Ol
Il.380E-Ol
1.0000
13.11011
28.837
.211.88
2.880E-Ol
4.888E-Ol
8.013E-02
2.705E-Ol
3.307E-Ol
3.0000
.0.118
58.0411
221.21
Il.01IlE-02
2.052E-01
1.145E-02
8.811.E-02
1.004E-Ol
•. 0000
54 .• 24
1l1l.1l!55
178.00
Il. 127E -02
, .503E-0'
Il.574E-03
5.1133E-02
Il.15111E-02
8.0000
108.847
12•. 078
111.113
2.158E-02
Il.243E+02
1.453E-03
1 . 823E -02
1 .1I8IE -02
FE VIII
100
EO. Il.11810E-Ol (RYD)
Na.
Il.51132
MU· .
.43B8
E (RYDI
E (EV)
E PHOT (EVI
LAMIDA (A)
(L/R/L-l)
(L/A/L+I)
SIGMA L-'
SIGMA L+l
SIGMA
(MB)
.0000
.000
Il.521
1302.18
1.384E+00
1.311IE-00
•. 582E-Ol
11.1I43E-Ol
1.1531-00
1.0000
13.11011
23.127
5311.10
3.043E-Ol
4.7'1111-01
15.384E-02
1.1Ii12E-Ol
2.5301-01
2.0000
27.212
311.733
337.53
, .3112E-Ol
2.1I03E-Ol
1.713E-02
Il.382E-02
1. 110E-Ol
3.0000
40.818
50.3311
2411.30
7.823E-02
1.118I1E-Ol
7.7.41-03
1.3115E-02
Il. l1111E - 02
5.0000
118.030
77.551
1511.88
3.1l17E-02
Il.0111E-02
2.550E-03
2.37U-02
2. ll)4E -02
8.0000
108.847
118.31111
'04.75
1.11771-02
•. 711 E-02
8.3721-04
Il.1I0IlE-03
1.07.E-02
FI VIII
120
10. 4.7858E-Ol
(RYD)
Na.
, 1.51U2
MU·
.4358
E (RYD)
E (EV)
1 PHOT (EVI
LAMBDA (A)
(L/A/L-!)
(L/R/l+l)
SIGMA L- 1
SIOMA L+l
SICMA (MB)
.0000
.000
Il.511
1110•. 13
2.017E+00
1.728E+00
Il.1l5IlE-Ol
7.334E-Ol
1 .311111 -00
1.0000
'3.11011
20.117
11111.31
2.1154E-Ol
4.380E-0'
•.• '3E-02
1 .• 55E-Ol
1.8117E-Ol
2.0000
27.212
33.723
3117.1111
1.20SE-Ol
2.21SE-0'
1.230E-02
Il.237E-02
7.41l7E-02
3.0000
.0.818
.7.3211
2111 .117
Il.1133E-02
1.387E-Ol
5.235E-03
3.435E-02
3.1158E-02
7.0000
115.241
101.753
121. 815
1.117IlE-02
4.483E-02
7.1141-04
7.710E-03
8.428E-03
37
FE VIII
II1D
EO'
2.1I~II1E-Ol
(AYDI
1'1.' HI. 51151
MU'
.~3~1I
E (AYD)
E (EV)
E PHOT (EV 1
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lA)
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(L/A/L+1)
SIGMA L- 1
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SIGMA (MIl
.0000
.000
3.511~
3~~1I.12
3.5111E+00
2.~~IIE+00
1.1115E+00
8.12I1E-Ol
1.1178E+00
1.0000
13.11011
17.200
720.85
2.51I1E-Ol
3.511 E-O 1
2.737E-02
7.11115E-02
1.073E-Ol
2.0000
27.212
30.801
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Il.15lE-02
1.11 18E-Ol
Il.~8~E-03
3.0~OE-02
3.118I1E-02
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58.018
213.70
2.1188E-02
Il.15I1E-02
1.302E-03
Il.700E-03
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5.0000
118.030
71 .1I2~
173. Il
2.0~7E-02
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7 .5~ lE-O~
Il. ~53E -03
7.207E-03
8.0000
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110.27
Il.007E-03
2.~52E-02
2.2113E-0~
2.5~IIE-03
2.778E-03
FE VIII
20D
EO$ 1.11718E-Ol
(AYD)
1'1.' 111.51155
MU'
· "3~5
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
IL/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGIU (MI)
.0000
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2.275
5~50.17
5.55I1E+00
3.227E+00
1.717E+00
8.112I1E-Ol
2.IIIOE+00
1.0000
13.11011
15.881
780. 7~
2.0113E-Ol
2.711I1E-Ol
1 . IIIIIE - 02
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Il.380E-02
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27.212
251.~a7
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7.050E-02
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7.237E-02
1 . ~ IllE - 03
8.50IlE-03
Il.1I25E-03
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511.11118
218.118
2.218E-02
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7. 0 I~E -0"
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7.0000
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8.325E-03
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1.73~E-03
1 . 1I0~E -03
FE VIII
~F
EO' ... la8~E+00 (RYO)
1'1.'
3.110110
MU'
.01110
E lAYD)
(EV)
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LAMBDA
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(L/R/L+l)
SIGMA L- 1
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1511. 1187
217.57
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1.512E-02
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5.022E-Ol
1.0000
13.11011
70.5113
175.1I~
Il.~25E-02
3.0117E-Ol
7.8~8E-03
2.3a5E-Ol
2.~1I3E-Ol
3.0000
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117.8015
121.77
3.21I1E-02
1.~1I2E-Ol
2.72I1E-03
7.821E-02
8.0Ild-02
Il.0000
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138.122
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8.122E-~
2.2I1lE-02
2.372E-02
FE VIII
5F
EO' 2.11757E+00 (RYD)
1'1.'
~.aIl07
MU'
· 10113
E IRYOl
E (EV)
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lEV)
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.0000
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311.~01
3~0.57
2.18I1E-Ol
8.278E-Ol
~.700E-02
8.1158E-Ol
Il.~27E-Ol
1.0000
13.11011
50.011
2~7.12
1.180E-Ol
~.517E-Ol
1.87IE-02
3.81~E-Ol
3. 851E-0 1
2.0000
27.212
83.817
111~.811
7.280E-02
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77.223
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1.888E-Ol
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Il.8815(-02
1.037E-Ol
5.0000
88.030
10~.~35
118.72
2.1528E-02
1. 003E-0 1
1.7518E-03
3.71I1E-02
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7.0000
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1.503E-02
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1 . 7~8E -02
1.82I1E-02
FE VIII
ltF
EO'
1 . 8~1I5E +00
(RYO)
1'1.'
5.8826
MU'
.117"
E (RYO;
E (EV)
E PHOT (EV)
LAMIIDA
(A)
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SIGMA L- 1
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.0000
.000
25. 11~
~1I2.72
3.71I1E-Ol
1.170E+00
Il.37~E-02
1.237E+00
1.330E+00
1.0000
13.11011
38.718
3111.80
1.113I1E-Ol
5.~~2E-Ol
2.80IlE-02
".123E-Ol
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3.0000
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115.1181
187.111
5.1I"8E-02
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5.III1I1E-03
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Il.8112E-02
5.0000
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2.71~E-02
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3.2115E-02
3."50E-02
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120.~05
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1.538E-02
5783E-02
7. 1175E -O~
1 . "~IIE -02
1 .523E-02
FE VIII
8F
EO·
1.0318E+00 (RYD)
1'1.'
7.87511
MU'
.12 ....
E (RYO)
E (EV)
E PHOT
(EV)
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(L/R/L+ 1 )
SIGMA L- 1
SIGMA L+'
SIGMA (MI)
.0000
.000
1~.0311
883.15
7.737E-Ol
1.1I00E+00
2.2113E-Ol
1.820E+00
2.0~IIE+00
1.0000
13.1011
27.1I~5
~~8.~1I
2.223E-Ol
8. 2~ lE-Ol
3. 8711E-02
3.88I1E-Ol
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3.0000
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5~. 857
228.02
5.80~E-02
1.8111E-Ol
~.1I78E-03
8.51I1E-02
7.01~E-02
8.0000
81 .1135
115.1175
1211.511
1.7117E-02
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8. 31I1E-0~
1 .2111 E- 02
1 .37~E-02
7.0000
115.2~1
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8.5111 E- 03
Il.08I1E-03
FE VIII
lOF
EO' 8.51181E-Ol
(RYD)
N·· Il.8727
MU'
.1273
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/A/L+ 1)
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(MI)
.0000
.000
8.113~
1387.83
1.2117E+00
2.707E+00
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2. 350E +00
2.755E+00
1.0000
13.11011
22. 5~0
550.08
2.~25E-Ol
8.213E-Ol
3.570E-02
3. 125E-·Ol
3.~82E-Ol
2.0000
27.212
311. 1~1I
U3.02
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2.715111-01
Il.~37E-03
Il.882E-02
1.083E-Ol
3.0000
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~II . 752
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5.22I1E-02
1.5~8E-Ol
3.115IE-03
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5.0000
118.030
711.11113
181. 10
2.118E-02
8.757E-02
Il.2118E-0''
1.2112E-02
1.355E-02
8.0000
81.1135
110.51111
138.80
1.~1I3E-02
... 8118E-02
5.~3I5E-0~
7.8021-03
8.3~IIE-03
FE VIII
12F
EO' ".5~I~E-Ol (RYD)
1'1.' 11.8712
MU'
.1288
E (RYD)
E (EVI
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+ 1)
SIGMA L- 1
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.0000
.000
8. 1711
20011.58
1.1137E+00
3.5115E+00
8.2~~I-Ol
2.887E+00
3,"1I1E+00
1.0000
13.1108
111.785
1128.117
2.3118E-Ol
5.81I1E-Ol
3.01171-02
2.~05E-Ol
2.7121-01
2.0000
27.212
33.3111
371.32
8.8.IE-02
2.3115E-Ol
7.10IlE-03
Il.880E-02
7.5110E-02
~.OOOO
5~. ~2..
10.1103
20~ . 511
2.11118E-02
8.1101-02
1.188E-03
1.~3lE-02
1 . 550E - 02
5.0000
118.030
7~. 2011
1117.08
1.7117E-02
5.'0~E-02
Il.237E-0~
8.073E-03
8.11117E-03
8.0000
108 .8~7
115.0211
107.711
Il.7117E-03
2 . 211111 - 02
1.~31E-0~
2.178E-03
2.321E-03
FE vIII
ll1F
EO' 2.5~12E-Ol (RYD)
1'1.' 15.81187
MU'
.1303
E (RYD)
E (EV)
E PHOT (EV)
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(A)
(L/R/L-1)
(L/R/L+1)
SIGMA L- 1
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(nI
.0000
.000
3.~58
3585.1111
3.5~IIE+00
5.1112E+00
1.173E+00
3.1I11E+00
5. 08~E+00
1.0000
13.11011
17.0113
7211.12
2.088E-Ol
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2.00~E-02
1.3118E-Ol
1.5117E-Ol
2.0000
27.212
30.11111
~O~. 27
Il.11121-02
1. 78111-01
3.1I~1I1-03
3.524E-02
3.1118E-02
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5~.~2"
117.881
21~.21
1 . 1153E- 02
5.712E-02
5 . II~ 5E - O~
Il.781E-03
7.37IE-03
7.0000
115.2~1
118.11111
125.82
Il.282E-03
2.032E-02
1 . O~IE-O~
1 .~1I3E-03
1.5118E-03
8.0000
108.8~7
112.305
110.~0
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1.5115E-02
Il. 732E-05
Il. 878E-0~
1. 055E -03
FE VIII
20F
EO·
1.11212E-Ol
(AYD)
N.· 111.811111
MU'
· 13011
E (RYO)
E (EV)
E PHOT (IV)
LAMIOA
(A)
(L/R/L-1)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA
(MIl
.0000
.000
2.2011
11121.10
5.58~E+00
7.1I~~E+00
1.852E+00
".III1I1E+OO
Il.851~+00
1.0000
13.1011
15.812
78~. 15
1. 73~E-Ol
3.8~IIE-Ol
1.280E-02
8."'2E-02
Il. 11112E -02
2.0000
27.212
211."'8
~21. ~7
5.311~E-02
1.311I1E-Ol
2.305E-03
1.1180E-02
2.211E-02
3.0000
~0.818
~3.023
288.18
2.5112E-02
7.01IlE-02
7.1I07E-0~
7.810E-03
8.371E-03
!S.OOOO
118.030
70.235
1711.53
II. 3112E-03
2.82I1E-02
1 .III1I1E -O~
2. 01~E-03
2.181E-03
Il.0000
81.1135
83.8~1
1~7.88
8.~~IE-03
2.005E-02
Il.311I1E-05
1.210E-03
1 .30~E-03
38
ZN XII
45
EO·
1.3871E+Ol
(RYD)
N.· 3.2105
MU'
.7885
E (AYD)
E (EV)
E PHOT (EV)
L"'1II10'" ( ... )
(L/R/L-O
(L/R/L+l)
SIGIII... L-l
SIGIII... L+l
SIGIII... (MIl
.0000
.000
180.083
811. 23
.000
8.882(-02
.000
1.122E-Ol
1.1221-01
1.0000
13.808
203.888
80.87
.000
8.844E-02
.000
1. 001 E-Ol
1. OOlE-Ol
2.0000
27.212
217.285
57.08
.000
8.114E-02
.000
8.880E-02
8.880E-02
ZN XII
5S
EO' 8.08421+00 (RYD)
N··
4.2257
MU'
.7743
E (AYD)
E (EV)
E PHOT (EV)
L'"1118 0 ... C"')
(L/R/L-l)
(L/R/L+l)
SIaM'" L- 1
SIaM'" L+l
SIGM... (11181
.0000
.000
108.720
113.00
.000
1.48lE-Ol
.000
1.533E-Ol
; .533E-Ol
2.0000
27.212
138.832
80.55
.000
1.08eE-Ol
.000
1.03eE-Ol
1.038E-Ol
4.0000
84.424
184.144
75.54
.000
8.528E-02
.000
7.488E-02
7.4881-02
ZN XII
85
10' 5.2810E+00 IRYD)
N··
!5.2317
IIIU'
.7883
E (RYD)
E (!V)
E PHOT (EV)
L"'MBO'"
( ... )
(L/RIL-l)
(L/R/L+ 1 )
SIGM'" L-l
SIaM'" L+l
SIGM... (MB)
.0000
.000
71.581
173.21
.000
2.108E-Ol
.000
2.0021-01
2.0021-01
2.0000
27.212
88.783
125.50
.000
1.338E-Ol
.000
1.1121-01
1 112E-Ol
4.0000
54.424
126.001S
88.40
.000
8.443E-02
.000
7.08lE-02
7.08lE-02
ZN XII
as
10' 2.74871+00 (RYD)
N·· 7.2387
MU'
.7833
E (AYD)
E (EV)
E PHOT (IV)
L"'M'O'"
( ... )
(L/R/L-l)
(L/R/L+l)
SIaM'" L - 1
SIaM'" L+l
SIaM'"
(Mil
.0000
.000
37.412
331.41
.000
3.81lE-Ol
.000
3.088E-Ol
3.088E-Ol
2.0000
27.212
84.824
181.88
.000
1.828E-Ol
.000
1. 078E-0 1
1.0781-01
4.0000
54.424
81.838
138.01
.000
8.703E-02
.000
5.4331-02
5.433E-02
ZN XII
lOS
EO'
1.8871E+00 (AYD)
N··
8.2387
MU'
.7813
E ( AYD)
E (IV)
E PHOT (EV)
L"'MID'"
( ... )
(L/R/L-l)
(L/R/L+l)
SIaM'" L - 1
SIaM... L+'
SIaM'"
(M8)
.0000
.000
22.885
840.14
.000
5.448E-Ol
.000
4.278E-Ol
4.278E-Ol
2.0000
27.212
50.188
247.15
.000
1.107E-Ol
.000
8.183E-02
8.183E-02
4.0000
54.424
77.318
180.23
.000
8.814E-02
.000
3.884E-02
3.884E-02
10.0000
138.058
158.014
77.87
.000
3.02I1E-02
.000
Il. 148E-03
8.148E-03
ZN XII
12S
EO'
1.1388E+00 IRYD)
N·· 1).2387
MU'
.7803
E CRYD)
..(
(EV)
E PHOT (EV)
L"'MID'"
( ... )
(L/R/L-l )
(L/R/L+ll
SIGM... L- 1
SIQlIl... L+l
SIaM'" CMB)
.0000
.000
15.809
788.45
.000
7.583E-Ol
.000
5.81eE-Ol
S.81IE-Ol
2.0000
27.212
42.721
280.23
.000
1.81S8E-01
.000
7.381E-02
7.381E-02
8.0000
81.831S
87.14.
127.83
.000
4.778E-02
.000
1.383E-02
1 .383E-02
8.0000
108.847
124.358
18.70
.000
3.288E-02
.000
8.4515E-03
8.4!15E-03
ZN XII
185
EO' 8. 1815E-Ol
IAYD)
N.· 15.2408
NU'
.7!19.
E (RYD)
E (EV)
E PHOT lEV)
L...M8D'" ( ... )
(L/R/L-l )
(L/R/L+ 1 )
SIaM'" L-l
SIGMA L+l
SIGM... (M8)
.0000
.000
8.435
1488.81
.000
1.218E+00
.000
8.888E-Ol
8.888E-Ol
2.0000
27.212
35.847
347.82
.000
1 .• 14E-Ol
.000
•. 4811-02
4.481 E-02
8.0000
81.835
80.070
137.85
.000
3.43lE-02
.000
8.882E-03
8.8821-03
ZN XII
20S
EO.
3.8888E-Ol
(RYD)
N·· 18.2411
MU'
.75811
E (AYD)
E (EV)
E PHOT (EV)
L...M8D... ( ... )
(L/RIL-l )
(L/R/L+ 1 )
SIaM'" L-l
SIaM'" L+l
SIGM... CMB)
.0000
.000
S.282
2342.83
.000
1.1113E+00
.000
1. 217E+OO
1. 2171+00
.5000
8.803
12.0115
1025.08
.000
5.351E-Ol
.000
2.1781-01
2.178E-Ol
1.0000
13.808
18.888
8158.08
.000
2.884E-Ol
.000
a.5571-02
8.!I571-02
2.0000
27.212
32.504
381.45
.000
1.1821-01
.000
2.75I1E-02
2.788E-02
4.0000
54.424
58.718
207.83
.000
4.5811-02
.000
7.8081-03
7.80SE-03
8.0000
108.847
114.138
108.83
.000
1 .884E-02
.000
2.058E-03
2.058E-03
ZN XII
4P
EO'
1. 2831E+0 1 (AYD)
N••
3.3488
MU'
.8804
E (RYD)
E (EV)
E PHOT (EV)
L"'MBD'"
( ... )
(L/R/L-l)
(L/R/L+O
SlGM'"
L-l
SIGM'" L+l
SIGtII... (MI)
.0000
.000
174.1528
71.00
8.380E-02
1.300E-Ol
2.888E-02
1.238E-Ol
1 .• 821-01
2.0000
27.212
201.837
81.43
8 .1584E -02
1.0871-01
1. 83eE -02
1.01eE-Ol
1.2011-01
4.0000
54.42.
228.04'
84.13
5.355E-02
8.403E-02
1.3781 -02
8 .• 8!11-02
1.8811-02
ZN XlI
IP
10' 7.5443E+00 (RYD)
N·'
4.3888
MU'
.8311
E (RYD)
E (EV)
E PHOT (IV)
L"'MBO'"
( ... )
(L/R/L-l)
(L/R/L+l)
SIaM'" L-l
SIaM'" L+l
SIaM'"
(M8)
.0000
.000
102.847
120.18
1.45lE-Ol
1.788E-Ol
4.5281-02
1.38eE-Ol
1.840E-Ol
2.0000
27.212
12'.8!18
8 •. 48
8.818E-02
1.358E-Ol
2.8211 -02
1.004E-Ol
1.28IE-Ol
4.0000
54.424
157.071
78.84
7. 143E -02
1.072E-Ol
1.879E-02
7.1588E-02
9.24!5E-02
ZN XII
8P
EO' 4.8810E+00 (RYD)
N··
5.3788
MU'
.8232
E (RYD)
E (EV)
E PHOT (EV)
L...... DA ( ... )
(L/R/lo-l)
(L/R/L+l)
SI aMI. L-l
SIaM'" L+l
SIGM... (M8)
.0000
.000
87.771
182.115
2.222E-Ol
2.34.E-Ol
7.0111-02
1.1580E-Ol
2.2811-01
2.0000
27.212
84.'83
130.153
1.2841-01
1 . 15UE - 0 1
3.1811-02
8.840E-02
1.2821-01
8.0000
108.847
178.818
70.20
4.434E-02
8.188E-02
7.2741-03
3.582(-02
4.320E-02
ZN XII
8'
EO'
2.1l418E+00 (RYD)
N.· 7.3834
MU'
.11188
E (RYD)
E (EV)
1 PHOT (EV)
L..... D... ( ... )
(L/R/L-l )
(L/R/lo+l)
SIaM'" L- 1
SlGM'" L+l
SIGM... (Mil)
.0000
.000
35.840
344.18
4.210E-Ol
3.5881-01
1.33!5E-Ol
1.818E-Ol
3.2511-01
2.0000
27.212
113. 152
188.33
1.838E-Ol
1.758E-Ol
3.53IE-02
8. 180E -02
1.172E-Ol
8.0000
81.835
117.571
101S.45
5.883E-02
7.7371-02
7.881 E-03
2.848E-02
3.747E-02
311
ZN XII
10P
EO'
1.8345E+00 CRYDI
N-'
Il.3881
MU·
.81311
E (RYDI
E CEV)
E PHOT (EV 1
LAMBDA
CA)
(L/R/L-Il
(L/R/L+11
SIGMA L -1
SIGMA L+l
SIGMA (MBI
.0000
.000
22.2311
5e7.51
8.785E-Ol
4.114I1E-01
2.132E-Ol
2.282E-Ol
4.414E-Ol
2.0000
27.212
411.451
250. 73
1.787E-Ol
1.788E-Ol
3. 233E -02
8.474E-02
Il.707E-02
8.0000
81.835
103.875
1111.38
4.118I1E-02
8.518E-02
5.41 8E -03
1. 848E -02
2.3110E-02
10.0000
138.0511
158.2118
7'.32
2.41I1E-02
3.847E-02
1.1140E-03
8. 822E -03
1.07I1E-02
ZN XII
12P
EO·
1.1105E+00 cnDI
N-' 11.3875
MU'
.8125
E CRYD)
E CEV)
E PHOT (EV)
LAMBDA
CA 1
(L/R/L-l1
CL/R/L+l1
SIGMA L -1
SIGMA L+ 1
SIGMA
(MBI
.0000
.000
15. 1011
820.111
Il.884E-Ol
8.47I1E-Ol
3.07I1E-Ol
2.1157E-Ol
5.738E-Ol
2.0000
27.212
42.321
2112.117
1.745E-Ol
1.1174E-Ol
2.811I1E-02
4 .III1I1E-02
7. lIlISE - 02
4.0000
54.424
1111.533
178.31
7.4113E-02
8.548E-02
8. 177E-03
2.12I1E-02
2.1148E-02
8.0000
108.847
123.158
100.02
2. 77I1E -02
3.881E-02
2. 005E -03
7.742E-03
Il.748E-03
ZN XII
ll1P
EO·
8.0807E-Ol
(RYD)
N-' 15.3888
MU'
.8112
E CRYD)
E CEV)
E PHOT (EV)
LAMBDA
CA)
(L/R/L-l)
(L/R/L+l)
SIGMA L-l
SIGMA L+ 1
SIGMA CMBI
.0000
.000
8.273
14118.82
1.7113E+00
Il.1158E-Ol
5.387E-Ol
3.437E-Ol
8.824E-Ol
2.0000
27.212
35.485
3411.40
1.520E-Ol
1.3115E-Ol
1.718E-02
2.8113E-02
4.80IlE-02
4.0000
54.424
82.8117
1117.75
5.754 E-02
8.381E-02
4. 3411E -03
1.08I1E-02
1.504E-02
Il.0000
81.835
811.11011
137.110
3. OIlIlE -02
3.875E-02
1.80IlE-03
5.85BE-03
7.485E-03
8.0000
108.847
117.121
105.88
1.11115E-02
2.882E-02
Il.4 78E -04
3.531E-03
4.478E-03
ZN XII
20P
EO' 3.8303E-Ol
(RYD)
N·· 111.38114
MU·
.8108
E (RYDI
E CEV)
E PHOT (EV)
LAMBDA
tA)
CL/R/L-I)
(L/R/L+ 1 )
SIGMA L-'
SIGMA L+ 1
SIGMA
CMB)
.0000
.000
5.212
2371.011
2.741E+00
1.3117E+00
8. 20 lE ...0 1
4.280E-Ol
1.248E+00
.5000
8.803
12.014
1031.118
8.788E-Ol
4.4115E-Ol
1.152E-Ol
1.003E-Ol
2.158E-Ol
1.0000
13.8011
18.817
858.811
3.174E-Ol
2.405E-Ol
3.1172E-02
4.55I1E-02
8.530E-02
4.0000
54.424
511 . 1135
207.111
4.4155E-02
4.875E-02
2.47I1E-03
5.1138E-03
8.417E-03
8.0000
81 .835
88.847
142.75
2.338E-02
2.8112E-02
Il.1I2S1E-CM
3.0421-03
4.035E-03
10.0000
138.0511
141.271
87.77
1 . 008E -02
1 . 483E -02
3.00IlE-04
1.287E-03
1.588E-03
ZN XIl
3D
EO' 2.240111+01
(RYDI
N-'
2.53411
MU'
.4851
E (RYD)
E (tV)
E PHOT CEV)
LA• •OA tA)
CL/R/L-l)
(L/R/L+ 1 )
SIGMA L -1
SIGMA L+ 1
SIGMA
CMB)
.0000
'.000
304.8118
40.88
2.1188E-02
1.528E-Ol
8. 844E -03
2.878E-Ol
2.748E-Ol
2.0000
27.212
332.110
37.33
2.578E-02
1.30lE-Ol
5.53I1E-03
2.12lE-Ol
2.178E-Ol
10.0000
138.0511
440.1157
28.12
1 . 558E -02
7.544E-02
2.8112E-03
Il.482E-02
Il.731E-02
ZN XII
4D
EO'
1.1001E+Ol
(nD)
N-'
3.81711
MU'
.3821
E CRYD)
E CEV)
E PHOT CEV)
LAMBDA
(A)
(L/R/L-l )
(L/R/L+l)
SIGMA L- 1
SIGMA L+ 1
SIGMA
(MB)
.0000
.000
1411.88,
82.83
7. 217E -02
2.2117E-Ol
1 . 115111 - 02
2.1178E-Ol
3.174E-Ol
2.0000
27.212
178.8113
70.011
5.378E-02
1.784E-Ol
1.285& -02
2.122E-Ol
2.251E-Ol
4.0000
54.424
204.104
80.75
4.187E-02
1.424E-01
8.1I07E-03
1.580E-Ol
1.84I1E-Ol
8.0000
108.847
258.528
47.18
2.720E-02
Il.852E-02
4.808E-03
Il.081 E-02
Il.581E-02
ZN XII
50
EO' 8.70112E+00 CRYD)
N-'
4.832.
MU·
.3872
E CRYD)
E CEV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l1
CL/R/L+l)
SIGMA L-l
SIGMA L+ 1
SIGMA
CMB)
.0000
.000
III .285
1'35.82
1.30IlE-Ol
3.1471-01
3. 1132E -02
3.40SE-Ol
3.801E-Ol
2.0000
27.212
118.417
1«M .83
8.273E-02
2.178E-Ol
2.038E-02
2.118E-Ol
2.320E-Ol
8.0000
81.835
172.1120
71.70
4.203E-02
1. 2211E-0 1
7.871E-03
Il.848E-02
1.08lE-Ol
12.0000
183.271
254.558
48.71
2. 088E -02
Il.5821-02
2. 738E -03
4.133E-02
4.408E-02
ZN XII
80
EO' 4.52115E+00
CRYD)
tt-· 5.8384
MU·
.3818
E (RYD)
E (EV)
E PHOT CEV'
LAMBDA
CA)
CL/R/L-Il
(L/R/L+ 11
SIGMA L-1
SIGMA L-l
SIGMA
CMB)
.0000
.000
81.828
201. III
2.052E-Ol
4.0571-01
Il.520E-02
3.825E-Ol
4.477E-Ol
2.0000
27.212
88.831
1311.58
1.0821-01
2.454E-Ol
2.812& -02
2.017E-Ol
2.278E-Ol
8.0000
81 .1135
143.283
88.54
4.800E-02
1.211E-Ol
7.820E-03
7.1I1IE-02
8.88lE-02
12.0000
183.271
224.81111
55. 13
2.00IlE-02
5.1I10t-02
2.2821-03
2.18lE-02
3. 11I0E -02
ZN XII
80
EO' 2.4851E+00 CRYD)
N··
7.8430
MU'
.3570
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
CA)
(L/R/L-l)
(L/R/L-l)
SIGMA L-l
SIGMA L+l
SIGMA
(MBI
.0000
.000
33.540
381.87
3.1174E-Ol
8.050E-Ol
1.332E-Ol
4.82I1E-Ol
5.1180E-Ol
2.0000
27.212
80.752
204.01
1 .41 8E -0 1
2.703E-Ol
3.08lE-02
1.874E-Ol
1.1180E-Ol
4.0000
54.424
87.184
140.115
7.347E-02
1.5110E-Ol
1.1113E-02
8.382E-02
Il.578E-02
8.0000
81.1135
115.178
107.85
4.124E-02
1. 084E -0 1
5.1124E-03
4.1118E-02
5.51 1E- 02
ZN XII
100
EO'
1.54801-00 CnD)
N··
Il.8448
MU·
.3552
E (RYD)
E (EV)
E PHOT CEV)
LAMBDA
CAl
CL/R/L-Il
CL/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
21.082
588.87
8.452E-Ol
8.283E-Ol
2.2«ME-Ol
5.422E-Ol
7.828E-Ol
2.0000
27.212
48.274
2511.84
1.537E-Ol
2.874E-Ol
2.888E-02
1.302E-Ol
1.58I1E-Ol
4.0000
54.424
75.488
IlW.2S
8.1172E-02
1.409E-Ol
Il.223E-03
5.854E-02
B.577E-02
8.0000
81. 835
102.8118
120.73
4.009E-02
8.1127E-02
4. 149E-03
3.085E-02
3.500E-02
12.0000
183.271
184.333
87.28
1 . 388E -02
3.IIOE-02
8.885E-04
8.1158E-03
Il.827E-03
ZN XII
120
EO'
1.0818E+00
(RYD)
N·· 11.8487
MU·
.3543
E (RYD)
E (EVl
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
CL/R/L-l)
SIGMA L-l
S.GMA L+ 1
SIGMA
(MBI
.0000
.000
14.448
888.28
8.4&OE-Ol
1 .088E-00
3.250E-Ol
8.223E-Ol
Il.472E-Ol
2.0000
27.212
41 .858
2117.83
1.524E-Ol
2.S081-01
2.432E-02
Il. 883E-02
1.232E-OI
4.0000
54.424
88.870
180.03
8.28IE-02
1.219E-Ol
8.804E-03
3.881E-02
4.541E-02
8.0000
108.847
123.284
100.58
2. 1811E-02
5 . 08 1 E- 02
1.488E-03
1.205E-02
1.353[-02
10.0000
138.0111
150.505
82.38
1.517E-02
3.730E-02
8.708E-04
7.8118E-03
8.787E-03
.. 0
ZN XII
18D
EO· !l.8818E-Ol
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N.· 15.841111
MU'
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E IRTD)
E lEV)
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LAMBDA
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SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
8.003
15"8.2B
1.700E+00
1.1l15E+00
5.81"E-Ol
7.8731-01
1.3B8E+00
.15000
B.803
1... 808
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5.870E-Ol
Il.857E-01
1.3211E-Ol
2.702E-Ol
".028E-Ol
1.0000
13.BOB
21.B08
1173.78
3.118E-Ol
".11BE-Ol
5.278E-02
1.3.0E-Ol
1.808E-Ol
2.0000
27.212
35.2111
3152.08
1.335E-Ol
2.071E-Ol
1.577E-02
5.1183E-02
7.270E-02
".0000
15..... 2 ..
82 ... 27
188.Bl
... 858E-02
8.08lE-02
3.70"E-03
1. 8 .. , E-02
2.311 E-02
B.OOOO
81.1135
88.1l3B
13 •. 32
2.537E-02
5.311E-02
1."51E-03
8.535E-03
1.088E-02
•. 0000
108.8047
1111.850
lOB. 11
1. 5117E -02
3.5"81-02
7.208E-0"
5.5048E-03
B.270E-03
ZN XII
20D
EO· 3.730I5E-Ol
IRYD)
N.· 18.8"70
MU'
.3530
E CRYD)
E lEV)
E PHOT lEV)
LAMBDA
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(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
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5.0'78
2 .... 2.7..
2.8"8E+00
2.2"OE+00
•. 853E-Ol
8.800E-Ol
1.855E+00
.5000
8 .•03
11. 878
10"3.77
8.257E-Ol
8.885E-Ol
1.188E-Ol
2.111 E-Ol
3.280E-Ol
1.0000
13.8011
18.8.2
883.88
2 .• 78E-Ol
3.837E-Ol
3.88"E-02
8.320E-02
1.320E-Ol
2.0000
27.212
32.2.8
3 .... 01
1.113E-Ol
1.877E-Ol
i . 005E -02
·3."23E-02
..... 28E-02
".0000
15..... 2..
58."88
208.38
3.78I1E-02
8.8"'E-02
2.1"3E-03
1.08lE-02
1.285E-02
8.0000
81.1135
BB.711
1"2.88
1.8215E-02
3.871 E-02
8.078E-0"
5.155E-03
5.883E-03
10.0000
138.0118
, .. 1 . 135
87 .•15
7.800E-03
1.880E-02
2.21"E-0"
1.88IE-03
2.1021-03
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N.·
3.8838
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SIGMA L-l
SICMA L+l
SIGMA 1MB)
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.000
128.223
811.85
".123E-02
2.1BOE-Ol
5.815E-03
2.205E-Ol
2.28"E-Ol
2.0000
27.212
158."35
78.28
2.77041 -02
1."38E-Ol
3.2"11-03
1.1118E-Ol
1. 181 E-Ol
".0000
5 ..... 2 ..
1.3.8.. 7
87.!l1
1.8701-02
1.00IlE-Ol
1.8201-03
8.87"E-02
8.81lIlE-02
8.0000
108 ....·7
238.071
sa. O.
1. 112E -02
Il. 582E -02
7.827E-0"
2.873E-02
2.7!l3E-02
.....
ZN XII
III'
,
EO. 8.0"32E+00 (RYD)
N··
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MU'
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E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
lA)
(L/R/L-l)
(L/R/L+1)
SIGMA L - 1
SIGMA L+l
SIGMA (MB)
.0000
.000
82.223
150.78
8.1!lOE-02
3.88!lE-Ol
1.8!l"I-02
3.88BE-Ol
".152E-Ol
2.0000
27.212
108."311
113.30
!l.188E-02
2.120E-Ol
7.83"E-03
1.7815E-Ol
1. 8 .. !lE-0 1
".0000
1104."2"
13'1. 8"7
80.7"
3.28BE-02
1, 3112E-Ol
3.878E-03
8.103E-02
8.500E-02
8.0000
108.8047
181.070
84.88
1.807E-02
8.802E-02
1.328E-03
3. 17 .. E-02
3.307E-02
10.0000
138.01111
218.2.2
511. .80
1.187E-02
5.11.E-02
8 ... 25E -0"
2.0!l3E-02
2. 137E-02
ZN XII
Ill'
EO· ".1705E+00
(RYD)
N··
15..781
MU'
,1238
E IIVD)
E (EV)
E PHOT ( EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
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.000
58.7....
21 •. 50
1.!l88E-Ol
5. 178E -0 1
3. 757E -02
5."1I0E-Ol
5.83!lE-Ol
2.0000
27.212
.3.11511
, .. 7.88
7.38"E-02
2.5.2E-Ol
t . 221lE -02
2.008E-Ol
2.1321-01
".0000
5" ... 2..
1 11 . 1117
111.53
".183E-02
1.52111-01
5 .. 2113E-03
8.288E-02
8.822E-02
•. 0000
10 ..... 7
1115.581
7".88
1.818E-02
Il.8!l7E-02
1."7!lE-03
2.878E-02
3.025E-02
10.0000
138.0511
.182 .•03
8".31
1.307E-02
5.082E-02
8.884E-0"
1 . 78!lE -02
1.8UE-02
ZN XII
.1'
EO. 2.32"OE+00 (RYD)
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7.8715
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. 1285
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
tA)
IL/R/L-I)
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SIGIIIA L·l
SIGMA L+ 1
SIGMA (MB)
.0000
.000
31.821
382.10
3.31lE-Ol
8.0428E-Ol
8. 33.. E -02
8.01l5E-Ol
8.nBE-Ol
2.0000
27.212
58 .•33
210.7..
1. 03.E-0 1
3.032E-Ol
1.708E-02
1."'3E-Ol
2.113E-Ol
".0000
5" ."2"
88.0....
1..... 10
".830& -02
1.1152E -0 1
1l.1I32E -03
7 ..... OE-02
•. 003E-02
8.0000
108 .... 7
, .. 0 .....
.8.27
1.8021 -02
8.1.8E-02
1.228E-03
1.8301 -02
2. 053E -02
10.0000
138.0118
187.11'0
73.8"
1.23"1-02
".31l.. E-02
8.877E-0"
1.1 .. 7E-02
1 .21111 -02
12.0000
183.271
18 ....82
113.82
•.•8IlE-03
3.223E-02
... , .. 5E -0"
7.288E-03
7.883E-03
ZN XII
lOI'
EO·
1. "783E+00
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N••
8 .• 11117
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.1303
E (RYD)
E (EV)
E PHOT (IV)
LAIIIBDA
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(L/R/L-l)
(L/R/L+I)
SIGIIIA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
20.113
1118 .....
5.81041-01
1.20"E+00
1.707E-OI
1.0"7E+00
1.218E+00
2.0000
27.212
"7.325
281.88
1.IIlIIE-Ol
3.0.'E-0'
1. 73 lE -02
1.813E-Ol
1.78IlE-Ol
".0000
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7".537
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".705E-03
5.3"7E-02
5.81BE-02
•. 0000
108 .... 7
128.8111
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5.1118E-02
8.757E-0"
1.2371-02
1 . 3215E-02
10.0000
138.0118
158. 172
78.38
1.05.E-02
3.1170E-02
".7071-0"
7.1"7E-03
7.1l1.E-03
ZN XII
12F
EO·
1.0222E+00 (RYD)
N.. 11 .•11.7
MU'
.1313
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lA)
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.0000
.000
13.808
.81 .....
8."58E-Ol
1.&03E+00
2.880E-OI
1.2.3E+00
1.151E+00
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8 .•03
20.712
588.113
... 180E -0 1
8.731E-Ol
8.853E-02
5.870E-Ol
Il.1135E-Ol
1.0000
13.8011
27.51"
"110.112
2 ....·41-01
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".571E-02
3.088E-Ol
3.555E-Ol
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3.780E-02
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8.0000
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101 .00
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8.118E-03
•. 72IlE-03
ZN XII
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(RYD)
N·· 15.81178
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SIGMA L-l
SIGMA L+l
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.0000
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7.7.1
1583.38
1.570E+00
2.!l11E+00
5.188E-OI
1.781E+00
2.27.E+00
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•.• 03
'''.5.''
850.13
5. 188E-0 1
8.7181-01
1.0821-01
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8.005E-Ol
1.0000
13.808
21. 387
178.72
2.1l1lE-Ol
1.37"1-01
3.828E-02
2.218E-Ol
2.811E-Ol
2.0000
27.212
3".883
311".32
1.055E-Ol
2."551-01
1.0"BE-02
7.5721-02
8.821E-02
".0000
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82.205
188.32
3. 51BE -02
8.388E-02
2.073E-03
1.8'72E-02
2.1781-02
B.OOOO
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.8 ... 17
138.88
1.712E-02
".81181-02
7.058E-0"
7 .88BE-03
8.802E-03
10.0000
138.058
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8.38IE-03
2.047E-02
1.582E-0"
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2.322E-03
ZN XII
20F
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(RYD)
N" 18.8B7"
MU'
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E (RYD)
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2"87.85
2 ... 8 .. E+00
3.582E+00
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2.2821+00
3.083E+00
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8 .•03
11.7117
10113.71
5.520E-Ol
8. B881-01
8.81151-02
3.UOE-Ol
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1.0000
13.808
18.570
887.B8
2.438E-Ol
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2.875E-02
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1.82"E-OI
2.0000
27.212
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2.003E-Ol
8. 8BlE -03
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5.32"E-02
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58.387
208. '78
2.772E-02
7.2 .... E-02
1.2281 -03
1.1181-02
1.2"21-02
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1.31"E-02
3.'7"'E-02
".027E-0"
".353E-03
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10.0000
1311.058
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87.82
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1.518E-02
8.1l8IE-05
1.184E-03
1.2!llE-03
KA
XVIII
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2.8028E+Ol
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.0000
.000
381.318
32.152
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15.187E-02
.000
8.473E-02
B.473E-02
2.0000
27.212
408.1530
30.315
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4.728E-02
.000
15. 7315E-02
15. 7315E-02
14.0000
180.483
1571.801
21. 88
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2.8154E-02
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3. 1315E-02
3. 135E-02
KA
XVIII
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1.8848E+Ol
IAYD)
N·· 4.4118
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E IAYD)
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LAMBDA
(A)
(L/A/L-O
IL/A/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
228.484
154.74
.000
7.877E-02
.000
8.831E-02
8.831E-02
2.0000
27.212
2153.8811
48.87
.000
B.707E-02
.000
7.171E-02
7.17IE-02
14.0000
180.483
418.8ee
28.74
.000
3.283E-02
.000
2.823E-02
2.823E-02
KA
XVIII
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1.1043E+Ol
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E (AYD)
E (EV)
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1MB)
.0000
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1150.250
82.152
.000
1.104E-Ol
.000
1.1151E-Ol
1.1151E-Ol
2.0000
27.212
177.481
H.87
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8.881E-02
.000
8.403E-02
8.403E-02
10.0000
138.058
288.308
43.31
.000
4.313E-02
.000
3.347E-02
3.347E-02
KA
XVIII
8S
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(AYDI
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E (RYD)
E (EV)
E PHOT (EV)
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SIGMA L-l
SIGMA L+l
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(MB)
.0000
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80.0154
1154.88
.000
1.871E-Ol
.000
1.781 E-Ol
1.781E-Ol
2.0000
27.212
.107.288
1115.158
.000
1.213E-Ol
.000
t1.820E-02
8.820E-02
8.0000
81.8315
181.880
78.88
.000
8.1571E-02
.000
4.387E-02
4.387E-02
KA
XVIII
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3.8484E+00 IAYD)
N·· 8.4224
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E (RYD)
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48.8154
248.70
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2.807E-Ol
.000
2.4158E-Ol
2.458E-Ol
2.0000
27.212
7B.888
181.30
.000
1.454E-01
.000
1.0221-01
1.0221-01
4.0000
154.424
104.078
118.13
.000
8.180E-02
.000
15.1523E-02
15.523E-02
KA
XVIII
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SIGMA L+'
SIGMA
(MB)
.0000
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33.783
387.01
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3.804E-Ol
.000
3.23!5E-Ol
3.2315E-Ol
2.0000
27.212
80.8815
203.27
.000
1.1588E-Ol
.000
8.870E-02
8.870E-02
•. 0000
154.424
88.207
140.158
.000
9.031E-02
.000
4.152IE-02
4.52 le -02
12.0000
183.271
187.0154
82.82
.000
2.838E-02
.000
8.801E-03
8.801E-03
KA
XVIII
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1.3818E+00 CAYO)
N·· 115.4240
MU'
.15780
E (AYD)
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SIGMA L+l
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.0000
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18.1530
888.11
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8.1558E-Ol
.000
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15.0071-01
2.0000
27.212
415.742
271.08
.000
1.823E-Ol
.000
7.1573E-02
7.1573E-02
8.0000
81.831i
100.188
123.78
.000
4.820E-02
.000
1.482E-02
1.482E-02
8.0000
108.847
127.377
87.34
.000
3.324E-02
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8.8415E-03
14.0000 . 180.483
2011. 013
158.32
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1.1548E-02
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3.1153E-03
3.1153E-03
KA
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205
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(AYD)
N·· 18.4244
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E (RYD)
E (EV)
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(L/A/L-l)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA
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t 1. 884
1081.20
.000
8.788E-Ol
.000
7.0150E-Ol
7.050E-Ol
2.0000
27.212
38.8815
318.77
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1.150lE-Ol
.000
15.1505E-02
15.1505E-02
8.0000
81.UI5
83.318
132.88
.000
3.837E-02
.000
8.832E-03
8.832E-03
10.0000
138.088
147.743
83.82
.000
1.8aU-02
.000
3.288E-03
3.288E-03
KA
XVIII
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2.8355E+Ol
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SIGMA L+l
SIQMA
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.0000
.000
3158.1580
34.158
3.8815E-02
7.17lE-02
1.1221-02
7.72!IE-02
8. 848E -02
2.0000
27.212
385.782
32.14
3.428E-02
8.151lE-02
8.487E-03
8.B152E-02
7.801E-02
14.0000
180.483
1548.083
22.58
1.807E-02
4.014E-02
4.184E-03
3.708E-02
4.124E-02
KR XVIII
15P
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1.15848E+Ol
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N·· 4.15213
MU'
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(MB)
.0000
.000
2115.B44
157.50
8.887E-02
1.012E-Ol
1. "88E -02
8.2158E-02
1.122E-Ol
2.0000
27.212
242.858
151. 015
15.414E-02
8.8501-02
1.4" 1 E-02
7.813E-02
8.104E-02
8.0000
81.8315
287.278
41. 71
3.880E-02
8.1583E-02
8.278E-03
15.387E-02
8.32!5E-02
KA XVIII
8P
EO'
1.0804E+Ol
IRYDI
N·· 15.15277
MU'
.4723
E (RYD)
E (EV)
E PHOT 1 EV)
LAMBDA
(A)
IL/A/L-l )
CL/A/L+l )
SIGMA L-l
SIGMA L+l
SIGMA
1MB)
.0000
.000
144.274
815.84
1.001E-Ol
1.3.4E-Ol
3.027E-02
1.0"21-01
1.3"15E-Ol
2.0000
27.212
171.488
72.30
7.4"8E-02
1.087E-01
2.020E-02
8.18IE-02
1.020E-Ol
8.0000
108.847
2153.121
48.118
3.8"2E-02
8.21515E-02
8.030E-03
4.1."E-02
4.852E-02
KR XVIII
8P
EO. 15.70"15E+00 (RYD)
N·· 7.15331
MU'
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E (RYO)
E (EV)
E PHOT lEV)
LAMBDA
CA)
CLIR/L-l 1
IL/R/L-l)
SIGMA L-l
SlaMA L+l
SIGMA
(MB)
.0000
.000
77.883
1158.BO
1.878E-Ol
2.107E-Ol
15.730E-02
1.4415E-Ol
2.018E-Ol
2.0000
27.212
104.8"15
118.20
1.1315E-Ol
1.3""E-Ol
2.830E-02
8.1188E-02
1.143E-Ol
8.0000
108.847
188.1531
88.47
4.280E-02
8.2152E-02
7.11511E-03
3.054E-02
3.770E-02
42
KR XV 111
10P
EO' 3.5835E+00 (RYDI
N••
Il.!l3!l3
MU'
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1
(RYO)
1
<EV)
E PHOT (Ev,
LAM80A (A)
(L/AIL-l)
(L/A/L+I)
SIGMA
L - 1
SIGMA
L+l
SIOMA
(M8)
.0000
.000
48.484
255.72
2. VVllE-Ol
2.VV4E-Ol
V.135E-02
1.82H-Ol
2.734E-Ol
2.0000
27.212
7!l.8VII
183.7V
1.421E-Ol
1.1112E-Ol
3.202E-02
8.238E-02
1.144E-Ol
8.0000
81. 8S5
130. t 20
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!l.1I74E-02
7.488E-02
8.774E-03
3. 0!l7E -02
3.V34E-02
10.0000
138.0eV
184.!l43
87. IV
3. 121 E-02
4.!l37E-02
3.711!lE-03
1.5V2E-02
I.V88E-02
14.0000
IVO.483
238.V1I7
51.88
2.00lE-02
3.122E-02
2. 003E -03
S.7!l8E-03
1. 178E-02
KR xv 111
12P
EO'
2.4344E+00
(RYO)
N••
1'.!l311!l
MU'
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E (IIYO)
E lEV)
E PHOT (EV)
LAMeDA (A)
(L/A/L-l)
IL/A/L+I)
SiaMA
L - 1
SIGMA
L+l
SIOMA
(Mil)
.0000
.000
33.123
374.32
4.3!lVE-Ol
3.VV8E-Ol
1.318E-Ol
2.218E-Ol
3.538E-Ol
2.0000
27.212
110.335
20B.!l0
1. !lV4E-01
1.71!lE-OI
3.211E-02
7.438E-02
1.08U-OI
Il.0000
81.83!l
114.7!l8
108.04
!l.3!lIE-02
Il.837E-02
Il.882E-03
2.247E-02
2.V3SE-02
12.0000
183.271
IVII.3V4
83.13
2. U8E -02
3.143E-02
1.8113E-03
8.1211-03
V.VV1E-03
KA XVIl 1
ll1P
EO'
1.342lE+00 (AYO)
N••
1!l.!l3711
MU'
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E (EV)
E PHOT (EV)
LAM80A lA)
(L/A/L- t 1
(L/R/L+I)
SIGMA
L - 1
SIGMA L+l
SIGMA
(Mil )
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.000
18.280
87V.00
7.711!lE-Ol
Il.340E-Ol
2.308E-Ol
3.075E-Ol
!l.381E-Ol
2.0000
27.212
4!l.472
272.88
1.1178E-01
1.702E-Ol
2.1181 E -02
s , !l17E-02
8. tVII-02
4.0000
!l4.424
72.8U
170. !l8
7. !l88E -02
8.1121E-02
8.720E-03
2.2113E-02
3.135E-02
8.0000
108.847
127.108
87.84
2.VOVE-02
3.82I1E-02
2.284E-03
7.7V4E-03
1.00!lE-02
12,.0000
1113.211
181.!l31
118.30
1. !l74E -02
2.274E-02
V.42I1E-04
3.11341-03
4.878E-03
KA XVIl 1
20P
EO' 8.4875E-Ol
(AYDI
N•• 19.8381
MU'
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E (RYD)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+l)
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L - 1
SiaMA
L+l
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(M8)
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.000
11.!l48
1013.1I!l
1 .20!lE+00
S.105E-Ol
3.512E-Ol
".011E-Ol
7.!l23E-Ol
2.0000
27.212
38.780
31S.81
1. !l7!lE-0 1
1.!l!lOE-01
2.014E-02
3.8VVE-02
!l.VI3E-02
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Il!!. vn
t87.14
8.37VE-02
7.1 tBE-02
5.824E-03
1.400E-02
1.V83E-02
Il.0000
1'.113!l
V3. ' ' ' '
133.011
3. !l3!lE-02
4. 297E -02
2.43IE-03
7.208E-03
Il.848E-03
10.0000
138.0SV
147.1107
84.00
1.1I03E-02
2. lV3E-02
7.V48E-04
2.113E-03
3.711IE-03
KA XVIl 1
3D
EO' ".1I474E+Ol
(AYDI
N••
2.11404
MU'
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E <EV)
E PHOT (EV)
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(L/R/L-l )
(L/R/L+1)
SIGMA
L - 1
SIGMA
L+l
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(Ma)
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832.32!l
lV.1I1
1.270E-02
Il. !l!l2E-02
2. !lUE -03
1·.023E-Ol
1.049E-Ol
2.0000
27.212
Il!lV.!l37
18.80
1.17H-02
Il.03IE-02
2.2UE-03
V.045E-02
Il.27!lE-02
18.0000
244.VOII
877.231
14.13
Il.1177E-03
3,400E-02
1.073E-03
3.825E-02
3.832E-02
20.0000
272.118
904.443
13,71
e. !l88E -03
3,1V4E-02
Il. 888E-04
3.479E-02
3.!l7IE-02
KA XV111
40
EO'
2.311!l2E+Ol
(RYDI
N••
3.7012
MU'
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E (AYD)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/A/L-l)
(L/R/L+I)
SIGMA
L-l
SIGMA
L + 1
SIOMA
(M8)
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.000
321.801
38.53
3.107E-02
1.058E-Ol
7. 80llt -03
1.3!lVE-Ol
1.437E-Ol
2.0000
27.212
34V.013
35.82
2. 118liE -02
V.278E-02
8.32I1E-03
1.133E-Ol
1.188E-Ol
4.0000
84.424
378.225
32.V8
2.34!lE-02
8.1VVE-02
s , 202E -03
V.!l38e-02
1.00BE-Ol
14.0000
lVO.483
5t2.284
24.20
1.331 E-02
4.83I1E-02
2. 280E -03
4.517E-02
4.74!lE-02
KA XVIl 1
80
EO'
1.4882E+Ol
(RYOI
N••
4.7137
MU'
.2883
E (AYD)
E (EV)
E PHOT ( EV)
LAM8DA
(A)
(L/A/L- 1 )
(L/A/L+ 1 )
SIGMA
L-l
SIGMA
L+l
SIGMA
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.000
1118.402
112.4V
5.811VE-02
1.4V5E-Ol
1 . SV7E -02
1.1172E-Ol
1.832E-Ol
2.0000
27.212
22!!. e 14
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4.502E-02
1.232E-Ol
, . 14'" -02
1.2VOE-Ol
1.40!lE-Ol
4.0000
!l4.424
252.8211
4V.04
3.1170E-02
1.033E-Ol
8.S5BE-03
1,018E-Ol
1.103E-Ol
8.0000
81 .83!l
280.038
44.21
3.0!lOE-02
8.80U-02
Il. 5411E-03
8.178&-02
8.833E-02
18.0000
244.V08
443.30V
27.V7
1.30IlE-02
4. 133E-02
I.V01E-03
2. 8811E -02
3.048&-02
KA XVIII
80
EO' Il.V080E''00 (RYD)
N·· !l.718!l
MU'
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E (RYO)
E (EV)
E PHOT (EVI
LAM8DA
(A)
(L/R/L-T)
(L/A/L+l )
SIGMA
L-l
SlaMA
L + 1
SIGMA
(M8)
.0000
.000
134.808
Vl.V7
8. VOU-02
1.1171E-OI
2.888E-02
1.874E-Ol
2.243E-Ol
2.0000
27.212
1112.020
78.!l1
8.4341-02
1.!lOBE-Ol
1. 8811E -02
1.3aU-Ol
1 .ISU -0 1
8.0000
81.83!l
2111.444
!l7.21
3. 830E-02
8.722E-02
7. V7IE-03
7.714E-02
8.!l12E-02
14.0000
lVO.483
32!l.2111
18.12
1.81I1E-02
!l.092E-02
2.8vaE-03
3. 180E-02
3.4!lOE-02
KA XVIII
80
EO' 8.4331E+00 (AYD)
N••
7.7223
MU'
.2777
E (RYD)
E (EV)
E PHOT (EV)
LAM8DA (Al
(L/R/L-l)
(L/A/L+ T)
SIGMA
L - 1
SIOMA
L+ 1
SIOMA
(M8)
.0000
.000
73.823
187.72
1.73SE-Ol
3.034E-Ol
!l.1S83E-02
2.58aE-Ol
3.12!lE-Ol
2.0000
27.212
101.134
122.80
r . 004E-0 1
1.1137E-Ol
2. !l8lE-02
1.430E-Ol
1.118I1E-Ol
4.0000
54.424
128.348
811.00
Il.!l8SE-02
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1.3.IE-02
Il.0I2E-02
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Il.0000
81 .1I3!l
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4.8a.I-02
1. 023E-Ol
8. !l23E -03
8.13BE-02
8 .•88E-02
12.0000
183.271
237.184
12.21
2. 188E-02
!l.32!lE-02
2.8021-03
2.!l38E-02
2.8UIE-02
KA XVIII
100
EO' 3.428I1E+00 (AYDI
N·· 8.7238
MU'
.27111
E (AYD)
E (EV)
E PHOT (EV)
LAMflOA
(AI
(L/II/L-l)
(L/A/L+I)
SIOMA L-l
SIGMA
L-l
SlaMA
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48.1122
28!l.84
2.830&-01
4.24tf,-01
V.381E-02
3.1821-01
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2.0000
27.212
73.83_
187 .•3
1.27SE-Ol
2.1 •• E-Ol
3.017E-02
, .344E-01
1.848E-Ol
4.0000
14.424
101.048
122.10
7.337E-02
1.381l-01
1.387E-02
7.33l1E-02
8.702E-02
Il.0000
81.835
128.258
811.87
4.7.15E-02
V,718E-02
7.41I1E-03
4.587E-02
!l.308E-02
12.0000
1113.271
208 .••3
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4.55I1E-02
2.031 E-03
1 .1I43E -02
1.84I1E-02
111.0000
217.'.5
284.317
411.81
1.281E-02
3.1118E-02
1.090E-03
Il.1I38E-03
1.103E-02
18.0000
244.8011
2111.Il2V
42.!l3
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2.15851-02
•. 338E-0_
7.885E-03
8.81VE-03
KA KV 11 1
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11.7247
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SIGMA
L - 1
SIGMA
L+l
SIGMA
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.000
32.088
388.84
4.157E-Ol
1I.!l87E-0\\
1.400E-Ol
3.77!lE-Ol
5.174E-Ol
2.0000
27.212
!l1l.280
208. III
1.442E-Ol
2.313E-Ol
3.0117E-02
1.18!lE-Ol
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815.4112
143.3!l
7.4221-02
1.328E-Ol
1.18IE-02
5. 7S3E -02
Il.1151E-02
15.0000
81.1535
113.703
108.04
4.51121-02
8.828E-02
!l.947E-03
3.3411-02
3 . •38E-02
14.0000
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222.551
!l!l. 71
1.34!lE-02
3.133E-02
1.0121-03
8.238E-03
8.24VE-03
111.0000
2 t7. '.!l
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2.807E-02
7.40n-04
8.3.U-03
7.13.E-03
43
KR XVIII
180
EO·
1.3102E+00 (RYO)
N··
15.7254
MU·
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E (RYO)
E (EV)
E PHOT (EV)
LAMBOA (A)
(L/R/L-l)
(L/R/L+1)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
17.827
III1IS. 52
7.534E-Ol
8.1178E-Ol
2.543E-Ol
5.0112E-Ol
7.80IlE-Ol
2.0000
27.212
411.038
275.211
1.531 E-O 1
2.2112E-Ol
2.1153E-02
8.1187E-02
1.134E-OI
4.0000
54.424
72.250
171.111
Il.1I84E-02
1. 1211E -0 1
8.114E-03
3.457E-02
4.288E-02
8.0000
108.847
1211.1174
117.88
2.4113E-02
4.840E-02
1.1117E-03
1.III1E-02
1.311 E-02
10.0000
1311.0511
153.8811
80.57
1.724E-02
3.5110E-02
1. 150E-03
7.47I1E-03
8.1128E-03
12.0000
1113.271
181.0118
118.411
1.280E-02
2.788E-02
7.4112E-04
5.30IlE-03
Il.052E-03
20.0000
272.118
2811.1145
42.711
5.342E-03
1 . 3111E-02
2.080E-04
1.8113E-03
2. 101 E-03
KR XVIII
200
EO· 8.32118E-Ol
(RYO)
N··
111.7258
MU·
.2742
E (RYO)
E (EV)
E PHOT leV)
LAMBOA
(A)
(L/R/L-l)
(L/R/L+l )
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
11.3211
10114.38
1. 1711E+00
1.228E+00
3.115I1E-Ol
Il.431lE-Ol
1.040E+00
1.0000
13.11011
24.11311
4117.23
3. 01l7E-0 1
3.877E-Ol
5.8118E-02
1.413E-Ol
2.003E-Ol
2.0000
27.212
38.541
321.70
1.444E-Ol
2.044E-Ol
2.02IE-02
Il.073E-02
8.0115E-02
4.0000
54.424
115.753
188.511
5.11117E-02
Il.270E-02
5.308E-03
2. 130E~02
2.1I111E-02
8.0000
108.847
120.177
103.17
1.1133E-02
3.738E-02
1.128E-03
Il.332E-03
7.4111E-03
10.0000
1311.0511
147.388
84.12
1.335E-02
2.733E-02
Il.1I01lE - 04
4. 151 E- 03
4.811 E-03
18.0000
244.11011
2511.2311
48.311
4.81I1E-03
1.143E-02
1.4114E-04
1.2113E-03
1.412E-03
KR XVIII
4F
EO· 2.1332E+Ol
(RYO)
N··
3.81173
MU·
.1027
E (RYO)
E (EV)
E PHOT (EV)
LAMBOA (A)
(L/R/L-l)
(L/R/L+l )
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
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2110.235
42.72
1.114I1E-02
Il.417E-02
2. 125E -03
Il. 242E-02
Il.455E-02
2.0000
27.212
317.447
311.011
1.3117E-02
7.720E-02
1.5117E-03
Il.7114E-02
Il.1154E-02
Il.0000
81.1135
371. 870
33.34
Il. 748E-03
5.411 E-02
Il.5IBE-04
3.1I10E-02
4.005E-02
14.0000
1110.483
480.718
25.711
5.531E-03
3. 002E -02
3.1I110E-04
1. 5511E -02
1.5115E-02
20.0000
272.118
5112.353
22.05
3.811I1E-03
2.078E-02
2.2117E-04
8.723E-03
8.1150E-03
KR XVIII
5F
EO·
1.3543E+Ol
(RYO)
N.·
4.81112
MU·
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E (RYO)
E (EV)
E PHOT (EV)
LAMBOA
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(L/R/L-l)
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SIGMA L- 1
SIGMA L+ 1
SIGMA (MB)
.0000
.000
184.21111
117.211
3.11112E-02
1.5115E-Ol
Il.711I1E-03
1.1183E-Ol
1.7111E-Ol
2.0000
27.212
211.477
58.113
2.804E-02
1.2231-01
4.480E-03
1.13111-01
1. 181 E-Ol
4.0000
54.424
238.11811
51.114
2.11131-02
Il.1138E-02
3.0111 E-03
7.1I111E-02
8.270E-02
12.0000
1113.271
347.5311
35:118
Il.1141E-03
4.411I1E-02
Il. 2411E-04
2.4110E-02
2.582E-02
20.0000
272.118
4511·.384
27.17
5.451 E'-03
2.488E-02
3.11112E-04
1.015E-02
1.051E-02
KR XVIII
IIF
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Il.3448E+00 (RYO)
N·.
5.8883
MU·
. 1117
E (RYO)
E (EV)
E PHOT
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LAMIIOA (A)
(L/R/L-l)
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
127.145
117.52
Il.383E-02
2.270E-Ol
1.3115E-02
2.352E-Ol
2.4112E-OI
2.0000
27.212
154.357
80.32
4.384E-02
1.1I08E-Ol
7.1I110E-03
1.433E-Ol
1.513E-Ol
4.0000
54.424
181.51111
118.211
3.180E-02
1.1I14E-Ol
4.1145E-03
Il.300E-02
Il.7115E-02
10.0000
1311.0511
2113.204
47.11
1 . 4811E- 02
5.874E-02
1 .571 E-03
3.2111E-02
3.418E-02
14.0000
1110.483
317.112lr
311.04
Il.11115E-03
4.035E-02
8.54I1E-04
1.857E-02
1 .ll431 -02
20.0000
272.118
31111.2113
31.05
Il.071E-03
2.518E-02
3 .1lI3E -04
Il.08I1E-03
Il. 485E-03
KR
XVIII
8F
EO· 5.2103E+00 (RYO)
N••
7.8857
MU·
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E (RYO)
E (EV)
E PHOT (EV)
LAMIIDA (A)
(L/R/L-l )
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
70.8110
174.110
1. 31111E -01
3.737E-Ol
3.5111E-02
3.1154E-Ol
3.1I10E-Ol
2.0000
27.212
118.102
1211.38
7.440E-02
2. 1113E -0 1
1.4112E-02
1.11114E -0 1
1.840E-Ol
4.0000
54.424
125.314
118.114
4.1152E-02
1.445E-Ol
7.302E-03
Il.400E-02
1.013E-Ol
8.0000
108.847
1711.738
118.118
2.280E-02
7.1113E-02
2.51I1E-03
3.741E-02
3.11112E-02
14.0000
1110.483
2111. 373
47.44
1.055E-02
3.77IE-02
7.828E-04
1.334E-02
1.413E-02
18.0000' 244.11011
315.7117
311.211
7.04I1E-03
2.1I04E-02
4.22I1E-04
7.1187E-03
8.110E-03
KR
XVIII
lOF
EO· 3.31110E+00 (RYO)
N··
Il.8847
MU·
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E (RYO)
E (EV)
E PHOT
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LAMBOA (A)
(L/R/L-Il
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
45.118
274.81
2.338E-Ol
5.378E-Ol
Il.1I43E-02
4.1187E-Ol
5.351E-Ol
2.0000
27.212
72.3211
171. 42
Il. 83I1E-02
2.54I1E-Ol
1.885E-02
1 .1I83E -0 1
1.872E-Ol
4.0000
54.424
1111.541
124.511
5.380E-02
1.503E-Ol
7.711I1E-03
8.074E-02
8.850E-02
8.0000
108.847
153.11115
80.53
2.211I1E-02
7.07I1E-02
2. 1811E-03
2.7118E-02
2.1187E-02
12.0000
1113.271
208.3811
511.50
1.244E-02
4.085E-02
8.1I110E-04
1.241lE-02
1.33I1E-02
14.0000
1110.483
235.1100
52.113
Il.1151E-03
3.247E-02
5.1I10E-04
8.112IE-03
Il.1112E-03
20.0000
272.118
317.2311
311.08
5. 134E-03
1 . 8211E-02
2.252E-04
3.810E-03
4.035E-03
KR XVIII
12F
EO.
2.2ll41E+00 (RYO)
N··
Il.8842
MU·
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E (RYO)
E (EV)
E PHOT
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LAMBDA (A)
(L/R/L-l)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
31.213
3117.23
3.548E-Ol
7.1118E-Ol
1.058E-Ol
5.808E-Ol
Il.811I1E-Ol
2.0000
27.212
58.425
212.22
1.138E-Ol
2.70IlE-Ol
2.038E-02
1.53I1E-Ol
1.743E-Ol
4.0000
54.42.
85.1137
144.78
5.5110E-02.
1.45I1E-Ol
7.130E-03
Il.511 E-02
7.224E-02
8.0000
108.847
140.0110
88.52
2.143E-02
Il.300E-02
1.732E-03
1.III1I1E-02
2.111I1E-02
12.0000
1113.271
1114.484
113.75
1.107E-02
3.500E-02
Il.417E-04
8.553E-03
Il.1115E-03
18.0000
2.4.11011
2711.1111
4•. 110
5.331E-03
1.812E-02
2.1131-04
3.257E-03
3.4118E-03
KR XVIII
ll1F
EO·
1.28.2E+00 (RYO)
N•• 15.8837
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E (RYO)
E (EV)
E PHOT (EV)
LAMBOA (A)
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SIGMA L- 1
SIGMA L+l
SIGMA (MB)
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17.473
7011.58
Il.III1.E-Ol
1. 1311E+00
2. 083E-O 1
8.101E-Ol
1.018E+00
2.0000
27.212
44.1185
277.47
1.2.0E-Ol
2.1175E-Ol
1.850E-02
1.148E-Oi
1.333E-Ol
4.0000
54.424
71.8117
172.45
5. 1211E-02
1.248E-Ol
5.088E-03
4.022E-02
4.530E-02
10.0000
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153.532
80.711
1.17I1E-02
3.44I1E-02
5.71I1E-04
Il.5.IIE-03
7.118E-03
20.0000
272.118
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3.1117E-03
1.01lIlE-02
7.821E-05
1.182E-03
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•
Kil XVIII
20F
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(IlYD)
N·· la.8834
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1L/R/L- 1)
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SIGMA L - 1
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11.150
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1.00.E+00
1 .nOE +00
3.401E-Ol
1.051E+00
1.3alE+00
1.0000
'3.000
2•. 7S0
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2.IS1.E-Ol
•. 7aVE-Ol
4.550E-02
2.047E-Ol
2.503E-Ol
2.0000
27.212
38.31S2
323.20
1. 180E-0 1
2.42VE-Ol
1. 453E -02
8.125E-02
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4.0000
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05.574
1811. 08
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1.033E-Ol
3.418E-03
2.513E-02
2.8S4E-02
8.0000
108.847
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1.380E-02
3.770E-02
IS.157E-04
O. 120E -03
IS.741E-03
10.0000
217.0V5
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5•. 18
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8.1547E-05
1.11S0E-03
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MO XXIV
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3.237E-02
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1.0000
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12.0000
183.271
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312.851
32.3V
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5.333E-02
5.333E-02
8.0000
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MO XXIV
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MO XXIV
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72.516
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27.212
111.122
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511.11811
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118.030
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6.1V2E-03
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5.1125E-02
1.0000
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5.883E-03
4.812E-02
5.400E-02
12.0000
1113.271
7117.570
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1.~88E-02
3.172E-02
3.55I1E-03
3.23111-02
3.5112E-02
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1.078E-02
6.172E-02
7.250E-02
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381.780
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3.520E-02
6.01I1E-02
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5.78I1E-02
Il. 780E-02
8.0000
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5.178E-03
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MO XXIV
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5.11180
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1.6153E-02
7.~27E-02
8.080E-02
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7.8~7E-02
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8.020E-02
8.353E-03
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11IO XXIV
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1.323E-01
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3.783E-02
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MO XXIV
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MO XXIV
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213.811
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7. 1113E -02
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13.1108
71.583
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1.8118E-Ol
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1.518E-Ol
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MO XXIV
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2.288E-Ol
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27.212
511.302
2011.08
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Il.887E-02
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118.030
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7 .1I54E -02
8.473E-03
2.457E-02
3.305E-02
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111.112711
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4.1145E-Ol
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33.11"8
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2,775E-Ol
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1 . 111111 E- 0 1
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2.584E-02
5.5110E-02
8.173E-02
4.0000
15".424
74. 71111
11115.83
7.488E-02
8.507E-02
8.781E-03
2.2117E-02
3.145E-02
7.0000
115.241
115.58..
107.27
3.511I1E-02
..... 33E-02
3.078E-03
II. 51 7E - 03
1.2110E-02
MO xxrv
3D
EO'
7.81177E--Ol
(RYD)
N••
2.7057
MU'
.28.. 3
E (AYD)
(EV)
E PHOT (EV)
LAMBDA (A)
(L/A/L-l)
( L/R/L-O
SlaMA L-l
SIOMA L--l
SlaMA
(IIIB)
.0000
.000
1070.4711
Il.58
Il.855E-03
3.578E-02
1. 2114E -03
Il.1I1H-02
5.2113E-02
1 .00.00
13.11011
10&4.082
Il.44
Il.lIl1l1E-03
3.488E-02
1.223i-03
~ .1I72E-02·
5.01l"E-02
8.0000
108.847
11711.324
10.51
5.737E-03
2.113I1E-02
Il. 755E-04
3.8~IE-02
3.113I1E-02
MO XXIV
40
EO'
4.08BIIE-Ol
(AYD)
N••
3.7542
IIIU'
.2458
E (RYD)
E (EV)
E PHOT
(EV)
LAMIDA (A)
(L/R/L -Il
(L/R/L--l )
SlaMA L-l
SlaMA L-l
SlaMA
(MB)
.0000
.000
5511.0110
22.30
1.1183E-02
5.11114E-02
3 .1I58E -03
7.53lE-02
7.1127E-02
1.0000
13.BOII
51111.111111
21.711
1.1I11E-02
5. 7511E -02
3.71eE-03
7.115E-02
7.487E-02
8.0000
108.847
1184.1107
18.85
1.21!lE-02
4.~22E-02
2.487E-03
~.1I03E-02
5.14l1E-02
MO XXIV
50
EO'
2.!l388E--Ol
(RYDI
N••
~,71150
MU'
.2350
E (nD)
E (EV)
E P+tOT (EV)
LAMBDA (A)
(L/R/L-l )
(L/A/L--l )
SIOMA L- 1
SIOMA L--l
SlaMA
(MB)
.0000
.000
34!l. 1111
35.112
3.070E-02
8.1I07E-02
8. 177E-03
Il'841E-02
1.04I1E-Ol
1.0000
13.8011
358.7117
34.!l1l
2. U5E -02
8.10"E-02
7.401E-03
8.885E-02
Il.1125E-02
8.0000
108.8"7
454.008
27.31
1.872E-02
!l.572E-02
3.11118E-03
5.314E-02
5.714E-02
1110 XXIV
110
EO'
1. 730eE--0 1 (RYD)
N••
5.711111
MU'
.23011
E UVD)
E (EVI
E PHOT (EV)
LAMlSDA (A)
(L/R/L-l )
(L/A/L-l)
SIOMA L-l
SlaMA L--l
SIQMA (1118)
.0000
.000
235.411!l
52.1111
4.83H-02
1.147E-Ol
1.385E-02
'.IB8E-Ol
1.30IlE-Ol
1.0000
13.1I0e
2411.071
"11.78
4.37I1E-02
1 . 0!l4 E- 01
1.200E-02'
1.043E-Ol
1.1114E-Ol
2.0000
27.212
282.1177
47.20
3.lI8"E-02
Il.725E-02
1.048E-02
Il.3117E-02
1.0"2E-Ol
3.0000
"0.818
2711.283
"4.88
3.1141E-02
Il.00!lE-02
Il.205E-03
8.44I1E-02
Il.3117E-02
MO XXIV
80
EO' Il.!l3''!lE--00 (RYD)
N.'
7.7725
MU'
.2275
E (RVD)
E (EV)
E PHOT (EV)
LAMBDA (A)
(L/R/L-l)
(L/R/L--l)
SlaMA L-l
SIaMA L--l
SlaMl. (Mil)
.0000
.000
1211.7211
115.58
Il.4!l8E-02
1.7113E-Ol
2.1117E-02
1. 572E-Ol
1.8B"E-Ol
1.0000
13.1I0e
1043.332
811.!l0
7 .II~IIE -02
1 . !l4l1E- 01
2.27!lE-02
1.211I1E-Ol
1.52 .. E-Ol
3.0000
"0.818
170.5"4
72.70
5.853E-02
1.1117E-Ol
1 . 4 illE - 02
Il.210E-02
1.088E-Ol
Il.0000
81.835
211.3111
58.1111
3.11117E-02
8 .1I15I1E -02
8."8I1E-03
5.117I1E-02
Il. 82!lE-02
MO XXIV
100
EO' Il.0211I1E--00
(AVD)
N••
Il.77311
MU'
.22111
E (AVD)
E (EV)
E PHOT (EV)
LAM8DA (A)
(L/R/L-Il
(L/R/L--l)
SlaMA L- 1
SlaMA L--l
SIQIIIlA (Mil
.0000
.000
82.038
151.13
1.5"7E-Ol
2.!l33E-Ol
~.1I3I1E-02
1.1184E-Ol
2.478E-Ol
1.0000
13.11011
85.1144
1211. 113
1.18BE-Ol
2. 024E-0 1
3.382E-02
1.~78E-Ol
1 .• IBE-Ol
3.0000
40.818
122.8511
100.112
7. 1158E -02
1. 31111E-0 1
1.811E-02
Il. Oille -02
1. 087E-0 1
B.OOOO
81 .1135
1113.B74
75.7!l
~.eI2E-02
Il.01l5E-02
8.7!lOE-03
5.104E-02
5.117I1E-02
MO XXIV
120
EO' ... 15.. 111+00 UVD)
N•• Il.77''11
MU'
.2254
E (RVD)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/R/L-l)
( L/R/L--ll
SIalllA L-l
SlaMA L--l
SIQIIIlA (Mil
.0000
.000
511.527
2111.34
2.283E-Ol
3.3e4E-Ol
7."04E-02
2.411E-Ol
3.1!l2E-Ol
1.0000
13 .1I0e
70.133
1711.711
1.574E-Ol
2.453E-Ol
4.3118E-02
1. !l1l1E-0 1
2.028E-Ol
3.0000
40.818
117.345
127.37
8. 811H -02
1. !l10E -01
1 .UH -02
8.37"E-02
1 . 031 E-O 1
Il.0000
81.113!l
138. 1113
811.74
4. 71111E -02
8.1132E-02
7.11117E-03
4. 1!lIlE-02
4.I1I5I1E-02
MO XXIV
180
EO- 2.31"IIE--00 (AVD)
N.· 15.7753
MU'
.22"7
E IAVD)
E (EV)
E PHOT (EV)
LAM8DA (A)
(L/R/L-I)
(L/R/L--l)
SlOMA L-l
SIOMA L--l
SI aMI. .iMII)
.0000
.000
31. "112
3113.71
".141 E-Ol
5.288E-Ol
1.358E-Ol
3.317E-Ol
4.117I5E-Ol
1.0000
13.1I0e
4!l.01l8
274.113
2.23I1E-Ol
3.110E-Ol
!l.1I80E-02
1.114"E-Ol
2.212E-Ol
2.0000
27.212
58.704
211. 21
1. 4111E-0 1
2.102E-Ol
2.1173E-02
Il.778E-02
1.275E-Ol
".0000
54."24
8!l.1I1!l
1..... 31
7.30"E-02
1. 1811E-Ol
1.152E-02
4.580E-02
5.732E-02
!l.0000
118.030
1111.521
124.158
5.e3I1E-02
Il. 530E-02
7.lI!l!lE-03
3.408E-02
4.203E-02
MO XX IV
20D
EO·
1. ~72I1E+00 (AYD)
No.
111.7755
MU·
.22~5
E CAYO)
E (EV)
E PHOT (EV)
LAMBDA (Al
(L/A/L-l).
(L/A/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MBI
.0000
.000
20. O~O
1118.70
Il.~1I8E·01
7.53I1E-Ol
2.127E-Ot
~.2115E-Ol
Il.~22E-Ol
1.0000
13.11011
33.1I~8
3118.51
2.1182E-Ol
3.~83E-Ol
Il.08~E-02
1.53I1E-Ol
2. 1~7E-Ol
2.0000
27.212
~7.252
2112.~0
1 .~1I3E-Ol
2.0115E-Ol
2.lIdE-02
7.822E-02
1. 0~7E-0 1
~.OOOO
5~.~2~
7~ .~1I3
11111.51
8.7111E-02
1.058E-Ol
8.557E-03
3.1~2E·02
3.11117E-02
7.0000
115.2~f
1 15.281
107.55
3. 1211E-02
5. ~57E -02
2.832E-1I3
l ,211~E-02
1.578E-02
MO XX IV
~F
EO· 3.7772E+Ol
(AYD)
No.
3.11051
MU'
.01l~1I
E (AYD)
E (EV)
E PHOT (EV)
LAMIIDA (A)
(L/A/L-l)
(L/A/L+t)
SIGMA L- 1
SlaMA L+l
SlaMA
(MB)
.0000
.000
513.1121
2~. 13
8.518E-03
5. 1511E-02
1.00~E-03
~ .1I07E-02
!l.007E-02
1.0000
13.11011
527.527
23.50
8.0113E-03
~.8113E-02
9. 235E-0~
~.~80E-02
~.572E-02
8.0000
108. 8~7
1122.7118
111.91
5.1155E-03
3.33I1E-02
5. 311~E-0~
2.~1I3E-02
2. 5~7E-02
MO XX IV
5F
EO· 2.31111I1E+Ol
( AYD)
No.
~.1I02~
MU·
.011711
E (AYD)
E (EV)
PHOT
(EV)
LAMIIDA (A)
(L/A/L-l)
(L/A/L+ 1 )
SIGMA L- 1
SIGMA L+l
SIGMA
(Mil)
.0000
.000
3211.085
38.02
1.1123E-02
8. 813E -02
3.2~8E-03
Il. OIl~E -02
Il.~II1E-02
1.0000
13.11011
3311.11111
311.50
1.7721-02
8.1~lE-02
2.871E-03
8.085E-02
8,372E-02
8.0000
108. 8~7
~3~.1I32
28.!l1
1.01lIlE-02
~ .1I8~E-02
1.338E-03
3. 880E -02
~.01~E-02
MO XX 1V
IIF
EO.
1 . 1I11~3E +01
(AYDI
No.
5.11008
MU·
. 011112
E (AYD)
E (EV)
E PHOT (EV)
LAMBDA (A)
(L/A/L-l)
(L/A/L+I)
SIGMA L- 1
SlaMA L+l
SlaMA
(Mil)
.0000
.000
225.078
55.011
3.3~~E-02
1.21121-01
Il.780E-03
1.2B7E-OI
1.3155E-Ol
1.0000
13.11011
238.lIa~
5 , . 115
2.1185E-02
1.137E-Ol
!l.728E-03
1.10BE-Ol
1.1115E-Ol
2.0000
27.212
252.2110
~II. 1~
2.117I1E-02
1.02I1E-Ol
~. 875E-03
Il.58lE-02
1.00BE-Ol
8.0000
108. 8~7
333.1125
37.13
1.532E-02
Il.128E-02
2.112E-03
~.503E-02
~.71~E-02
MO XX 1V
8F
EO. Il. 2301lE+00 (AYD~
No.
7.811113
MU·
.1007
E (RYD)
E (EV)
E PHOT 1EV)
LAMBDA lAI
(L/A/L-l)
(L/A/L+l)
SlaMA L -1
SIGMA L+l
SlaMA
(MBI
.0000
.000
125.5115
IIB.72
7.220E-02
2.0115E-Ol
1.783E-02
1.lIaOE-Ol
2.1!1I1E-Of
1.0000
13.11011
1311.201
811.07
5.II!1I1E-02
1.771E-Ol
1.331E-02
1.5117E-Ol
1.700E-Ol
3.0000
~0.818
lBll.~13
7~.51
~.2!13E-02
1.31!1E-Ol
8.105E-03
1. 03~E-Ol
1.I15E-Ol
~.OOOO
15~.~2~
180.0111
118."
3.115I1E-02
1.151 E-O 1
Il. ~1I2E-03
8. !l1I7E-02
Il.21I1E-02
MO XX 1V
lOF
EO· 5.8785E+00 (AYD)
No.
Il.81187
MU·
.1013
E (AYD)
E lEV)
E PHOT (EV)
LAMIIDA (A)
(L/A/L-t)
(L/A/L+ 1 )
SlaMA L- 1
SIGMA L+l
SlaMA
(Mil)
.0000
.000
711.1183
1!15.02
1.2~~E-Ol
3.033E-Ol
3.332E-02
2.1I~IE-Ol
2.1175E-Ol
1.0000
13.11011
113.5811
132.~8
Il.33~E-02
2.3117E-Ol
2.19I1E-02
1.882E-Ol
2.1021 -0 1
~.OOOO
1I~.~2~
13~.~01l
112.25
~.757E-02
1.318E-Ol
8.1112E-03
8.38lE-02
Il.200E-02
8.0000
108. B~7
188.830
115.1111
2.~80E-02
7 .~~~E-02
3. 1211E-03
3. 718E -02
~.070E-02
MO XX 1V
12F
EO· ~.08.8E+00 (AYD)
No.
11.81183
MU·
.1017
E (AYD 1
E (EV)
E PHOT
II!V)
LAMIOA (A)
(L/A/L-l)
(L/R/L+ 1 )
SlaMA
L- 1
SIGMA L+l
SlaMA
(MS)
.0000
.000
55.318
223.17
1.898E-Ol
~.075E-Ol
5.357E-02
3.300E-Ol
3.83111!-01
1.0000
13.BOII
88.11113
179.711
1.278E-Ol
2.8117E-Ol
3.022E-02
2.07I1E-Ol
2.381E-Ol
~. 0000
5~.~2~
1011.781
112 .II~
!I.~17E-02
1.383E-Ol
8.877E-03
7.la8E-02
8.~0IlE-02
7.0000
115. 2~ f
150.5811
82.33
2.I7BE-02
8.21I1E-02
3.51171!-03
3. 1153E-02
~.013E-02
MO XXIV
ll1F
EO· 2.27110E+00 (RYD)
No.
15.81180
MU·
.1020
E IRYD>
E (I!V)
E PHOT 1EV)
LAMBDA (A>
( L/A/L-I)
(L/R/L+l )
SIGMA L- 1
SIGMA L+l
SlaMA
(Mil)
.0000
.000
31.007
31111,BII
3.57BE-Ol
8.~III1E·Ol
1.01lIlE-Ol
~.1I!l5E-Ol
5.72~1!-01
1.0000
13.11011
~~.1I13
277.111
1. 87111!-0 1
3.701E-Ol
~.227E-02
2 . II1~E - 0 1
2.11171!-01
3.0000
~0.818
71.825
172.82
7.1115E-02
1.75I1E-Ol
1. 212E-02
7.1178E-02
9.1110E-02
~.OOOO
1~.~2~
85.~31
1~5. 13
5.7~BE-02
1.3315E-Ol
7.803E-03
5. ~1I5E-02
Il. 2211E-02
7.0000
115.2~1
1211.2~1I
118.21
2.7113E-02
7. 0.~1!-02
2.585E-03
2.275E-02
2.535E-02
MO XX 1V
20F
I!O·
1 . ~5~81!+00 (RYD)
No.
111.811711
MU·
.1021
E IRYD)
E 1EV)
E PHOT (EV)
LAMBDA (A)
CL/A/L-l)
IL/R/L+l)
SlaMA
L- 1
SIGMA L+l
SIGMA CMI)
.0000
.000
111. 711~
1128.38
1.7~7E-Ol
Il. 25~E-Ol
1.7111 E-Ol
Il.087E-Ol
7 .8~71!-01
1.0000
13.11011
33.~00
371.22
2.28I1E-Ol
~. 1521-01
~.712E-02
2.0118E-Ol
2.53I1E-Ol
3.0000
~0.BI8
110.1112
20~.!l1I
7.828E-02
1.8421!-01
!l.ll8I1E -03
5.811I1E-02
Il.BIIIII!-02
5.0000
liB. 030
87. 82~
1~ 1. 18
3 .1I50E -02
Il.107E-02
3 . 1111 lE -03
2.11151-02
2.11851-02
48
DEFAUTS QUANTIQUES, ELEMENTS DE MATRICE DIPOLAIRES
ET SECTIONS EFFICACES DE PHOTOIONISATION
Appendice
séquence de K
Appendice 2
séquence de Rb
Appendice 3
séquence de Cu
Appendice 4
séquence de Ag
Pour chaque élement, les états nI sont classés par valeur croissante de 1
et pour chaque 1 par valeur croissante de n.
Pour chaque état nI, la première ligne précise
Nom de l'élement.
NL
état initial nI.
EO
valeur théorique du potentiel d'ionisation -e: nI'
*
N*
nombre quantique effectif n
de l'état nj ,
MU
valeur théorique du défaut quantique ~nl'
Les valeurs tabulées concernent :
E
énergie €
du photoélectron en Rydberg ou eV.
E PHOT
énergie du photon incident en eV.
0
LAMBDA
longueur d'onde du photon incident en A.
(L/R/LI ± 1)
: éléments de matrice dipolaires de transition Rnl,l ±
(e:) en u.a.
1
SIGMA L ± 1 : sections efficaces partielles de photoionisation onl,l ± 1 (e:) en
Mb (1Mb. 10- 18 cm2).
SIGMA
section efficace totale de photoionisation onl (c) en Mb.
K
4S
EO' 3.03701-01
IRYD)
N"
1.81411
MU'
2.1854
E (RYD)
E (EV)
E PHOT (EV)
LÀMIDÀ (À)
(L/R/L-I)
(L/R/L+I)
SlaMÀ L-I
SlaMÀ L·'
SlaMÀ
(MB)
.0000
.000
4.132
3000.54
.000
-3.725E-Ol
.000
3.1I02E-02
3.1I02E-02
.0200
.272
4.404
2815. 15
.000
-1.750E-OI
.000
8.472E-03
8.47U-03
.0400
.544
4.11711
21151 .34
.000
-2.1I00E-02
.000
1. S87E -04
1. S87E-04
.01100
.8111
4.S48
2505.54
.000
8.703E-02
.000
2.35I5E-03
2.355E-03
.0800
I.oee
5.221
2374.S4
.000
1.731E-OI
.000
8.834E-03
8.834E-03
.1000
I.3BI
15.483
22157.2$
.000
2.388E-OI
.000
1. SB8E -02
1 . IBIE -02
.3000
4.082
8.214
1501.47
.000
4. 178E-OI
.000
8.00IE-02
1.00IE-02
.4000
!1. 442
1.575
1284.811
.000
4.032E-Ol
.000
8.781E-02
1.78IE-02
.5000
Il.803
10.8315
1133.84
.000
3.7117E-OI
.000
8.750E-02
8.750E-02
1.0000
13.8011
17.738
e18.88
.000
2.538E-OI
.000
7.188E-02
7.I'8E-02
K
5S
EO'
1. 2442E-Ol
(RYD)
N.·
2.8350
MU'
2.11150
E (RYD)
E (EV)
E PHOT (EV)
LÀMIDÀ ( A)
(L/R/L-I)
(L/R/L+I)
SlaMA L- 1
SlaMÀ L·'
SlaMA
(M8)
.0000
.000
I.IIS3
7324.211
.000
-I.7111E+00
.000
3.30U-Ol
3.30lE-OI
.0200
.272
1.888
8308.14
.000
-8.1118E-OI
.000
9.172E-02
8. 172E -02
.0400
.544
2.237
151542.38
.000
-3.448E-Ol
.000
I.1I72E-02
I.1I72E-02
.0800
.8111
2.508
4141.32
.000
-3.497E-02
.000
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4.082
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4.320E-02
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1.340E-02
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5.554E+00
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10.820
1.145.88
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1.737E-03
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7.485E-03
8.0000
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4.1I111E+00
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10.885
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1.488E-03
3.575E-03
2.5811E-08
3.578E-03
2.5000
34.015
35.275
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5.811E-02
1.858E-02
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3.881E+00
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SIOMA (MB)
.0000
.000
.380
325sas. 15
-2.487E+OI
8.877E+OI
8.38laE+00
Il.458E+Ol
7.0la8E+Ol
.0200
.272
.8152
18002.73
-la.02laE+00
2.402E+Ol
1.432E+00
1.352E+Ol
1.4la5E+Ol
.0400
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.825
13401a.85
-4.557E+00
1.158E+Ol
5.172E-OI
4.437E+00
4.854E+00
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1.088
1.488
8441.21
-1.774E+00
4.085E+00
1.245E-Ol
8.801E-Ol
1.005E+00
.1000
1 .381
1.741
7121.81
- 1. 242E+00
2.730E+00
7.228E-02
4. 85IE -0 1
15.38 lE -0 1
.2000
2.721
3.102
3887.158
-3.54I1E-Ol
8.2la3E-Ol
1.0151 E-02
4.410E-02
5.4110E-02
.4000
5.442
5.823
2129.311
-8.587E-02
9.848E-02
1 . 1511E - 03
2.028E-03
3.184E-03
.11000
8. 1114
8.1544
14151.17
-3.580E-02
2. 31111E -02
2.848E-04
1.718E-04
4.11117E-04
.8000
10.8815
11 .2815
1100.113
-1.875E-02
5.484E-03
1.0117E-04
1.217E-015
1 . 188E -04
1.0000
13.11011
13.la811
8811.48
-1.085E-02
3.077E-04
4.51I1E-05
4.7154E-08
4.521E-05
2.0000
27.212
27.592
448.315
-8.418E-04
2. 1114E -04
8.5lalE-07
4.1141E-08
7.055E-07
3.0000
40.818
41. liai
300.85
7.811E-05
9.070E-04
8.845E-08
1. 217E -011
1.224E-OII
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SICMA CMB)
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1. '82E+02
1.507E+OI
1.072E+02
1.223E+02
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4.885E+Ol
4.102E+00
3.121E+OI
3.531E+Ol
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'113151.54
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1.128E+Ol
4.III1IE-Ol
3.4114E+00
3.830E+00
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1.088
1.302
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3.548E+00
9.058E-02
5.810E-Ol
Il.78I1E-Ol
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2.721
2.8315
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4.la80E-Ol
8.335E-03
2.1114E-02
3.247E-02
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15.442
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7. !S80E -02
8.437E-04
1.170E-03
1.814E-03
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1. 1114
8.377
1410.04
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1.837E-02
1. 587E -04
1.015E-04
2.1112E-04
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10.815
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1117.15
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4.450E-03
5.70IlE-05
7.882E-OII
Il. 4811E-05
1.0000
13.8011
13.820
887.18
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4.384E-04
2.428E-05
8.452E-08
2.437E-05
2.0000
27.212
27.4211
452.08
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1.455E-04
3.1I05E-07
2. 014E - 01
3.814E-07
3.0000
40.111
41.031
302.17
5.430E-05
8.51I1E-04
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8.841E+00
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8.552E-OI
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1 .2215
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8.013E-02
3.737E-Ol
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2.0000
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1.048E-04
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1.074E-08
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1.418E-07
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1!5.241
IIlS.lIall
1211.17
3.327E-03
2.03I1E-03
2.e7IE-0!5
1.411I1E-0!5
4.170E-0!5
10.0000
13e.0!511
13e.803
1I0.e3
1 .1I!5 1E- 03
3. 780E-03
1.301E-05
7.2112E-OlS
8.eOIE-0!5
12.0000
le3.271
le~.014
7!5.!511
1 .~7111-03
3.787E-03
Il.01H-oe
8.870E-OlS
Il. 772E-0!5
14.0000
1110.483
1111.22e
e4.84
1.170E-03
3.!57eE,.03
e.!57I1E-Oe
Il.220E-OlS
Il.878E-0!5
le.oooo
217.ell!5
2Ia.~38
!5e.7e
Il.4I1lE-04
3.210E-03
4.II~eE-oe
8.1113E-OlS
Il.~08E-0!5
SR
I l
12D
EO· 3.!58IeE-02
(IlYD)
No.
10.lSlS77
MU·
1. ~~23
E (AYD)
e 4EV)
E PHOT (EV)
LAM8DA
(A)
(L/A/L-l)
CL/R/L+I)
SIGMA L-l
SIGMA L+t
SIGMA
4M8)
.0000
.000
.488
2!5313.5e
-1.02IE+Ol
-2.24!5E+Ol
1.2781+00
Il.278E+00
1 . O!5eE-O 1
.1000
1.3el
1 . 8~1I
1570e.13
-e.712E-Ol
-4. e83E+00
2. 1~~E-02
1. !52I1E+OO
1.!550E+00
.2000
2.721
3.2011
38e3.17
-1. elli-Ol
-2.237E+00
2.32I1E-03
e.05~E-Ol
e.078E-Ol
.3000
4.082
4.!570
2713.03
-!5.eoee-02
- 1 . 3~3E-00
3.eIOE-~
3.IOIE-OI
3.113E-Ol
.~OOO
!5.442
!5.131
2010.el
-1.8171-02
-1I.00eE-OI
4.1123E-05
1.8142-01
1.81~E-Ol
.8000
15.803
7.211
1700.411
-3.0171-03
-e.4~5E-Ol
l.eHE-oe
1.142e-Ol
1. 1~2E-Ol
.8100
7.~.3
7.172
15!51.37
Il.~3eE-04
-!5.!54eE-OI
1.78~E-07
Il.2~eE-02
Il.24eE-02
.15000
8.1154
8.852
1~33.07
3.eO~E-03
-4.817E-Ol
2.82lSE-oe
7. !5eeE-02
7.!5ele-02
.7000
Il.lS24
10.012
1238.33
e.e03E-03
-3.714E-OI
1 . OIlH -011
!5.207E-02
!5.208E-02
1.0000
13.eoe
14.01l~
8711.70
8.!s2IE-03
-1.1127E-Ol
2.572E-0!5
1 .1I73E -02
1 .1I7!5E-02
1 . !5000
20.~01l
20.817
!5113.32
7.e01E-03
-1.2!52E-02
3.035E-05
!5.3e!5E-03
lS.315E-03
2.!5000
34.0111
34.503
3511.3!5
e.17eE-03
-2.~83e-02
3.30IlE-0!5
8.02IE-04
8. 352E -o~
3.0000
40.818
41.3015
300.17
!5.e78E-03
-1.5e4E-02
3.3~8E-OlS
3.801E-04
4.14~1-04
3.!5000
47.'21
48. lOI
2!57.72
!5.180E-03
-1.020E-02
3.2~lSE-OlS
1.885e-04
2.210E-04
4.0000
114.~24
14.1112
225.711
4.HIIE-03
-e.e3IE-03
3.03!5E-,O!5
Il.I02E-O!5
1.21~E-04
!5.0000
158.030
e8.!518
laO.15
3.7842-03
-2.282E-03
2.4eeE-olS
I.U!5E-O!5
3.8IIE-OII
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7~ .U3
71.321
le4.el
3.388E-03
-s . 03eE -04
2.173E-OII
2.31I1E-oe
2.40!5E-05
e.oooo
81. e3!5
82.124
150.17
3.027E-03
1.303E-04
1.8I12E-08
!5.2!58E-08
1.8In-0!5
e.!5000
88.~38
88.1127
131.43
2.713E-03
Il.03IE-04
1 . e~5E-05
2.735E-oe
1.IIII1E-O!5
7.0000
Il!5.241
Il!5.730
1211.!52
2.4~eE-03
1 .~7!5E-03
1.4401-0lS
7.8~8E-oe
2.225E-05
8.0000
108.847
1011.3315
113.40
2. 0~E-03
2.20eE-03
1.103E-01
2.007E-OlS
3.lloe-0!5
10.0000
13e.0511
13e.!5~7
110.80
1 .• 30E-03
2.748E-03
7.023E-oe
3. 88eE-0!5
4.!510E-OlS
12.0000
le3.271
le3.7!511
71.71
1.081 E-03
2.7HE-03
4.80IE-oe
4.730e-olS
!5 . 21 1E- OlS
14.0000
1110.~83
1110.1171
e~ .12
8.!5!5IE-04
2.eI2E-03
3.!510e-Oe
4.1114E-OS
!5.2eSE-os
le.oooo
217.ell!5
218.183
se.83
e.III~E-04
2.403E-03
2.e22E-oe
4.7~IIE-OS
!S. OllE-OS
12
SR 1 1
IISD
EO·
1.8871E-02
(RYD)
N·· 14.55110
MU·
1.4410
E (RYOI
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+I)
SIOMA L- 1
SIGMA L+l
SIOMA
(MBI
.0000
.000
.257
482811.211
-2.1112E+Ol
-3. 185E+Ol
3.102E+00
Il.811IlE+00
1.280E+Ol
.0500
.880
.837
13231.51
-1.884E+00
-8.1188E+00
8.184E-02
1.725E+00
1.808E+00
.1000
1.381
1.817
7888.02
-5.802E-Ol
-3.500E+00
1.38I1E-02
7.48I1E-Ol
7.808E-Ol
.2000
2.721
2.978
4183 .•11
-1.300E-Ol
-1.5.2E+00
1. 285E -03
2.888E-Ol
2.881E-Ol
.3000
•. 082
4.3311
2887.711
-4. 148E-02
-8.1172E-Ol
1.875E-04
1.317E-Ol
1. 3111E -01
.• 000
5 .•• 2
5.81111
2175.53
-1 . 355E -02
-5.1118E-Ol
2.82I1E-05
7.520E-02
7.523E-02
.4500
8.123
8.3711
11143.54
-8.1150E-03
-4.114.E-Ol
7.7.5E-08
5.87I1E-02
5.880E-02
.5000
8.803
7.080
1758.25
-2.811I1E-03
-4.1110E-Ol
1. 2113E-08
4.874E-02
4.874E-02
.5500
7.483
7.7.0
1801.811
7.800E-05
-3.5112E-Ol
1. 124E-OII
3.788E-02
3.788E-02
. 8000
8.18•
8.420
'.72 •• 7
1.1172E-03
-3.110E-Ol
8.22I1E-07
3.070E-02
3.070E-02
. 8500
8 . . . .
Il.101
1382 .• 0
3.1117E-03
-2.71H-Ol
2.338E-08
2.528E-02
2.528E-02
1.0000
13.808
13.883
8114.311
5.341E-03
-1.228E-Ol
Il.1I42E-08
7.883E-03
7.883E-03
1.5000
20.4011
20.888
51111.118
4.730E-03
-5.20lE-02
1.182E-05
2. 107E~03
2.1111E-03
2.0000
27.212
27.4811
451.37
4.188E-03
-2.888E-02
1.210E-05
7.381 E-O.
7 .• 82E-04
2.5000
3 •. 015
34.272
381.78
3.818E-03
- 1 .548E-02
1.255E-05
3. 01l5E - 04
3.22IE-04
3.0000
.0.818
41 .075
301.88
3.507E-03
-1I.720E-03
1.270E-05
1. 4t13E -04
1 . 5110E - 04
3.5000
47.821
.7.877
258.117
3.203E-03
-8.333E-03
1.23d-05
7.2311E-05
8 .• 73E-05
5.0000
88.030
88.288
181 .57
2.350E-03
-1.427E-03
Il.480E-08
5.2311E-08
1.472E-05
5.5000
74.133
75.0811
185. 12
2.0ll!lE-03
-5.871E-04
8.28.E-08
Il.10.E-07
Il. 1115E- 08
8.0000
81.835
81. 8112
151.40
1.873E-03
7.81I1E-05
7.21I1E-08
1. 7112E -08
7.237E-08
8.5000
88.438
88 . 8115
1311.711
1.884 E -03
5.4115E-04
8.325E-08
1.010E-08
7.335E-08
8.0000
108."7
1011.10.
113.84
1.248E-03
1.383E-03
4.2.8E-08
7.838E-08
1.1811E-05
10.0000
138.0511
138.318
110.118
8.818E-0.
1. 81111E -03
2.883E-08
1.483E-05
1.7.11E-05
12.0000
183.271
183.528
75.82
8.875E-04
1.710E-03
1.832E-08
1.803E-05
1.1188E-05
1•. 0000
1110.483
1110.740
85.00
5.305E-04
1.815E-03
1.350E-08
1.875E-05
2.010E-05
18.0000
217.8115
217.1151
58.811
4.30IE-04
1 .• 8I1E-03
1.013E-08
1.821E-05
1.1122E-05
SR I l
200
EO·
1.1812E-02
(RYO)
N·· 18.55118
MU·
1 .•• 04
E ( RYPI
E (EV 1
E PHOT (EV 1
LAMBDA
(A)
(L/R/L-l1
(L/R/L+I)
SIGMA L-1
SIGMA L+ 1
SIGMA
fM8)
.0000
.000
• t 58
78473 .• 5
-3.788E+Ol
-4. 130E+Ol
5.8118E+00
1.018E+Ol
1. 588E+0 1
.0500
.880
.838
147110.32
·1 . 850E +00
-5.882E+00
5.740E-02
1.021E+00
1. 078E +00
.1000
1.381
1.5111
8184.57
-4. 885E -0 1
-2.8152E+00
8.377E-03
4.057E-Ol
4.1.'E-Ol
.2000
2.721
2.8711
4308.31
-1I.1I27E-02
-1. 128E+00
7. 132E-0.
1.378E-Ol
1.383E-Ol
.3000
4.082
4.2.0
21124.38
-3.118E-02
-8.454E-Ol
1.034E-04
8.858E-02
8.8881-02
.4000
. 5.4.2
5.800
2213.110
,-' .018E-02
-4.223E-Ol
1.458E-05
3.788E-02
3.787E-02
.• 500
8.123
8.281
11174.10
-5.311 E-03
-3.51I1E-Ol
4.454E-08
2.1133E-02
2.1133E-02
.5000
8.803
8 .1l8 1
1781. 17
-2.1112E-03
-2.1178E-Ol
8.408E-07
2.328E-02
2.328E-02
.5500
7.483
7.8.'
1822.511
-8. 3211E -05
-2.548E-0\\
7. 8113E - 10
1.871E-02
1.871E-02
.tlOOO
8.184
8.322
14811.11.
1.284E-03
-2.203E-Ol
3.341E-07
1.522E-02
1.522E-02
.8500
8.844
Il.002
1377.34
2.208E-03
-1.1120E-Ol
1. 103E-08
1.252E-02
1.252E-02
1.0000
13.808
13.784
900.81
3.752E-03
-8.827E-02
4.870E-08
3.8t12E-03
3.887E-03
2.0000
27.212
27.370
453.00
2 .1It12E -03
- 1. 888E -02
8.03H-08
3.5113E-04
3.88.E-04
2.5000
34.015
34.173
382.82
2. 8511E -03
-1.080E-02
8.074E-08
1:503E-04
1.583E-04
3.0000
40.818
40.1178
302.58
2.434E-03
-8.771E-03
8.100E-08
7.0831-05
7.8113E-05
3.5000
47.821
.7.7711
2511.50
2.210E-03
-4.41lE-03
5.888E-08
3. 505E -05
4.0112E-05
5.0000
88.030
88.188
181.83
1.8211E-03
-Il. 888E -04
4.5411E-08
2.513E-08
7.082E-08
5.5000
7•. 833
74.11111
185.34
1 .••• E-03
-3.7.8E-04
3.1132E-08
3.1173E-07
4.330E-oe
8.0000
81.835
81.7113
151.58
1.211IlE-03
4. 855E -05
3.471 E-08
8. 88.E-OII
3.478E-08
8.5000
88.438
88.5118
1311.118
1.185E-03
3.8851-04
3.022E-08
4.538E-07
3 .• 75E-08
7.0000
115.24 1
115.31111
1211.117
1.038E-03
8.380E-04
2.588E-08
1. 455E -08
4.041E-08
10.0000
138.0511
138.217
111.02
8.032E-04
1.1118E-03
1.2.8E-08
7.342E-08
8.588E-08
12.0000
183.271
183.4211
75.87
4.755E-0.
1. 1711E-03
Il.287E-07
8.585E-08
Il.411.E-08
14.0000
1110.483
,110.8.,
l5!l . 04
3. 73.E -04
1.121E-03
8.882E-07
Il.032E-,08
Il.700E-08
18.0000
217.8115
217.853
58.111
2.873E-04
1.038E-03
4.521E-07
8.8•• E-08
Il.2118E-08
SR Il
4F
EO· 2.51178E-Ol
(RYD)
N.· 3.11242
MU·
.0758
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(AI
(L/R/L-l)
(L/R/L+1 )
SlolllA L- 1
SlaMA
L+l
SiGMA
(MBI
.0000
.000
3.534
3508.18
-1.732E+00
7.138E+00
2.858E-Ol
8.483E+00
8.7.IIE+00
.2000
2.721
8.255
11182.08
-5.872E-Ol
1.838E+00
5.420E-02
7.572E-Ol
8.11.E-Ol
.8000
8.18.
".8118
10511.111
-1.500E-Ol
3 .•81E-Ol
7.0111E-03
5.011IE-02
5.800E-02
1.0000
13.808
17.140
723.37
-5.857E-02
1.180E-Ol
1.58.E-03
8.588E-03
1.015E-02
2.0000
27.212
30.7.8
403.25
-7.504E-03
3. 1112E-02
4.883E-05
1.125E-03
1.17lE-03
Sil
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5F
EO-
1. 8812E-Ol
(RYD)
H·· 4.11071
MU·
.01l211
E (RYDI
E (EV 1
E PHOT (EV)
LAMBDA
(A)
(L/A/L-l)
IL/R/L+I)
SIGMA L- 1
SIOMA L+l
SIOMA
IMBI
.0000
.000
2.280
5485.72
-3.884E+00
1.274E+Ol
8.173E-Ol
1.318E+Ol
1 .• 00E+Ol
.0200
.272
2.532
4811tl.22
-2.1188E+00
1.021E+Ol
5.11118E-Ol
Il.487E+00
1.00IlE+Ol
.1000
1.381
3.821
3.2.,32
- 1 .50.E+00
4.1138E+00
2.205(-01
3. 170E+00
3.3111E+00
.2000
2.721
4.1181
24811.01
-8.051 E-0 1
2 .• 72E+00
8.8118E-02
1. 01l3E +00
1.180E+00
.8000
8.18.
10.42.
11811.48
-1.742E-Ol
4.0117E-Ol
8.522E-03
8.282E-02
7.13.E-02
"1.0000
13.808
15.888
781 .•8
-8.533E-02
1.303E-Ol
1.824E-03
Il.888E-03
1. 1411E-02
2.0000
27.212
211 .• 72
420.811
-1I.0511E-03
3.02lE-02
8.514E-05
Il. 855E-04
1.031E-03
SA Il
8F
EO·
1.1.95E-Ol
(UD)
H.· 5.811110
MU'
.1010
E (UD)
E (EV 1
E PHOT (EV)
LAMBDA
(A)
(L/A/L-Il
IL/A/L+I)
SIGMA L-l
SIGMA L+l
SIGMA
IMBI
.0000
. 000
1.58•
71127.53
-8.108E+00
1.838E+Ol
1.570E+00
1.8117E+Ol
2.05.E+Ol
.0800
.818
2.380
5208.74
-2.8011E+00
8.58I1E+00
5.058E-Ol
8.278E+00
8.782E+00
.2000
2.721
4.285
28113-.37
-1I.05U-Ol
2.855E+00
Il.488E-02
1. 085E +00
1. 1711E+00
.8000
8.184
Il.728
1274.5f1
-1. 585E-Ol
3.1174E-Ol
7.434E-03
5. 517E -02
8.281E-02
1.0000
13.808
15. 170
817.32
-8.114E-02
1.2111E-Ol
1.527E-03
8.100E-03
Il. 827E -03
SR 1 1
8F
EO· 8.42211E-02
(RYDI
H·· 7.81118
MU·
.1084
E (IIYO)
E (EVI
E PHOT (EV)
LAMBDA
(A)
(L/R/L-O
(L/R/L+1l
SIGMA L-l
SIGMA L+l
SIGMA
(MBI
.0000
.000
.874
14187.82
-1.24I1E+Ol
3.033E+Ol
3.873E+00
2.888E+Ol
3.253E+Ol
.0800
.818
1.8110
7335.40
-3.778E+00
1.00IlE+Ol
8.4118E-Ol
8. 175E+00
8.825E+00
.2000
2.721
3.511!!
34.8.78
-8.1177E-Ol
2.478E+00
7.802E-02
7.1112E-Ol
8.8112E-Ol
.8000
8.184
9.037
1371.112
-'.378E-Ol
3.248E-Ol
4.810E-03
3.420E-02
3.881E-02
1.0000
13.808
14.480
858.27
-4. 7117E-02
Il.5111E-02
8.1174E-04
4.783E-03
5.880E-03
13
SR II
lOF
EO· ".OaOBE-02
(RYD)
No.
a.BBB..
MU·
.11111
E (AYD)
E lEV)
E PHOT (EV)
LAMBDA lA)
(L/R/L-I)
IL/R/L+I)
SIOMA L-I
SIOMA L+l
SIOMA (MI)
.0000
.000
.5157
22271.08
-2.080E+OI
".350E+Ol
Il.''82E+00
3.78IE+OI
..... 2aE+Ol
.01100
.8111
1.373
1il030.1I1il
-".123E+00
1.0IBE+Ol
Il.2B5E-Ol
5.107E+00
5.735E+00
.2000
2.721
3.278
3782.11..
-7.1il38E-Ol
2. lII1E+OO
5.5113E-02
5.270E-Ol
5.82I1E-OI
.11000
8. Ill"
8.720
, .. 21. 8..
-1.01il2E-Ol
2.573E-Ol
2.802E-03
2.072E-02
2.353E-02
1.0000
13.11011
'''.1113
875."11
-3. 7211E -02
7."III1E-02
Il.2aIlE-0''
2.83"E-03
3.311"E-03
SR Il
12F
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E (RYD)
E (EV)
E PHOT 1EV 1
LAMIDA
lA)
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CL/R/L+\\)
SIOMA L- 1
SIOMA L+l
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3218a.211
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Il.7Ii1aE+Ol
lil.alaE+OO
".1I111E+OI
Il.1I''3E+Ol
.0200
.272
.1157
18B153.05
-1.211E+Ol
2.5"IIE+Ol
2.lIa7E+00
1.1130E+OI
1.78aE+Ol
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1.202
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-".088E+00
1il.II11E+OO
Il.''07E-Ol
3.aI5E+00
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2.721
3.1011
31ilal.37
-1I.810E-Ol
1.77IilE+00
3.880E-02
3.1130E-Ol
3.1il18E-OI
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8.184
B.5"1il
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-B.780E-02
2.0117E-Ol
1.77I1E-03
1. 311 E-02
1. "8aE-02
1.0000
13.11011
13.aal
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5.1il3I1E-02
3. 2alilE-0"
1.770E-03
2.100E-03
SR Il
18F
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1.11852E-02 (RYD)
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Ill. BB51
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117"811.117
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1.8"IIE+Ol
Il.''08E+Ol
1.211"E+Ol
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2.112I1E+OI
2."53E+00
1.207E+OI
1. "1I2E+OI
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1.032
12013.7a
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7.aIl3E+00
3.1I110E-OI
2.3S0E+00
2.705E+00
.1000
1.3111
1.11711
71111!l.10
-1.1137E+00
3.aI3E+00
1.137E-OI
8.1188E-Ol
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2.721
2.1il37
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8.183E-0"
Il.021E-03
1.83aE-03
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20F
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llil.88 ....
MU·
.11511
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1."28E+00
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1.381
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3.20IE-03
3.113i5E-03
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1.4170E+00 (RYD)
N.· 2.5202
MU'
2.47118
E (RYD)
E (EV)
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LAMBDA
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SIGMA L - 1
SIGMA L+l
SIGMA (MB)
.0000
.000
111.2711
843.11
.000
3.535E-Ol
.000
1.514E-Ol
1.514E-Ol
1.0000
13.801
32.8815
377.03
.000
2.312E-Ol
.000
1.104E-Ol
1.104E-Ol
2.0000
27.212
48.4111
288.811
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1.812E-Ol
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7.58I1E-02
7.58I1E-02
8.0000
108.847
128.128
118.77
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4.1140E-02
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1.1185E-02
1.11815E-02
Y III
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7. 11311E-0 1 (RYO)
N.· 3.55811
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2.4431
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1280.118
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5.884E-Ol
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1.1151E-Ol
1.1151 E-Ol
1.0000
13.808
23.2115
1532.47
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2.3118E-Ol
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8.413E-02
8.413E-02
4.0000
54.424
84.103
113.42
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8 . 1111 lE -02
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1 .1I811E-02
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8.0000
108.847
118.528
104.81
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3.248E-02
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7.8158E-03
7.858E-03
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2.81183E-Ol
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N.· 5.5744
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2.4258
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3.1141
3148.32
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1.058E+00
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2.780E-Ol
2.7150E-Ol
1.0000
13.808
17.547
708.81
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1 .1I88E-0 1
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4. 3511E -02
4.35I1E-02
4.~00
54.424
58.384
212.44
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4.148E-02
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8.310E-03
8.310E-03
Y III
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1 . 15811E - 0 1 (RYO)
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2.4204
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2.131
5818.111
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1. 5117E -00
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3.418E-Ol
3.418E-Ol
1.0000
13.808
15.737
787.85
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1.51I1E-Ol
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2.282E-02
2.2821-02
2.0000
27.212
211.343
422.54
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8.587E-02
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8.000E-03
8.000E-03
4.0000
54.424
58.5515
2111.23
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2.758E-02
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2.703E-03
2.703E-03
Y III
125
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2.4182
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1.334
112118.01
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2. 181 E+OO
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3.1188E-Ol
3.1188E-Ol
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8.803
8.137
1523.711
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2.84I1E-Ol
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3.588E-02
3.588E-02
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13.808
14.1140
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1.172E-Ol
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1.2110E-02
1.2110E-02
2.0000
27.212
28.548
434.34
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4.887E-02
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4.24I1E-03
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2.4184
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3.484E-00
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5.005E-Ol
5.005E-Ol
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8.803
7.487
1880.54
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1.825E-Ol
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1.582E-02
1.582E-02
1.0000
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14.270
888.811
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7.153I1E-02
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5.0118E-03
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2.111 08E - 02
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2.4158
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4.888E+00
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5.11411-01
5.1141E-Ol
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2.721
3.117
31177.49
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4.077E-Ol
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3.258E-02
3. 258E -02
1.0000
13.808
14.002
885.411
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5.218E-02
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2.488E-03
2.488E-03
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1.1205E+00 (RYO)
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15.245
813.27
1.105E+00
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3.811I1E-Ol
8.3I1U-Ol
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8.184
23.4011
5211.85
5.838E·Ol
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1. 55IE -0 1
1.8117E-02
2.527E-Ol
1.0000
13.808
28.851
4211.74
4.08I1E-Ol
-1.58ZE-Ol
1.001E-Ol
3.0215E-02
1.303E-Ol
1.5000
20.4011
35.854
347.75
2.1130E-Ol
-8.344E-02
8.413E-02
8.01IE-03
7.014E-02
2.0000
27.212
42.457
2112.03
2.237E-Ol
-1.838E-02
4.451E-02
4.7721-04
4.4118E-02
2.5000
34.015
411.280
251.70
1.77I1E-Ol
8.854E-03
3.285E-02
1.818E-04
3.281E-02
3.0000
40.818
58.083
221.15
1.458E-Ol
2.211I1E-02
2.41115E-02
1. 241 E-03
2.81I1E-02
8.0000
81.835
118.881
127.118
8.2811-02
3.1113E-02
8.008E-03
8.215E-03
1.422E-02
7.0000
1115.241
110.487
112.22
5.127E-02
3.777E-02
8.083E-03
8.802E-03
1.288E-02
8.0000
108.847
124.0113
1111.111
4.282E-02
3.588E-02
4.787E-03
8.887E-03
1 . 145E -02
Il.0000
122.453
137.81111
110.04
3.843E-02
3.381E-02
3. 827E - 03
8.5113E-03
1.0421-02
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8.0002E-Ol
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2.1271
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1518.74
1.1180E+OO
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8.7041-01
1.251E+00
1.1122E+00
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1.381
Il.524
1301.78
1.542E+00
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4.74IE-Ol
7.432E-Ol
1.217E+00
.8000
8.184
18.327
7511.38
8.457E-Ol
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1.4215E-Ol
Il.748E-02
2.400E-Ol
1.0000
13.808
21.770
5811.54
4.073E-Ol
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7.1583E-02
2.587E-02
1. 012E -0 1
1.5000
20.4011
28.573
433.113
2.842E-Ol
-8.2871-02
4.178E-02
4.731E-03
4.881E-02
2.0000
27.212
35.378
3150.411
1.88SE-Ol
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2.832E-02
4.773E-04
2. BIOl -02
2.15000
34.015
42.1711
2113.118
1.42111-01
3.8481-03
1.804 E-02
2.817E-015
1.807E-02
3.0000
40.818
48.1112
2153.13
1.130E-Ol
1.1518E-02
1.311 E-02
4.713E-04
1.3BU-02
3.5000
47.821
55.784
222.28
Il.2215E-02
2.11I1E-02
Il.1145E-03
1.04I1E-03
1 . OIlIlE -02
8.0000
81.8315
811.71111
138.07
4.3118E-02
2.828E-02
3.835E-03
2.5118E-03
8.233E-03
7.0000
115.241
103.405
1111.110
3.530E-02
2.512E-02
2.8118E-03
2.733E-03
5.431E-03
8.0000
108.847
117.011
105.lIe
2.1I11E-02
2.3eIE-02
2.077E-03
2.744E-03
4.821E-03
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122.453
130.817
114.112
2.45IE-02
2.21151-02
1.844E-03
2.888E-03
4.330E-03
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1.078E-02
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8.027E-03
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5.181E-05
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8.180E-03
1.555E-03
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8.2811E-Ol
1.044E-Ol
1.0000
13.11011
411.2011
251.118
2.1881-01
-3.580E-Ol
5.11201-02
2.31BE-Ol
2.11701-01
2.0000
21.212
82.815
1111.38
1.548E-Ol
-8 .1l0 11-02
3.7831-02
1.811E-02
5.1180E-02
2.5000
34.018
811.818
111.10
1.33I1E-Ol
-2.112E-02
3.1241-02
1.110E-03
3.241E-02
3.0000
40.818
711.421
182.24
1.1881-01
2.318E-02
2.11211 -02
1 . 8211E -03
2. 184E -02
3.8000
41.1121
83.224
148.118
1.032E-Ol
5.313E-02
2.228E-02
Il. 0811-03
3.134E-02
4.0000
54.424
110.021
131.12
Il.ll1eE-02
7.3111-02
1.1115E-02
1.844E-02
3.15I1E-02
8.0000
108.841
144.450
88.83
4.511E-02
1.02111-01
1.381E-03
5.7211E-02
Il.41181-02
Il. 0000
122.453
158. OSII
18.44
3.8211-02
Il.8110E-02
Il.1081-03
5.1114E-02
8.4051-02
10.0000
1311. 011Il
1 7 1 . 11112
12.23
3.444E-02
Il.384E-02
8.117E-03
5.7001-02
8.212E-02
21
ZR IV
50
10'
1.214111+00 (RYD)
N.· 3.152117
MU'
1.3703
1
(RYD)
1
(IV)
1
PHOT (IV)
LAMBDA
(A)
(L/R/L-I)
(L/R/L+l )
SIGMA L-l
SlaMA L+l
SIGMA
(MB)
.0000
.000
115.524
750.311
5.4331-01
-1.8841+00
1.22151-01
2.2101+00
2.3331+00
.2000
2.721
111.245
1544.25
4.34111-01
-1.3731-00
Il. 1311-02
1.31111+00
1.4801+00
.11000
8.803
23.327
531.112
3.2851-01
-8.88111-01
15.32111-02
15.Q4111-01
7.5821-01
1.0000
13.808
30.130
411 .51
2.2711-01
-4.57111-01
3.11081-02
2.3821-01
2.7731-01
2.0000
27.212
43.7315
283.411
1.3271-01
-1.2351-01
1.1371-02
2.5181-02
4.4541-02
2.5000
34.0111
50.531
2411.33
1.0771-01
-5.4251-02
1.4731-02
5.15081-03
2.0341-02
3.0000
40.818
57.342
2115.22
8.111501-02
-1.2031-02
1.157E-02
3.12n-04
1.1881-02
3.5000
47.821
84.144
113.21
7.15041-02
1 .4411 -02
Il.3241-03
5.0251-04
Il.8281-03
4.0000
54.42"
70.147
174.78
15.1111151-02
3.1211-02
7.151551-03
2.15081-03
1.027E-02
15.0000
81.835
118.151
1215.31
4.0381-02
5.4181 -02
4. OlliE -03
1.1111-02
1.5211-02
8.0000
108.847
12!i.371
18.110
2.775E-02
5.50U-02
2.427E-03
1.43l5E-02
1.8771-02
'.0000
122.4113
138.177
81.21
2.384E-02
5.281E-02
1 .1531 -03
1.4811-02
1.151181-02
10.0000
1315.0111
152.583
81.2!l
2.041E-02
5.0041-02
1. 518E -03
1.4411-02
1.8011-02
ZR IV
8D
10' 7.3753E-Ol
CRYD)
N·. 4.151177
MU'
1.3423
1
(RYDI
1
(IV)
E PHOT
(IV)
LAMBDA
(A)
(L/R/L-l )
(L/R/L-l)
SIGMA L - 1
SlaMA L+l
SIGMA
CM15)
.0000
.000
10.035
1235.58
8.201E-Ol
·2.888E+00
1 . 818E -0 1
3.1111+00
3.2811+00
.5000
15.803
18.838
738.315
3.778E-Ol
- 1.0581+00
8.040E-02
7.1011-01
7.713E-Ol
1.0000
13.1508
23 . lS<t 1
524.415
2.212E-Ol
-4.8801-01
3. 12IE -02
2.1051-01
2.417E-Ol
2.0000
27.212
37.247
332.88
1.177E-Ol
-1.2201-01
1.2181 -02
2.08111-02
3.38151-02
2.5000
34.015
..... 050
281.47
Il.2051-02
-5.15031-02
1.3831-03
5.2131-03
1.4801-02
3.0000
40.818
50.8113
243.82
7.4521-02
-1.7781-02
7.01181-03
8.0581-04
7.7041-03
3.5000
"7.1521
57.155!l
215.05
8.1101-02
5.3121-03
5.5531-03
8.1331-05
5.8151-03
4.0000
54.424
84.458
112.35
5.245E-02
1.11571-02
".45IE-03
1.3011-04
Il. 3811 - 03
5.0000
81 .835
111.570
135.25
3.0101-02
3.1I02E-02
2.2011-03
5.2511-03
7."821-03
8.0000
108.847
118.882
10".21
2.0741-02
3.1181-02
1.285E-03
8.88IE-03
8.1155E-03
1.0000
122.413
132.488
13.118
1.7511-02
3.7481-02
1 .0211 -03
7.0111-03
8.0401-03
10.0000
1315.051
1415.014
84.87
1.501E-02
3.5441-02
8.2781-04
15.11111-03
7.7471-03
lA IV
8D
10' 3.1I102E-Ol
CRYO)
N.· 15.15757
MU'
1.3243
1
CRYD)
E CIVI
E PHOT
(IY)
LAMaOA
1A)
CL/R/L-ll
CL/R/L+11
SIQMA L-l
SlaMA L-l
SIGMA
CMBI
.0000
.000
4.885
21138.17
1.1071+00
-5.221'+00
2.7111-01
5.0311+00
5.3101-00
.15000
15.803
11.1588
10150.82
3.11881-01
-1.1381+00
".8251-02
5.151111-01
15.1531-01
1.0000
13.15015
18.411
1570.53
1.1141-01
-4.3711-01
1 .8411-02
1.3321-01
1.517E-Ol
2.0000
27.212
32.0117
3815.21
8. 7715'e -02
-11.7551-02
15.213E-03
1.152E-02
1.7731-02
2.'000
31·015
38.100
318.73
15.5141-02
-4.5221-02
... 252E - 03
2 . IISII - 03
7.2511-03
3.0000
40.818
45.703
271.21
5.1881-02
- 1 .15421 -02
3.01111-03
4.15"41-04
3.55151-03
3.5000
47.821
52.5015
2315. , ..
".217E-02
3.1171-04
2.3471-03
1.1231-07
2.347i-03
4.0000
54."24
51.301
2011. OS
3.5141-02
1.0351-02
1 . 84 lE -03
2.3a.l-04
2.0801-03
15.0000
81.U5
815.520
1"3.30
1 .11851-02
2.3531-02
8.5721 -04
1.80151-03
2.151531-03
8.0000
108.847
113.732
101.02
1.3031-02 .
2.31541-02
".8521-04
2.3171-03
2.883E-03
1.0000
122.453
127.338
17.37
1.0SI21-02
2.2581-02
3 . • 171-04
2.447E-03
2.8211-03
10.0000
1315.0511
140.1144
87.17
Il.3041-03
2.1301-02
3.01571-0"
2.41 11-03
2.717E-03
lA
IV
10D
10' 2.1227E-Ol
CRYD)
N••
8.15820
MU'
1.3180
1
(RYD)
1
CIV)
1 PHOT
CIV)
LAMaDA
CA)
CL/R/L-l)
(L/R/L+O
SlaMA
L - 1
SlaMA
L-l
SIGMA
(M15)
.0000
.000
2.888
"213.05
2.3401+00
-8.015111+00
3.11741-01
7.0821+00
7.4801+00
.2000
2.721
5.1501
2210.31
8.3421-01
-2.7481+00
Il.81IE-02
1.51171+00
1.15151+00
.5000
15.803
Il.1511
12711.31
3.15241-01
- 1.0471+00
3.111111-02
4.0021-01
".3221-01
1.0000
13.15015
115.41"
751.71
1.15241-01
-3.51111-01
1 .01131 -02
8.0551-02
1.1481-02
2.0000
27.212
30.100
411.112
15.5113E -02
-7.5081-02
3.2881-03
15.31171-03
1.158151-03
3.0000
40.818
43.7015
283.68
3.774E-02
-1.3031-02
1.51541-03
2.8001-0"
1.8441-03
3.5000
47.1521
50.1501
245.47
3.0381-02
-15 . UII - 04
1.172E-03
8 .• 1151-07
1.1731-03
.... 0000
54.424
57.312
2115.34
2.5131-02
15.8521-03
1. OUI - 04
1.51511-05
1.0051-03
15,0000
81.15311
8".524
1415.151
1.31141-02
1.151lE-02
4. 1211·- 0..
8.2701-04
1.2"01 -03
8.0000
108.847
111.735
110.118
Il.082E-03
1.15111-02
2.3071-04
1.104E-03
1.3351-03
Il.0000
122.413
125.341
18.12
7.5811-03
1.54"1-02
1 .8051-04
1.12151-03
1.3071-03
10.0000
1315.01l1
138.147
81.23
15.435E-03
1.411151-02
1 .44151 -04
1.1101-03
1.2541-03
ZR IV
12D
10'
1.40141-01
CRYO)
N··
10.681S0
MU'
1. 3150
1
(RYD)
1
CIV)
1 PHOT
CIV)
LAM15DA
CA)
(L/R/L-ll
(L/R/L+I)
SlaMA
L-l
SlaMA L-l
SIGMA
(M15)
.0000
.000
1.1107
15502.31
3.21IE+OO
-1.131S1+Ol
5.2181-01
Il.21581+00
1.7811+00
.1000
1.3151
3.2157
371".158
1."111+00
-4.8501+00
1 .15531-01
2.8181+00
3.01541+00
.2000
2.721
4.1528
21571.07
8.2811-01
-2.7"151+00
7 . 112E - 02
1.31151+00
1.31151+00
.5000
15.803
8.710
1423.54
3.1541-01
-1.1531-01
2. 171E -02
2.7511-01
2.1115IE-Ol
1.0000
13.15015
15.513
71111.28
1.3171-01
-2.1331-0-1
8.7511-03
5.0311-02
5.7071-02
2.0000
27.212
29. 111
42'.80
5.1081-02
-5.8831-02
1 . 1011- 03
3.711111-03
Il.70111-03
2.5000
34.015
35.122
345.115
3.7281-02
-2.7121-02
1.2551-03
1.1I1S11-04
2.2511-03
3.0000
40.818
42.725
2110.20
2.8741 -02
-1.033E-02
8.8701-04
1. 7181-04
1 . OISIE - 03
3.5000
47.1521
411.527
250.34
2.302E-02
-8.3221-04
15 . 5114E• 04
1:21131-015
15.15071-04
4.0000
54.424
58.330
220.11
1.8118E-02
4. 7411E-03
5.0101-04
".78111-05
Il.S8111-04
15.0000
81.1535
83.1142
148. '"
1.042E-02
1.18111-02
2.2811-0"
4 . 4 55 E- 04
15.7381-04
8.0000
108.847
110.754
11 1 .115
8.7451-03
1.11151-02
1. 215ISE - 04
5.111521 -04
7.22I1E-04
Il.0000
122.453
124.3150
1111.70
5.15271-03
1.13111-02
1 . 811ISE - 05
15.0871-04
7.0771-04
10.0000
138.0511
137.11158
81.87
".7741-03
1.0731 -02
7.1041 -OS
5.1111-04
8.78IE-04
lA IV
180
10' 7.41881-02
(RYO'
No.
14.158715
MU'
1. 3124
1
(RYD)
1
llV)
1
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LAM15DA
CA)
CL/R/L-l)
(L/Rh+l:
SlaMA
L-l
SIGMA L+l
SlaMA
(M15l
.0000
.000
1. 001
122815.53
5.15541+00
- 1 .12 1E +0 1
7.8251-01
1.4051+01
1.4831+01
.1000
1.381
2.370
5232.12
1.4551+00
-5.0311+00
1.21511-01
2.21511+00
2.3881+00
.2000
2.721
3.730
3323.715
7.2281-01
-2."141+00
4.81151-02
8.1151-01
8.15851-01
.5000
15.803
.7.812
1587. Il
2.3331-01
-15.802E-Ol
1.01511 -02
1.31531-01
1.4701-01
1.0000
13.15015
1".1515
848.35
1.01151-02
-2.0181-01
2.1187E-03
2.24111-02
2.5431-02
2.0000
27.212
28.221
431.34
3.3421-02
-3.88U-02
7.1231-0"
1.15011-03
2."011-03
2.5000
34.015
35.02"
35".00
2 .• 1151-02
- 1 .787E-02
5.1371-04
4.2151-04
Il.352E-04
3.0000
40.818
41.827
21115.43
1.81S01-02
-8.8781-03
3.51171-04
7.41511-05
4.3441-04
3.5000
47.1521
48.1530
254.115
1.4741-02
-7.2221-0"
2.155151-0"
1.51531-07
2.1515151-04
".0000
54.424
55.433
223.157
1.2101-02
2.8721-03
2.03111-04
1.7241-05
2.2111-04
15.0000
81.U5
82.1545
150.02
15.!lSI11-03
7.4311-03
1.0251-05
1.7211-04
2.15231-0"
22
ZA IV
200
EO· 4,58'OE-02
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N·· '8,11887
MU'
1.3113
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(L/R/L+I)
SIOMA L-l
SIQMA L+l
SIGMA CMB)
,0000
.000
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8.2'8E+00
-2.870E+Ol
1.058E+00
1.1135E+0'
2.041E+01
.0500
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1.304
11151' .20
2.51S5E+00
-1I.05I1E+00
2,15ISE-0,
4,034E+00
4,24I1E+00
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, . 31S 1
1.11&4
112411,70
1.33I1E+00
-4,1I111E+00
8,8II8E-02
1.1125E+00
',714E+00
,2000
2.721
3.3"4
3707,20
5.117I1E-Ol
-2.007E+00
3.002E"02
5.078E-Ol
5.378E~01
,5000
Il.103
7.4211
181111,57
1,7114E-Ol
-5. 154E-Ol
5.811 E-03
7.43I1E-02
8.020E-02
1,0000
'3.11011
14.2211
871,35
Il. 5115E-02
-1.473E-Ol
, .542E-03
1.1114E-02
1.318E-02
2.0000
27,212
27,835
448.43
2.384E-02
-2.78I1E-02
3.117I1E-04
8. 143E-04
" 212E -03
2.5000
34.0'5
34,1S38
387,115
'.7'5E-02
-1.277E-02
2.58lE-04
2.130E-04
4.1I111E-04
3.0000
40.818
41.441
2111,111
1.308E-02
-4,1141 E-03
1.783E-04
3.814E-05
2.1115E-04
3.5000
47.1S21
48.244
257.00
1.04 'E-02
-5.424E-04
1,313E-04
5.35'E-07
1.31SE-04
4.0000
54.424
55.0.. 7
225.24
8,541E-03
1.11117E-03
1. OOIIE -04
8.02I1E-OII
1.01l0E-04
Il.0000
81. 835
82.2511
'50.73
4.1132E-03
5,1117E-03
4.437E-05
8.377E-05
, ,28lE-04
8.0000
108.847
1011,471
113.211
2.11751-03
5,225E-03
2.435E-05
1.'27E-04
'.3701-04
Il.0000
122,453
123,077
100,74
2.4721-03
4,111161-03
1,8110E-05
1. 144E-04
1.333E-04
'0.0000
1311,0511
1311.1182
110.71
2. '0'1 -03
4.1180E-03
, .517E-05
1.12I1E-04
1.280E-04
ZR IV
4'
EO·
1,01l·70E+00 (RYD)
N·· 3.8111'
MU'
.18011
E (RYD)
E (EV 1
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LAMISDA (A)
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CL/R/L+I)
SlaMA L- 1
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SIOMA
(Mil)
.0000
.000
14.1125
830.72
-2,27'E-Ol
2.347E+00
2,073E-02
2.11531+00
2.1174E+00
.15000
Il,803
21.728
570.113
-8. 1311E-02
1, '48E+00
3.87I1E-03
1,028E+00
1.032E+00
',0000
13.11011
28.1531
434.57
-3. 180E-02
Il.8'2E-0'
7.770E-04
4.754E-0'
4.7112E-0'
2,0000
27.212
42.137
2114,.25
-, .832E-03
3.2',E-0'
4,237E-OII
1.5110E-0'
, .5110E-Ol
3,0000
40.818
55.743
222,43
4.71I1E-03
1,811I1E-Ol
3. 33I1E-015
8,8118E-02
Il.801E-02
ZlI IV
5'
EO· 7.0362E-Ol
(RYD)
N·· 4.711811
MU·
.2314
E (RYD)
E (EVI
E PHOT (EV)
LAMIDA
(A)
(L/R/L-l)
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SIOMA L- 1
SIGMA L+l
SIGMA
(Mil)
.0000
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Il.573
121115, 12
-5.074E-Ol
3.1134E+00
8.113111-02
4.540E+00
4.808E+00
,5000
Il,803
111.3711
757. , 1
-1.3117E-0'
1,470E+00
8.2441-03
1,27lE+00
1.27tll!+00
, .0000
13.1I01S
23.1711
534.110
-4.72111-02
7.115I1E-Ol
, ,388E-03
5.2721-01
5,28I1E-Ol
2.0000
27.212
311.785
337,011
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3.43,E-Ol
1.238E-05
1.51551-01
, .55I5E-0'
3.0000
40.8'8
50.3111
248,015
4.700E-03
1.1I0lE-Ol
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Il. 537E -02
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ZR IV
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CA)
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SlOMA (Mil)
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Il.582
1880.711
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4.75111+00
1,3118E-Ol
5.3112E+00
5.411I1E+00
.5000
Il.803
13.3115
1125.80
-1.728E-Ol
1 . 5114E +00
1.07SE-02
1.17I1E+00
1.187E+00
1.0000
'3.8011
20. '118
1113.85
-5.33I1E-02
7,81I1E-Ol
1.54111-03
4.43lE-Ol
4.447E-Ol
2.0000
27,2'2
33.804
3811.78
-4.030E-03
3,'48E-Ol
, .47I1E-05
1,203E-Ol
1.203E-Ol
3,0000
40.818
47.4'0
2111,52
4. '571-03
, , 1183E-0 1
2.20IlE-05
4.877E-02
4.87111-02
ZR IV
8'
EO· 2,1I711,E-Ol
(RYD)
N·· 7,7280
MU·
.2720
1 (RYO)
1 (EV)
1 PHOT
(EV)
LAMISDA
CA)
(L/R/L-I)
(L/R/L+')
SIOMA L- 1
SIOMA L+l
SIGMA (Mil)
.0000
.000
3.1145
3401,4'
- 1 , Il , 2 E+00
Il.1124E+00
3.588E-Ol
Il.278E+00
Il.1I35E+00
,5000
Il.803
10.448
, 1811. 1111
- 1. 1111111 - 0 1
'.482E+00
1. 124E-02
8.240E-Ol
8.353E-Ol
'.0000
13.11011
17.25'
7'8.72
-5.203E-02
Il.581E-0'
1.2581-03
2.883E-Ol
2,888E-OI
2.0000
27,2'2
30.857
401.81
-3.7"OE-03
2.428E-Ol
i . '1I3E-05
Il. 531E-02
Il.53I1E-02
3,'0000
40.8'8
44,4113
278.85
3.01151-03
',28lE-Ol
'.147E-05
2.53111-02
2.540E-02
4,0000
54.424
58.0811
213.52
4.01131 -03
7,1I84E-02
2.11201-05
'.23lE-02
1.234E-02
ZR IV
'0'
10· 1.111134E-Ol
(RYO)
N.· 8.7204
MU·
,271111
1 (RYD)
E (IV)
E PHOT
(EV)
LAMIDA
(A)
(L/R/L-I)
(L/R/L+I)
SlaMA L- 1
SIQMA L+ 1
SI QIIIA (Mil)
,0000
.000
2,304
5381,41
-3,3471+00
8.137E+00
Il,852E-Ol
Il.807E+00
7.11031+00
.5000
Il,803
Il. '07
'31S1 .45
-1.838E-Ol
1.2114E+00
Il.212E-03
5.475E-Ol
15,51S71-01
1.0000
'3.ISOII
15,810
7711,30
-4 . 5215E- 02
5,32I1E-Ol
8,7751-04
" 1123E-0 1
I,UlE-Ol
2.0000
27,2'2
211.5'11
420.07
-3.1 'SE-03
1,873E-Ol
7,7301-01S
3.7'111-02
3.720E-02
3.0000
40.818
43, '22
287,53
2.350E-03
8.54I1E-02
6,412E-OII
1.412E-02
'.413E-02
4.0000
154.424
58,728
218.511
3. '041-03
5,7115E-02
1.472E-05
Il, 770E-03
Il.784E-03
ZR IV
'2'
EO·
1, '1I155E-Ol
(RYD)
N·· 11,7'1111
MU·
,2834
E (RYDI
E lEV)
1 PHOT
(EV)
LAMIDA
lA)
(L/R/L-l )
(L/A/L+')
SIGMA L- 1
SIOMA L+l
SIOMA (Mil)
.0000
,000
1,581S
7818.57
-5, 184E+00
1. '45E+Ol
1. ,48E+00
7.41171+00
8.1114E+00
,2000
2.721
4,307
2878.73
-7.481S1-Ol
2.115 lE+OO
Il.411IE-02
1.347E+00
1. 4' 2E+00
. ISOOO
8.184
Il,748
'271.74
-1.233E-Ol
8,777E-0'
3.1I110E-03
2.1S17E-Ol
2.737E-Ol
1.0000
'3.11011
'5.1112
8'11. '4
-3.8341 -02
4.33I1E-0'
Il.014E-04
1. 027E-Ol
, .033E-Ol
2.0000
27.212
28.7118
430.54
-2.5741-03
1,48,E-Ol
5, '38 E• 011
2,2118E-02
2.211IE-02
3,0000
40.818
42.404
282.40
1. 8311E-03
7,473E-02
3,8113E-OII
8,503E-03
8.507E-03
4.0000
54,424
511.0011
221.37
2,434E-03
4.488E-02
8.1137E-OII
4.01l0E-03
4. 0511E -03
ZR IV
'11'
EO. Il.48051-02 (RYD)
N·· '8.7'211
MU'
.2871
E ( RYO)
1 (EV)
E PHOT
(IV)
LAM5DA (Al
( L/R/L-O
(L/R/L+O
SIOMA L-'
SIOMA L+'
SIGMA (Mil)
,0000
.000
,882
'4011',78
-1,004E+0'
1.1143E+0'
2.383E+00
8.545E+00
1,08"E+Ol
. '000
1 . 3111
2.242
511211,38
-1.773E+00
4,74'1+00
, . 8118E -0 1
1.8'OE+00
2.000E+00
.2000
2.721
3.1103
344' , 28
-1I.183E-Ol
2,4153E+00
4.7051-02
7.7831-0'
8.254E-Ol
.11000
8.1114
8,045
1370.73
-8. 40SE -02
Il.330E-Ol
2.15I1E-03
1.30lE-Ol
1.323E-Ol
1.0000
'3.11011
'4.488
858.81
-2,773E-02
3,013E-0'
3. OOOE -04
4.724E-02
4.7541-02
2.0000
27.2'2
28.0114
441.33
-'.7117E-03
8,1I78E-02
2.443E-06
1,004E-02
1,005E-02
3.0000
40,8'8
41 .1188
287,33
1.231E-03
4.87111-02
',70lE-08
3.7121-03
3.713E-03
4.0000
84.424
55.305
224. '8
1.82' E-03
2.11721-02
3.814E-01I
1 . 755E -03
, . 758E -03
23
ZR IV
20f
EO· 4.1180E-02
(RYD)
N'"
UI.7113
MU'
.2887
E (RYD)
E lEV)
E PHOT lEV)
LAMIIDA
lA)
(L/R/L-l)
IL/R/L+l)
SIGMA L - 1
SIGMA L·l
SIGMA
IMII)
.0000
.000
.SIO
22128.74
-1.143E+Ol
2.188E+Ol
4.075E+00
SI.134E+00
1.371E+Ol
.0500
.180
1.241
SlSISI4 . 13
-3.8S14E+00
7.112E+00
5.015E-Ol
2.581E+00
3.088E+00
.2000
2.721
3.281
3778.37
-5.SlSlSlE-01
1 . SlSIIE + 00
3. 181 E-02
4.ISl5E-Ol
Il.013E-Ol
.1000
8.114
8.724
1421.23
-7.214E-02
4.757E-Ol
1.240E-03
7.088E-02
7.212E-02
1.0000
13.101
14. III
875.23
-2.084E-02
2.222E-Ol
1. 157E-04
2.512E-02
2.528E-02
2.0000
27.212
27.772
441.44
-1.32S1E-03
7.247E-02
1.321E-06
5.237E-03
5 . 2311E - 03
3.0000
40.818
41. 378
2S1S1.14
B.8S15E-04
3.5S1S1E-02
8.817E-07
1 . Sl24E -03
1 .ll25E - 03
4.0000
S4.424
54.Sl84
225.!l0
1. 174E -03
2.144E-02
2.041E-06
SI.0711E-04
SI . OSlSlE - 04
24
NI V
I5S
EO'
2.11822E+00
(AYO)
N··
2.8854
MU'
2.10411
E (AYO)
E (EV)
E PHOT (EV)
LAMIOA (A)
(L/A/L-I)
(L/A/L+l)
SIQMA
L-l
SIGMA
L+l
SIGMA
(Mill
.0000
.000
40.5711
305.57
.000
2.1118E-Ol
.000
1.747E-Ol
1.747E-Ol
2.0000
27.212
117.787
182.110
.000
1.480E-Ol
.000
Il.4113E-02
8.4113E-02
Il.0000
81.135
122.211
101.45
.000
7.278E-02
.000
4.0118E-02
4.0118E-02
Nil V
liS
EO'
1.11184E+00
CAYOI
N··
3.112111
MU'
2.07011
E (AYO)
E (EV)
E PHOT (EV)
LAMIIDA
(A)
(L/A/L-l)
(L/A/L+l)
SIGMA L-l
SIGMA
L+l
SIGMA
(MBI
.0000
.000
22.033
5112.72
.000
4.103E-Ol
.000
2.331E-Ol
2. 33 lE -01
2.0000
27.212
411.245
251 . 77
.000
1.548E-Ol
.000
7.4 IllE -02
7.41I1E-02
Il.0000
81 . 1135
103.111111
1111.110
.000
5.875E-02
.000
2.24I1E-02
2.24I1E-02
12.0000
1113.271
185.304
1111.111
.000
2.735E-02
.000
8. 714E -03
8.714E-03
Nil V
8S
EO'
7.01187E-Ol
(AYO)
N··
5.11470
MU'
2.0530
E (AYO)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/A/L-l)
(L/A/L+l)
SIQMA
L - 1
SIQMA
L + 1
SIGMA
(Mill
.0000
.000
Il.1118
12811. 111
.000
7.83I1E-Ol
.000
3.711E-Ol
3.71lE-Ol
2.0000
27.212
311.8211
3311.115
.000
1. 344E - 0 1
.000
4.183E-02
4.183E-02
Il.0000
81.1135
81.253
135.87
.000
3.87lE-02
.000
8.5111E-03
8.581E-03
12.0000
1113.271
172.8811
71. 71
.000
1 . 1132E -02
.000
2.883E-03
2.8113E-03
NB V
lOS
EO' 3.1152I1E-Ol
(AYO)
N··
7.115211
MU'
2.0474
E (AYOI
E (EV)
E PHOT (EV)
LAMIOA (A)
(L/A/L-l)
IL/AIL+I)
SIQMA
L- 1
SIQMA
L+l
SIGMA
(MI)
.0000
.000
5.378
23015. 31
.000
1.23I1E+00
.000
5.188E-Ol
5.188E-Ol
2.0000
27.212
32.5110
380.44
.000
1.070E-Ol
.000
2.34I1E-02
2. 34 lIE -02
4.0000
54.424
58.802
207.33
.000
4.558E-02
.000
7.808E-03
7.808E-03
8.0000
108.847
114.2211
108.55
.000
1.8114E-02
.000
2.4113E-03
2.4113E-03
Nil V
12S
EO'
2.522I1E-Ol
(AYO)
N.·
Il.11551
MU'
2.04411
E (AYO)
E (EV)
E PHOT (EV)
LAMIIOA
(A)
(L/A/L-I)
(L/A/L+ 1 )
SIQMA L- 1
SIGMA
L+l
SIGMA
(Mil)
.0000
.000
3.432
31112.44
.000
1.7eIlE+00
.000
Il.748E-Ol
Il.74U-Ol
2.0000
27.212
30. lI44
404. '10
.000
8.4112E-02
.000
1.38I1E-02
1.38I1E-02
4.0000
54.424
57.8511
214.30
.boo
3.443E-02
.000
4.30IlE-Q3
4.308E-03
Nil V
1liS
EO'
1.2833E-Ol
(AYO)
N.·
13.11573
MU'
2.0427
E CAYO)
E (EV)
E PHOT (EV)
LAMIOA U)
IL/A/L-I)
CL/A/L+l)
SIGMA L - 1
SIGMA
L+l
SIGMA
(Mil)
.0000
.000
1.7411
7100.711
.000
3.037E+00
.000
1.012E+00
1. 012E+00
.2000
2.721
4.4117
2775.44
.000
8.300E-Ol
.000
1.1134E-Ol
1 .1I34E -0 1
.5000
6.803
8.549
1450.211
.000
3.287E-Ol
.000
5.80eE-02
5.80eE-02
1.0000
13.1106
15.352
807.'12
.000
1.413E-Ol
.000
1.1125E-02
1.925E-02
2.0000
27.212
28.1158
428.16
.000
5.e3I1E-02
.000
5.787E-03
5.787E-03
Nil V
20S
EO'
7.7521E-02
(AYO)
N.'
17.11581
MU'
2.0419
E (AYO)
E (EV)
E PHOT av)
LAMBOA
(A)
(L/A/L-I)
(L/A/L+I)
SIGMA L - 1
SIQMA L + 1
SIGMA
(Mill
.0000
.000
1 . 055
11755.15
.000
4.5118E+00
.000
1.383E+00
1.383E+00
.1000
1.3'11
2.415
5133.30
.000
1.427E+00
.000
3.01l0E-Ol
3.01l0E-Ol
.11000
8.1114
9.218
1345.00
.000
2.05I1E-Ol
.000
2.45I1E-02
2.45IE-02
1.0000
13.110'1
14. '1111
845.71
.000
1.048E-Ol
.000
1. 011E-02
1.011 E-02
2.0000
27.212
28.2117
438.113
.000
4.02I1E-02
.000
2.883E-03
2.883E-03
Nil V
5P
EO' 2.5178E+00
(AYO)
N··
3. 1511
MU'
1 .84811
E (AYO)
E (EV)
E PHOT (EV)
LAMBOA
(A)
(L/A/L-I)
(L/R/L+ 1 )
SIGMA L - 1
SIQIU L + 1
SIGMA
(Mil)
.0000
.000
34.257
3111.113
4.1I1I1E-Ol
-8.837E-02
1.73I1E-Ol
1 . 121 E-02
1.848E-Ol
.0500
.1180
34.1137
354.811
4.7118E-Ol
-7.817E-02
1.11114E-Ol
8.1144E-03
1.753E-Ol
.4000
5.442
311.111111
312.32
3.8113E-Ol
-2.445E-02
1.2eOE-Ol
8.841E-04
1. 270E-Ol
.11000
8.1114
42.420
282.28
3.505E-Ol
-3.773E-03
1.0111E-01
2.52I1E-05
1.0112E-Ol
.8000
10.885
45. 14 1
274.'1'1
3. 1711E-Ol
1. 201E-02
Il.538E-02
2.72I1E-04
8.5115E-02
1.0000
13.110'1
47.8113
258.05
2.8.5E-Ol
2.415E-02
8.403E-02
1.1e.E-03
8.518E-02
2.0000
27.212
111.4118
201.71
1.848E-Ol
5.40IlE-02
4.883E-02
7.527E-03
5.lI4I1E-02
3.0000
40.818
75.074
1'15. 15
1.422E-Ol
Il.14I1E-02
3.180E-02
1.188E-02
4.3118E-02
5.0000
118_030
102.2811
121.22
8.733E-02
5.881E-02
l.e34E-02
1.482E-02
3. 1 IllE - 02
Il.0000
81 . U5
115.882
1011.88
7.172E-02
5.534E-02
1.24.E-02
1.487E-02
2.73eE-02
7.0000
85.241
12 •. 488
85.74
Il.020E-02
5.174E-02
8.828E-03
1.452E-02
2.435E-02
Nil V
IIP
EO'
1.4252E+00 (AYO)
N··
4.1882
MU'
1.8118
E UYO)
E (EV)
E PHOT
(EV)
LAMIIOA
(A)
(L/A/L-I)
(L/R/L+ 1)
SIGMA L-l
SIGMA
L+l
SIGMA
(Mil)
.0000
.000
18.381
113•. 38
8.42IE-Ol
-2.575E-Ol
2.885E-Ol
5. 38U -02
3.424E-Ol
.4000
5.442
24.834
41111.27
5.1134E-Ol
-8.210E-02
1.1151E-Ol
8.825E-03
1.73I1E-Ol
.11000
8.1'14
27.555
4411.1111
4.758E-Ol
-4 .1I0U - 02
1.30IlE-Ol
2.78lE-03
1.334E-Ol
.8000
10.885
30.2711
408.52
4.083E-Ol
- 1 .•9E-02
1.057E-Ol
4.885E-04
1.0112E-Ol
1.0000
13.11011
32.11117
375.75
3.550E-Ol
•. 287E-04
8.711 E-02
1.1112E-OII
8.711 E-02
2.0000
27.212
411.1103
21111.05
2.030E-Ol
4.2110E-02
4.021E-02
3.5114E-03
4.380E-02
3.0000
40.818
110.20.
205.113
1.343E-Ol
5.00IlE-02
2.273E-02
e.32I1E-03
2.1I0IlE-02
4.0000
54.424
73.815
1117.117
Il.e77E-02
4.1I02E-02
1.448E-02
7.431E-03
2. 1111 E- 02
5.0000
'18.030
87.421
141.83
7.37U-02
4.581E-02
8.8117E-03
7.118I1E-03
1.711!lE-02
'1.0000
81.1135
101.027
122.73
5.8!l3E-02
4.222E-02
7.250E-03
7.544E-03
1.478E-02
25
NB V
8P
10· 8.48271-01
(RYD)
N'"
8.2100
MU·
1.7800
1 (RYD)
1 (IV)
1 PHOT (IV)
LAMBDA (A)
(L/R/L-l)
(L/R/L+1 )
SigMA
L-l
SigMA
L+l
SlaMA
(MB)
.0000
.000
8.820
1405.88
1.8081+00
-7.81l71-01
8.0481 -0 1
2.1881-01
8.2121-01
.2000
2.721
11.1l42
1074.28
1.11l81+00
-3.71l11-01
3.2481-01
8.8031-02
3.8301-01
.8000
8.1a4
18.8'4
730.02
8.111l1-01
-1.0481-01
1.3301-01
7.8211-03
1.4081-01
.8000
10.8all
18.705
828.21
4.78U-Ol
-5.2331-02
8.4381-02
2.2801-03
8.8821-02
1.0000
13.a08
22.428
1552.'8
3.8801-01
-2.07U-02
8.9981-02
4.0301-04
7.0381-02
2.0000
27.212
38.032
344.10
1.7841-01
2.11541-02
2.31l01-02
1.3171-03
2.4811-02
3.0000
40.81'
411.838
248.7'
1. 0431-01
3.4781-02
1.1301-02
2.511l1-03
1.3821-02
4.0000
1l4.424
83.244
1118.04
7.0181-02
3.2841-02
8.521l1-03
2.8741-03
8.38'1-03
5.0000
88.030
78.850
181 .34
5.1121-02
2.118U-02
4.2081-03
2.8801-03
7.087E-03
8.0000
81. 831l
80.4.8
137.07
3.11251-02
2.8851-02
2.11181-03
2.752E-03
5.87U-03
NB V
10P
10· 3.70251-01
(RYD)
N··
8.2172
MU·
1.7828
1
( RYD)
1 (IV)
1 PHOT (EV)
LAMBDA
(Al
(L/R/L-ll
(L/R/L+I)
SlaMA L-l
siaMA L+l
SigMA
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.0000
.000
Il. 038
2481.22
3.102E+00
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1.0151+00
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1.3481 -02
8.2871-04
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7.8881-02
2.525E-02
5.11741-03
1.2241-03
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4.0000
54.424
58.481
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5.1451-02
2.3481-02
3.21171-03
1.3741-03
4.871E-03
5.0000
88.030
73.087
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2.1031-02
2.0851-03
1.3541-03
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4.28111-04
3.287E-02
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8.38lE-03
2.148E-02
2.787E-02
2.0000
27.212
28.770
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4.888E-02
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1.589E-03
1.223E-03
2.812E-03
3.0000
40.818
42.378
282.18
2.540E-02
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8.873E-0.
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8.988E-04
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54.424
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221.48
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8.218E-03
3. 78llE-04
8.182E-05
4.581E-0.
5.0000
88.030
118.587
178.17
1. 180E -02
Il.115E-03
2.353E-04
2.180E-04
4.533E-0.
7.0000
85.241
118.788
128.08
8.888E-03
Il.7112E-03
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4.848E-04
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108.8.7
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112.30
5.585E-03
8.372E-03
8.5l13E-05
3.1187E-04
4.518E-04
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122.453
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3.842E-04
4.307E-04
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4.831E-03
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5.1l44E-05
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88.188
138.01
1.2I5U-Ol
3.8321-02
3.552E-02
5.1118E-03
4.072E-02
2.0000
27.212
15.882
1211. 18
1.1211E-Ol
8.480E-02
3.058E-02
1.525E-02
4.1580E-02
8.0000
81.835
150.418
82.43
5.1123E-02
1.123E-Ol
1.1851-02
7.1151E-02
8.348E-02
7.0000
85.241
184.022
75.58
4.808E-02
1.0118E-Ol
8.825E-03
7.427E-02
8.420E-02
8.0000
108.847
177.1128
88.80
4.324E-02
1.0158E-Ol
8.348E-03
7.483E-02
8.287E-02
8.0000
122.4153
181.234
84.83
3.844E-02
1.00U-Ol
7.101 E-03
7. 33l1E -02
8.04U-02
31
MO VI
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2.04180E+00
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3.71112
MU·
1.2038
E (RYD)
E (EV)
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LAMBDA
(A)
(L/R/L-1)
(L/R/L+I)
SIGMA
L-l
SIGMA
L+l
SIGMA
(MB)
.0000
.000
33.888
11104 . 71
3.28I1E-Ol
-04.3111E-Ol
9.22I1E-02
2.0437E-OI
3.15IE-Ol
.11000
8. 11104
042. 152
2104.104
2.30404E-Ol
-1.18I1E-Ol
5.8204E-02
Il.288E-02
1. 20lE -0 1
1.0000
13.808
047.lll04
280.51
1.119E-Ol
-1.018E-Ol
04.0417E-02
2.182E-02
8.8llIE-02
1.5000
20.0401
ll04.387
227.13
l.ll73E-Ol
-3.lll04E-02
3.38llE-02
3.207E-03
3.708E-02
2.0000
27.212
81.200
202.51
1.30IE-Ol
3.8I5llE-03
2.83llE-"2
3.042IE-Oll
2.838E-02
2.5000
304.01ll
88.001
182.33
1. 110E-Ol
3.127E-02
2.10llE-02
2.ll08E-03
2.358E-02
04.0000
504.04204
88.0412
1040.204
7.3ll2E-02
8.87llE-02
1.201E-02
1.048llE-02
2.888E-02
ll.OOOO
88.030
102.018
121.53
5.888E-02
7.21IE-02
8.82ll~-03
2.004IE-02
2.131E-02
7.0000
115.2041
128.UI
115.104
04.02IE-02
7.110E-02
ll.273E-03
2.lllIE-02
3.0048E-02
8.0000
108.8047
1042.8311
88.80
3.0432E-02
8.8804E-02
04.230E-03
2.1552E-02
2.1175E·02
1.0000
122.04ll1
1158.04'"
71.115
2.1804E-02
8.ll28E-02
3.04158E-03
2.ll13E-02
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3.578E-Ol
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8.ll204E-02
1.8504E-Ol
2.707E-Ol
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10.8815
31.113
388.27
2.8155E-Ol
-2.317E-Ol
5.880E-02
8.llIE-02
1.258E-Ol
1.0000
13.808
304.8ll04
3ll7.78
2.331E·01
-1.779E-Ol
4.733E-02
04.137E-02
8.870E-02
l.ll000
20.040.
041.04ll7
281.07
1.7ll3E-Ol
-7.78IE-02
3.201E-02
1.04304E-03
04.10404E-02
2.0000
27.212
048.280
258.11
1.377E-Ol
-2. 180E-02
2.21IE-02
8.8047E-004
2.385E-02
2.ll000
304.011
5ll.083
22ll.17
1.118E-Ol
1. 087E -02
1.7204E-02
2.04152E-004
1.7"IE-02
3.0000
040.818
81 . 888
200.041
9.275E-02
3.0048E-02
1.338E-02
2.187E-03
1.155"E-02
04.0000
504.04204
715.472
1804.28
Il.758E-02
4.148E-02
8.885E-03
8.182E-03
1.583E-02
15.0000
88.030
81.078
131.11
ll .• 87E-02
ll.588E-02
8.025E-OI
1.0..1 E-02
1.8043E-02
7.0000
15.241
118.210
108.82
3.382E-02
5. 0488E -02
3.3043E-03
1.320E-02
1. 855E -02
8.0000
108.8047
121.818
Ill. 45
2.828E-02
5.228i-02
2.813E-03
1.33IE-02
1 .800E -02
1.0000
122.453
1043.502
88.040
2.407E-02
04.130E-02
2.010E-03
1.31I5E-02
1. ll204E-02
MO VI
80
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7.8885E-Ol
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8.8423
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LAMBDA
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(L/R/L·I)
IL/R/L+l)
SI GlU
L-l
SIGMA
L+l
SIGMA
1MB)
.0000
.000
10.482
1185.08
1. OOI5E -00
-1.713E+00
2.815I5E-Ol
1.15IE+00
1.0423E+00
.2000
2.721
13.183
840.047
0.817E-Ol
- 1 .0504E+00
1.578E-OI
5.125E-Ol
7.102E-Ol
.8000
8.184
18.828
885.87
3.138E-Ol
-04.7040E-Ol
7.281E-02
1.1578E-Ol
2.3004E-Ol
.8000
10.885
21.3047
580.81
3.158E-Ol
-3.330E-Ol
5.352E-02
8.1204E-02
1.0428E-Ol
1.0000
13.808
204.088
ll15. III
2.1I01E-Ol
-2.375E-Ol
04.0104E-02
ll.118E-02
1.212E-02
2.0000
27.212
37.8704
321.10
1.2112E-Ol
-3.81IE-02
1.501E-02
2.070E-03
1.715E-02
2.15000
304.015
0404.0477
278.78
9. 85llE -02
-04.30IlE-03
1.042E-02
3.1ITE-Oll
1.04llE-02
3.0000
040.818
s r , 280
2041.78
7.8704E-02
i . 438E -02
7.512E-03
3.118E-04
7.111E-03
04.0000
504.04204
804.888
111.08
5.250E-02
3.1104E-02
04.0415E-OI
2.373E-03
8.888E-03
7.0000
115.2041
1015.7004
117 .30
2.383E-02
3.llI57E-02
1.50IE-OS
15. 042E -03
8.551E-03
8.0000
108.8047
1111.310
101.12
1.lIllTE-02
3.388E-02
1.104IE-OS
ll.102E-03
Il.2llIE-03
1.0000
122.04153
132.11S
13.28
1 .8041 E-02
3.11571-02
8.1131-04
04.11151-03
5.II"E-03
MO VI
100
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(RYD)
N"· 8.8488
MU·
1.1512
E (RYD)
E (EV)
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LAMBDA
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(L/R/L-l)
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SIGMA
L-l
SIGMA
L+l
SIGMA
1MB)
.0000
.000
0.255
1882.0e
1 . 8204E +00
-2.878E+00
04.1471-01
1.1504&+00
2.38IE+00
.2000
2.721
8.177
1381.22
8.1118E-Ol
-1.0433E+00
1.827E-Ol
0.1045E-Ol
8.772E-Ol
.8000
8. 1804
104.0411
851.88
04.151E-Ol
-ll.2048E-Ol
8.288E-02
1.04II1E-01
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.8000
10.885
17.140
723.37
3.1040E-Ol
-3.0487E-Ol
04.2047E-02
7.85IE-02
1.2IIE-Ol
1.0000
13.808
111.881
8204.28
2.0471E-Ol
-2.3UE-Ol
3.048E-02
04.28'E-02
7.338E-02
1.5000
20.0401
28.8804
04804 .111
1.531 E -01
-1.883E-02
1.572E-02
1.77IE-03
2. 550E-02
2.0000
27.212
33.0487
370.047
1.05IE-Ol
-3.778E-02
1.04304E-03
I.801E-03
I.123E-02
2.5000
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040.270
307.11
7.843E-02
-7. 78IE-03
8.227& -03
1.210E-Oll
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8.31IE-03
3.0000
047.073
283.31
8.088E-02
8.1204E-03
04.388E-03
1.171E-004
04.503E-03
04.0000
504.0424
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204.33
04. 033E -02
2. 178E-02
2.481E-OI
1. 0804E -03
3.584E-03
7.0000
1!5.2041
101.0417
122.18
1.7047E-02
2.ll1I1E-02
7.711E-04
2.0428E-03
3.207E-03
8.0000
108.'047
Illl. 103
107.72
1.04231-02
2.3781-02
5.8581-04
2.04531-03
3.03IE-03
1.0000
122.4153
128.701
18.33
1. 1.I5E -02
2.2221 -02
04.5043E-04
2.387E-03
2.8151E-03
MO VI
120
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N"· 10.8520
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1.1480
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LAM8DA (Al
IL/R/L-l)
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SIGMA
L-l
SIGMA
L+l
SIGMA
(MB)
.0000
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04 . 1511
2180.1111
2.3804E+00
-04.277E+00
ll.8042E-Ol
2.888E+00
3.0453E+00
.2000
2.721
8.880
1802.02
1.037E+00
- 1 .8851 +00
1.85111-01
7.382E-Ol
1.222E-Ol
.04000
5.04042
Il.802
1211.31
8.018E-Ol
-8.738E-Ol
8.704041-02
2.783E-Ol
3.8371-01
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10.8'5
15.0404
8204.18
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B.15TE-02
1.3211-02
1.0000
13.80e
17.781S
887.12
2.208E-Ol
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2.1781-02
3.235E-02
15.0413E-02
1 .5000
20.0408
204.1588
5004.88
1.3021-01
-8.7301 -02
1.0048E-02
7.080E-03
1 .7504 E -02
2.0000
27.212
31.371
315.23
8.7"IIE-02
-3.3150E-02
0.0381-03
1.328E-03
7.383E-03
2.5000
304.0 III
38.1704
324.71
Il. 357E -02
-7. lUI -03
3.877E-03
Il.177E-05
3.181E-03
3.0000
040.818
404.177
275.87
04.888&-02
ll.213E-03
2.87IE-03
04.801E-Oll
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04.0000
154.04204
58.583
211 .804
3.1571-02
1.828E-02
1.0477E-03
5.837E-004
2.0801-03
5.0000
88.0S0
72. 181
171.75
2.25041-02
1.134E-02
1.220E-004
1.018E-03
1.10401-03
7.0000
15.2041
Il.0401
1204.73
1.338E-02
1.81ISE-02
04.04704E-04
1.3045E-03
1.713E-03
8.0000
108.847
113.007
101.72
1.084E-02
1.7851 -02
1.341 E-04
1. 358E - 03
1."2E-03
1.0000
122.0453
128.812
17.13
1.000E-03
1.888E-02
2.578E-04
1.3215E-03
I.583E-03
32
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1.l!l31"E·01
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1 . 1"52
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LAUDA
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SIGMA L-I
SIGMA L+I
SIQIIiIA
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.0000
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2.220
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8.872E-03
1.207E-02
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1.281E-03
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7.712E-02
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34
TC VII
55
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115
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105
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TC VII
125
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211.221
424.30
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112.828
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27.212
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1.818E-Ol
7.822E-02
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8.711I1E-OI
1.713E-02
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217.711
1.218E-Ol
8.842E-02
1.71l0E-02
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2.874E-02
TC VII
80
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1.011511
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8.72111-01
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55".75
3.823E-Ol
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8. 138E-02
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13.808
27.5113
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2.888E-Ol
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1.811I1E-02
8.828E-02
1.5000
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380.~7
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2.1821-03
3.11181-02
2.0000
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300.115
1.3801-01
1 .511~1-03
1.1173E-02
3.1I~81-08
1.173E-02
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115.822
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3.~58E-02
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2.8701-03
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7.0000
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1.51I1E-Ol
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22.002
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2.112111-03
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1. 287E -03
Il.208E-02
Il.333E-02
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lOF
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RU VIII
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27.212
211.7.·7
418.81
Il. 177E-02
3. IIIIIE -02
5.2"7E-03
1 . 27!IE-03
8.522E-03
3.0000
40.818
"3.353
285.1111
".855E-02
2.312E-02
2. , .. 0E - 03
Il.708E-0''
3. 111 E-03
RU VIII
40
EO·
8. 1780E+00 CAYO)
N··
2.71175
MU'
1.2025
E CRYD)
E (EVI
E PHOT CEV)
LAM8DA (A)
CL/R/L-l1
(L/R/L+ 1 )
SIGMA L- 1
SlaMA L+I
SIGMA (M8)
.0000
.000
111.2811
111."3
1.185E-Ol
Il. 032E -02
3.7118E-02
3.422E-02
7.220E-02
1.0000
13.808
12".875
1111 . 211
Il.71eE-02
1.113E-Ol
2.1183E-02
5.828E-02
8.7111E-02
4.0000
54.42"
185."3
7".83
8.200E-02
1.218E-Ol
1.80IE-02
Il.245E-02
1.085E-Ol
5.0000
88.030
1711. Utl
111.15
5."83E-02
1.18"E-Ol
1 . 3"SE -02
Il.483E-02
1. 083E-Ol
8.0000
81.83S
112.11011
&4.27
".81581-02
1.141 E-O 1
1 . 143E -02
Il.474E-02
1.082E-01
7.0000
111.2.'
208.511
80.0"
".3.IIE-02
1.01131-01
Il.818E-03
Il.301E-02
1.028E-Ol
RU VIII
50
EO' •. 1810E+00 {AYD)
N··
3.11125
MU'
1.0875
E CRYD)
E (EV)
E PHOT CEV)
LAMIDA CA)
(L/R/l-l )
(L/R/L+l)
SIGMA L-I
SIGMA L+l
SIGMA CMB)
.0000
.000
58.888
217.'8
2.130E-Ol
-1.103E-02
8."1I0E-02
2.81lE-0"
8.518E-02
.0800
.818
57.702
21".87
2.0821-01
- ... a02E -03
8.2a7E-02
5.017E-05
8.2112E-02
.1000
1.311
58.247
212 .88
2.051 E-01
-8.457E-0"
8.158E-02
1.57IE-08
8.157E-02
.2000
2.721
51.807
208.01
1.1I15E-Ol
8.401E-03
5.847E-02
1.588E-0"
5.883E-02
.4000
S."42
82.328
1118.112
1.8381-01
2."43l-02
5.2t12E-02
1 ... 03E -03
Il.432E-02
1.0000
13.808
70.4t12
175.811
1.508E-Ol
5.778l-02
".0201-02
8.888E-03
... 1I07E- 02
2.0000
27.212
8".0118
'''7.43
1.132E-Ol
8."271-02
2. 701lE- 02
2.252E-02
".1I81E-02
5.0000
".030
124.1115
111.28
5.IIS1E-02
Il.203E-02
1.112E-02
3.118I1E-02
5.IOlE-02
8.0000
81.835
138.521
8t1.51
5.028E-02
8.800E-02
8.711"E-03
4.0"'E-02
".1I2"E-02
7.0000
115.2'"
152.127
81.50
4.30IlE-02
8.333E-02
7.10tE-03
3.883E-02
".8113E-02
RU VIII
80
la' 2.82211+00 (RYD)
N.· ".1405
MU-
1.05115
E CAYO)
E CIV)
E PHOT CIV)
LAMIDA CA)
CL/R/L-Il
CL/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (Mil
.0000
.000
35.878
3 .. 7.5..
3.3110E-Ol
-1.302E-Ol
1.030E-Ol
2.27I1E-02
1.258E-Ol
.0800
.818
38."112
3311.78
3.288E-Ol
-1.151E-Ol
Il. 785E-02
1.822E-02
1.18lE-Ol
.3000
4.082
311.757
311.88
2.837E-Ol
-8.537E-02
8.0"8E-02
8."05E-03
8.888E-02
.8000
8.18"
43.8311
282.82
2."'7E-0'
-2.117E-02
8.437E-02
7 ... 08E -04
8.511 E-02
.8000
10.885
48.580
288.211
2.1l10E-Ol
5.048E-0"
5.811 E-02
•. 470E-07
5.811E-02
1.0000
13.808
411.281
251.1511
1.11115E-Ol
1.783E-02
4.112I1E-02
5. 778E-0"
".1I88E-02
2.0000
27.212
82.887
1117.18
1.337E-Ol
8.211I1E-02
2.82!IE-02
Il ... 08& -03
3.785E-02
3.0000
40.818
78."113
182.01
tI.887E-02
7.87BE-02
1.80"E-02
1 . 700E-02
3.50"E-02
5.0000
88.030
103.705
1111.58
5.888E-02
7.880E-02
8.888E-03
2.308E-02
3.203E-02
8.0000
81.835
117.311
1015.811
•. 784E-02
7.28tE-02
8.7"8E-03
2.345E-02
3.020E-02
7.0000
115.2'"
130.1117
114.71
3.1188E-02
8.827E-02
5.233E-03
2.301E-02
2.8:UE-02
311
RU VIII
8D
EO'
1.3215E+00 (RYD)
N·· 8.115112
MU'
1.0408
E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA
( A)
(L/R/L-1)
(L/R/L+I)
SICMA L-l
SICMA L+l
SICMA 1MB)
.0000
.000
17.1180
15811.57
8.887E-Ol
-4.585E-Ol
2. 02 lE -0 1
1.413E-Ol
3.434E-Ol
.1000
1.381
111.341
841.08
5.1125E-Ol
-3.888E-Ol
1.707E-Ol
9.1I08E-02
2.898E-Ol
.8000
8.184
28.144
474.25
3.5115E-Ol
-1.255E-Ol
8.492E-02
1. 552E -02
1.004E-Ol
.8000
10.885
28.885
4211.54
3.050E-Ol
-7.857E-02
8.751E-02
8.381E-03
7.38I1E-02
1.0000
13.'08
31.588
312.53
2.827E-Ol
-4. 153E-02
5.478E-02
2.054E-03
5.883E-02
1.5000
20.4011
38.3811
322.117
1.1I00E-01
1.054E-02
3.483E-02
1.8011-04
3.500E-02
2.0000
27.212
45.112
274.35
1.44111-01
3. 583E -02
2.3"'E-02
2.188E-03
2.803E-02
4.0000
54.424
72.404
171.24
8.808E-02
5.728E-02
7.1147E-03
8.11117E-03
1.8110E-02
5.0000
88.030
88.010
144.15
4.1157E-02
5.528E-02
5.31lE-03
Il.1I04E-03
1.522E-02
8.0000
81.835
1111.818
124.48
3.877E-02
5.172(-02
3. 784E -03
1.005E-02
1.38lE-02
7.0000
118.241
113.222
1011.51
3. 1211E-02
4.785E-02
2.785E-03
9.774E-03
1.2seE-02
RU VI I l
10D
10- 7.11814E-Ol
(RYD)
N··
8.118511
MU'
1,0341
E (RYD)
1
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LAM8DA CA)
(L/R/L-l)
(L/R/L+I)
SICMA L- 1
SIGMA L+l
SICMA (MB)
.0000
.000
10.832
1144.80
1.01131+00
-8.1170E-Ol
3.253E-Ol
3.288E-Ol
8.53I1E-Ol
.8000
8.184
18.118
852.70
4.2117E-Ol
-1.1188E-Ol
8."71-02
2.773E-02
1.15I1E-Ol
.900q
!:l.U5
23.078
537.28
3.108E-Ol
-9.503E-02
5.8041-02
7.8S81E-03
8.3110E-02
1.0000
13.808
24.438
507.35
2.825E-Ol
-7.211E-02
4.11041-02
4.8118E-03
5.3113E-02
1.5000
20.4011
31.241
318.87
1.878E-Ol
-7.075E-03
2.784E-02
5. 81I8E-05
2.770E-02
2.0000
27.212
38.044
325.10
1.350E-Ol
2.140E-02
1.744E-02
8.B88E-0"
1 . 801E-02
2.5000
34.015
44.847
278.48
1.02BE-Ol
3.448E-02
1.1881-02
2.008E-03
1.387E-02
3.0000
40.818
51.850
240.05
8.018E-02
4.0351-02
8.515E-0~
3.17lE-03
1.18I1E-02
5.0000
88.030
78.882
157.22
3.1183E-02
4.133E-02
3. 1411E-03
5.080E-03
8.22I1E-03
8.0000
81 .835
112.488
134.01
3.0481-02
3.838E-02
2.180E-03
5.13llE-03
7.2115E-03
7.0000
115.241
108.074
118.81
2.411E-02
3.524E-02
1.58lE-03
4 .1I87E -03
8.528E-03
RU VI l 1
12D
EO'
5.3111E-Ol
IRYD)
N.' 10.118111
MU-
1.0301
E (RYD)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/R/L-l )
(L/R/L+I)
SIQMA L-l
SIGMA L-l
SIQMA (M8)
.0000
.000
7.237
1713.21
1.805E+00
-1.445E+00
4.888E-Ol
5.700E-Ol
1.031E+00
.8000
8.184
1!I.401
805.07
4.573E-Ol
-2.3501-01
8.01181-02
3. 20.E -02
1,130E-Ol
1.0000
13.808
20.843
5114.88
2.7821-01
-8.515E-02
3.11181-02
5.811BE-03
4.1188E-02
1.5000
20.4011
27 .... 8
4"8.48
1.723E-Ol
-1.480E-02
2.084E-02
2.1.12E-04
2.085E-02
2.0000
27.212
34.4"11
351.11
1.1I13E-Ol
1.383E-02
1. 2321E-02
2.414E-04
1.258E-02
2.5000
34.015
-e 1 . 252
300.58
8.818E-02
2.587E-02
8.0831E-03
1.04lE-03
Il.104E-03
5.0000
88.030
75.287
184.73
3.211E-02
3.20BE-02
1.150E-03
2,121E-03
4.871E-03
8.0000
81.835
88.873
131.51
2.427E-02
2.185E-02
1.3181-03
2.1451 -03
4.281 E-03
7.0000
15.241
102.478
120.11
1.IIOIE-02
2.710E-02
9.383E-04
2. 838E -03
3.77BE-03
RU VII 1
18D
EO.
2.855lE-Ol
(RYD)
N.· 14.11721
MU-
1.0279
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
lA 1
(L/R/L-l)
(L/R/L+I)
SICMA L-l
SIGMA L+l
SIGMA tMB)
.0000
.000
3.885
31111.77
2.87IE+00
-2.8481+00
8.013E-Ol
1.188E+00
1.117E+00
.0200
.272
4.157
21182.82
2.5731+00
-2.417E+00
8.915E-Ol
9.775E-Ol
1.88IE+00
.2000
2.721
8.108
1878.15
1.1112E+00
-9.824E-Ol
2.358E-Ol
2.404E-Ol
4.781E-Ol
.8000
8.184
12.048
10211.011
4.38U-Ol
-2.485E-Ol
5.822E-02
2.804E-02
8.828E-02
1.0000
13.808
17.4110
708.88
2.354E-Ol
-8.35IE-02
2.437E-02
4.808E-03
2.818E-02
1 .5000
20.4011
24.213
510.37
1 . 3511E- 0 1
-1.727E-02
1.128E-02
2.73lE-04
1.185E-02
2.0000
27.212
31.088
3118.72
8.988E-02
8.8071-03
8.312E-03
5. 118E -08
8.383E-03
2.5000
34.015
37.8111
327.15
8.447E-02
1..8371-02
3.115IE-03
3.831E-04
4.342E-03
4.0000
54.424
58.308
212.84
3.123E-02
2.218E-02
1.42111-03
1.081 E-03
2.511 E-03
5.0000
8'.030
71.11,.
172.41
2.1I12E-02
2. 112 E-02
8.888E-04
1.210E-03
2.078E-03
8.0000
81.835
BIl.520
144.118
1.838E-02
1.142E-02
5.7581-04
1.218E-03
1.7112E-03
7.0000
115.241
Il.128
125.08
1.27llE-02
1 . 787E -02
".049E-04
1,187E-03
1.572E-03
RU VIII
20D
EO'
1.7778E-Ol
IRYD)
N.' 18.1734
MU'
1.0288
E (RYD)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/R/L-l)
(L/R/L+l)
SIGMA L -1
SIGMA L-l
SIQMA (M8)
.0000
.000
2.411
5125.72
4.487E+00
-4.838E+00
1.213E+00
1.882E+00
3.175E+00
.0200
.272
2.891
4807."0
3.7"21+00
-3.805E+00
9.4701-01
1.4881+00
2.4181+00
.0800
.818
3.235
3832.34
2.7581+00
-2.81131+00
8.175E-Ol
8.8451-01
1 .1502E +00
.2000
2.721
5.140
2412.14
1.2771+00
-1.01151+00
2.1 OBI -01
2.3221-01
4.4301-01
.8000
8.184
10.1582
1171.12
3. 843E -01
-2.2871-01
3.12B1-02
2.051E-02
5.180E-02
1.0000
13.808
18.025
773.71
1.11231-01
-7.218E-02
1.48I1E-02
3.148E-03
1.804E-02
1.5000
20.401
22.828
543.14
1.0841-01
-1.548E-02
8."1I3E-03
2. 08U -04
8.'001-03
2.0000
27.212
211.831
418.44
8. 88BE -02
3 .842E -03
3.5131-03
1. 8150E-05
3.830E-03
2.8000
34. OUI
38.434
340.31
4.853E-02
1.1501-02
2.1571-03
1.81IlE-04
2.33I1E-03
4.0000
54.424
5'.843
218.12
2.284E-02
1.5131-02
7.81BE-04
5.437E-04
1.2851-03
5.0000
8'.030
70."48
178.00
1.5117E-02
1.514E-02
4.518E-04
8. 0811E-04
1.081 E-03
8.0000
81.835
84.054
147.51
1 . 188E -02
1.388E-02
2.11871-04
8.1071-04
Il.075E-04
7.0000
118.241
17.880
128.118
Il. 1114E -03
r , 28lE -02
2.0'BE-04
5.852E-04
7.11271-04
RU VII 1
4F
10' 4.8272E+00 (RYD)
N.·
3.8412
MU'
.3588
1
(RYD)
E (EV 1
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LAMIDA (A)
CL/R/L-1)
(L/R/L+ 1 )
SIQMA L-l
SIQIlIA L+l
SIQMA (MI)
.0000
.000
88.8'11
188.78
8.174E-02
8.527E-Ol
8.742E-03
1.008E+00
1.012E+00
.8000
8.803
72.482
171.08
5.311I1E-02
5.448E-Ol
5.1811-03
7.728E-Ol
7.78!1E-01
1.0000
13.808
'11.285
158.38
4.7701-02
4.8131-01
4.8158E-03
8.01lIlE-Ol
8.108E-Ol
8.0000
81.835
147.314
84.18
1.8801-02
1.3'71-01
1.417E-03
1.0181-01
1.0321-01
RU VIII
5F
10' 2.17821+00 IRYD)
N·· 4.83411
MU-
.3851
1
(RYD)
1
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1 PHOT (IV)
LAMBDA (A)
(L/R/L-l)
(L/R/L+l )
SIGMA L -1
SIOMA L-l
SIOMA (MB)
.0000
.000
40.535
305.87
1.1741-01
8.11381-01
1.5041 -02
1.183E+00
1.1781+00
.5000
8.803
47.338
281.12
Il.3411-02
7.028E-01
1.1121-02
8.31151-01
8.507E-Ol
1.0000
13.808
54.141
221.01
7.81151-02
5.8871-01
8.5451-03
8.243E-Ol
8.3211-01
4.0000
54.424
114 .11511
130.57
3.23U-02
2.18lE-Ol
2. 877E -03
1.51121-01
1.81111-01
8.0000
81. 835
122.171
101.411
2.1 5lE -02
1.3811-01
1.5231-03
8.12'E-02
8.2781-02
40
RU V III
8F
10' 2.011171+00 (RYOt
N.· 5.82112
MU·
.3708
E (no )
E (EV)
E PHOT (IV)
LAllIIIOA
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(L/R/L-l)
(L/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA (MS)
.0000
.000
27.4aO
451.111
1.874E-Ol
1.128E+00
2.800E-02
1.255E+00
1.281E+00
.5000
8.a03
34.283
381.88
1.33I1E-Ol
8.2431-01
1.es8E-02
8.38SE-Ol
8.53lE-Ol
1.0000
13.808
41.0a8
301.77
1.015E-Ol
8.28H-Ol
1. 141 E-02
5.851E-Ol
Il.'8SE-Ol
2.0000
27.212
54.812
228.70
8.524E-02
4.02H-Ol
8.289E-03
3.185E-Ol
3.248E-Ol
8.0000
81.835
109.115
113.53
2.140E-02
1.23l1E-Ol
1 . 348E -03
8.015E-02
8.150E-02
RU VIII
8F
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1.1011 E+OO (RYO)
N.· 7.8239
MU·
.3781
E (RYO)
E (EV)
E PHOT (IV)
LAM8DA
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(L/R/L-l)
(L/R/L+l)
SIOMA L-l
SIOMA L+l
SICMA (MB)
.0000
.000
14.982
827.5'
3.1192E-Ol
1.591E+00
S.20H-02
1.382E+00
1.414E+00
.5000
8.a03
21.785
589.15
2.012E-Ol
9.744E-Ol
2.3751-02
7.427E-Ol
7.885E-Ol
1.0000
13.808
28.587
433.71
1.318E-Ol
8.889E-Ol
1.337E-02
4.51151-01
4.8"E-Ol
2.0000
27.212
42.193
2'3.85
7.130E-02
3.747E-Ol
!1. 777E-03
2.127E-Ol
2.185E-Ol
4.0000
54.424
89.405
178.~
3.183E-02
1.894E-Ol
1.894E-03
7.154E-02
7.343E-02
8.0000
81.8all
98.817
128.33
1.UlIE-02
9.849E-02
8.700E-04
3.230E-0.2
3.317E-02
RU V Il)
lOF
EO. 8.9133E-Ol (RYOI
N·· 9.8218
MU·
.3784
E (RYOI
E (EV 1
E PHOT (EV)
LAM80A lA)
(L/R/L-l)
(L/R/L+l)
SIGMA L- 1
SICMA L-l
SlaMA. (M8)
.0000
.000
Il.408
1318.14
Il.834E-OI
2.083E+00
8.040E-02
1.437E+00
1.518E+00
.5000
8.803
18.209
784.112
2.42U-Ol
1.030E+00
2.55'E-02
8.178E-Ol
8.432E-Ol
1.0000
13.808
23.012
53a.79
1.401E-Ol
8.382E-Ol
1.21 8E -02
3.3851-01
3.4871-01
2.0000
27.212
38.818
338.119
8.70lE-02
3.25IE-Ol
4. 42l1E -03
1.390E-Ol
1.43.E-Ol
4.0000
114.424
83.830
194.25
2.708E-02
1.381E-Ol
1.258E-03
4.247E-02
4.3731-02
8.0000
81. 835
91. 042
1311. 111
1.48SE-02
7.504E-02
5.418E-04
l.84U-02
1. 8915E-02
RU V[II
12F
EO·
4.731151-01
(llYO)
N.· 11.8204
MU·
.3798
E (no )
E (IV)
1 PHOT (IV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l )
SIOMA L- 1
SIGMA L+l
SlaMA
(M8)
.0000
.000
8.449
1922.70
7.UU-Ol
2.550E+00
1. OS3E-Ol
1.5011+00
1.81I5E+00
.5000
8.803
13.252
835.84
2.598E-Ol
1.0241+00
2.410E-02
4.1I10E-Ol
Il.231E-Ol
1.0000
13.808
20.0&4
818.25
1.380E-Ol
5. 8·37E-0 1
9.992E-03
2.454E-Ol
2.55.1-01
2.0000
27.212
33.880
388.34
5.970E-02
2.770E-Ol
3.23lE-03
9.278E-02
Il. 59ln -02
4.0000
54.424
80.872
203.88
2.283E-02
1.104E-Ol
8.393E-04
2.8821i-02
2.748E-02
RU VIII
18F
EO·
2.82331-01
(llYOI
N·· 15.8183
MU'
.3807
E (RYOI
(EV)
E PHOT (EVI
LAM80A (Al
(L/ll/L-11
IL/R/L+I)
SIGMA L- 1
SICMA L+l
SIGMA (M8)
.0000
.000
3.589
3473.88
1.31I1E+00
3.5751+00
1.884E-Ol
1.838E+00
1.80151-00
.5000
8.803
10.372
, 195.38
2.538E-Ol
9.230E-Ol
1.800E-02
3.173E-Ol
3.353E-Ol
1.0000
13.808
17.175
721.811
1.158E-Ol
4.885E-Ol
8.181 E-03
1 . 3.,2E -0 1
1.4041-01
2.0000
27.212
30.781
402.80
4.587E-02
2.028E-Ol
1.7211-03
4.53I5E-02
4.70n-02
4.0000
54.424
57.1113
213.80
1.814E-02
7.830E-02
4.087E-04
1.212E-02
1.2531-02
8.0000
81.B35
85.205
145.52
8.399E-03
4.0411-02
1.819E-04
4.997E-03
5.15IE-03
RU VIII
20F
EO'
1.8112al-Ol
(RYO)
N·· 19.8188
MU·
.3812
E (llYO)
E (IV)
E PHOT (EV)
LAMBDA
(A)
(L/ll/L-1)
(L/ll/L+11
SIGMA L-l
SIGMA L- 1
SIGMA (MB)
.0000
.000
2.282
5480.311
1.9091+00
4.872E·+00
2.22lE-Ol
1.7731+00
1.'1151-00
.2000
2.721
4.984
2487.111
5. S73E-Ol
1.7291+00
4.3201-02
5.3511-01
5.7831i-Ol
.8000
8.184
10.428
11811.21
1.8221i-01
Il.511t1-01
9.320E-03
1.818E-Ol
1.70IE-Ol
1.0000
13.808
15.888
781.35
9.48U-02
3.709E-Ol
3.8251-03
7.137E-02
8.2201-02
2.0000
27.212
29.474
420.88
3.530E-02
1.5331-01
9.8113E-04
2.488E-02
2.588E-02
4.0000
54.424
58.888
218.72
1.2041-02
5.813E-02
2.215E-0.
8.414E-03
8.835E-03
8.0000
81.835
83.898
147. T'
8.1831-03
2.943E-02
8.83U-05
2.80IE-03
2.8151-03
41
RH IX
ilS
EO' 7.25117E+00
(RYD)
No'
3.3403
MU'
1 . 115117
E IRYD.
E 1 EV)
E PHOT (EV'
LAMIIDA
lA)
(L/R/L-I)
lL/R/L+ 1)
SIGMA L-l
SIOMA L+l
SlaMA
(MI)
.0000
.000
118.775
1211.112
.000
1.437E-Ol
.000
1.2821-01
1.282E-Ol
2.0000
27.212
125.1187
118.41
.000
1. 01l2E-Ol
.000
8.1I30E-02
8.1130E-02
10.0000
1311. 01111
234.834
52.80
.000
4.725E-02
.000
3.284E-02
3.2114E-02
RH IX
liS
EO' 4.2445E+00
(RYD)
No.
4.31185
MU'
1 .11315
E (RYD)
E 1 EV)
E PHOT ( EV)
LAMIDA lA'
(L/R/L-l'
(L/R/L+1'
SIOMA L-l
SIGMA L+l
SIOMA
(Mil)
.0000
.000
57.750
214.70
.000
2.1111 E-O 1
.000
1 .1I114E -0 1
1.11114E-Ol
2.0000
27.212
84 .11112
1411.113
.000
1.300E-Ol
.000
1I.023E-02
1I.023E-02
Il.0000
81 .11311
138.3811
88.115
.000
Il.114 lE - 02
.000
3.8153E-02
3.883E-02
RH IX
as
EO'
1.118117E+00 CRYD.
N··
Il.38112
MU'
1.11148
E (RYD)
E CEV)
E PHOT ( EV)
LAMIIDA
CA)
IL/R/L-1l
tL/R/L+I)
SIOMA L- 1
SIOMA L+l
SIOMA
(MB)
.0000
.000
27.031
4118.1111
.000
3.811I1E-Ol
.000
2.712E-Ol
2.712E-Ol
2.0000
27.212
54.243
228.58
.000
1.514E-Ol
.000
7.814E-02
7.814E-02
Il.0000
81 .1135
108.11811
114.10
.000
5.1I1I1E-02
.000
2.1114E-02
2. 154E-02
12.0000
1113.271
1110.302
115. 15
.000
2. 5211E - 02
.000
7.1150E-03
7.1150E-03
RH IX
lOS
EO'
1.11I05E+00 (RYD'
N··
8.31108
MU'
, .110112
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+I)
SIOMA L- 1
SIOMA L+l
SIOMA
(MB)
.0000
.000
15.B1I3
7112.08
.000
Il.27I1E-Ol
.000
3.875E-Ol
3.875E-Ol
2.0000
27.212
42.11115
288.25
.000
1.481E-Ol
.000
5.1I0SE-02
5.1I08E-02
8.0000
108.847
124.1101
1111.1111
.000
3.130E-02
.000
7.III1I1E-03
7.11115E-03
RH IX
12S
EO' 7.41184E-Ol
IRYD)
No'
10.31134
MU'
1 . 1101111
E (RYD)
E (EV,
E PHOT (EV)
LAMBDA
lA)
(L/R/L-l'
(L/R/L+I)
SIOMA L-I
SIOMA L+l
SIGMA
(MB)
.0000
.000
10.202
1215.28
.000
8.1I87E-Ol
.000
Il. 1118E-0 1
5.158E-Ol
2.0000
27.212
37.414
331.38
.000
1.347E-Ol
.000
4.287E-02
4.287E-02
8.0000
8 1 . 1135
111.838
135.01
.000
3.578E-02
.000
7.38lE-03
7.381E-03
12.0000
183.271
173.473
71.47
.000
1.417E-02
.000
2. 188E-03
2. 188E-03
RH IX
18S
EO' 3.1I088E-Ol
(RYD)
N··
14.31158
lIIIu.
1.11044
E (RYD)
E (EV)
E PHOT lEV)
LAMBDA
(A)
(L/R/L-Il
(L/R/L+I)
SIGMA L-l
SIOMA L+l
SIGMA
(MB)
.0000
.000
5.318
2331.44
.000
1.551 E+OO
.000
8.038E-Ol
8.038E-OI
2.0000
27.212
32.530
381. 15
.000
1. 045E-0 1
.000
2.23lE-02
2.23lE-02
4.0000
54.424
511.742
207.54
.000
4.203E-02
.000
Il.831E-03
8.831E-03
10.0000
138.0511
'41.377
'7.70
.000
1. 177E-02
.000
1.230E-03
1. 230E -03
RH IX
20S
EO' 2.31134E-Ol
CRYD)
N··
18.311118
MU'
1 .11034
E lRYD)
E 1 EV)
E PHOT (EV)
LAMBDA
(Al
(L/R/L-l)
(L/R/L+')
SIOMA L- 1
SIGMA
L+l
SIOMA
(MB)
.0000
.000
3.2118
3807.48
.000
2.352E+00
.000
1. 132E+00
1.132E+00
1.0000
13.8011
18.882
735.28
.000
1.878E-Ol
.000
4. 138E-02
4.138E-02
4.0000
54.424 .
57.880
214.88
.000
3.087E-02
.000
3.455E-03
3.411I1E-03
RH IX
5P
EO' 8.4778E+00
(RYD)
N°'
3.5381
MU'
1.48311
E ( RYD-)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-' )
(L/R/L+1 )
SIOMA L- 1
SIOMA L+l
SIOMA
(Mill
.0000
.000
88.138
140.87
1.84I1E-0'
1.00IE-Ol
Il.28lE-02
3.1187E-02
8.888E-02
.8000
8.184
88.302
128.711
1.80lE-0'
1I.717E-02
5.173E-02
3.808E-02
8.883E-02
1.0000
13.8011
101.744
121.88
1.488E-OI
Il.481 E-02
4.1182E-02
3.8321-02
8.414E-02
1.1000
20.4011
108.1147
114.22
1.322E-Ol
Il.184E-02
3.87IE-02
3.818E-02
7.780E-02
2.0000
27.212
115.380
107.48
1.118E-OI
8.838E-02
3.4721-02
3. 77:U-02
7.24I1E-02
RH IX
8P
EO' 3.81114E+00
(RYOl
No'
4.11882
MU'
1.4318
E (RYD)
E (EV)
E PHOT (IV)
LAM8DA
( ....
(L/R/L-I)
(L/R/L+I)
SIOMA L-l
SIOMA L+I
SIOMA
(M8)
.0000
.000
52.811
234.78
3.028E-Ol
1.117E-Ol
1.014E-Ol
2.758E-02
1.280E-Ol
.0800
.8111
53.827
231. 20
2.853E-Ol
1.115E-Ol
11. 787E-02
2.782E-02
1.258E-OI
.8000
12.245
85.018
180.58
2.153E-Ol
1.0481-01
8.3151-02
3.000E-02
8.3'51-02
, .0000
13.808
88.418
188.88
2. 08 lE - 0 1
1.038E-Ol
Il.0251-02
3.002E-02
8.027E-02
2.0000
27.212
80.022
1114.84
1.534E-Ol
8.285E-02
3.8421-02
2.887E-02
Il. 838E -02
3.0000
40.818
83.828
132.42
1.188E-Ol
8.270E-02
2.7571-02
2.H2E-02
Il.440E-02
RH IX
8P
10.
1.811110E+00 (nO)
No'
Il.11885
MU'
1.41111
E (RYD)
E (IV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-I)
(L/R/L+11
SIGMA L- 1
SIGMA L+l
SIGMA
(M8)
.0000
.000
211.3811
488.35
Il.225E-Ol
1.20IlE-Ol
2.01lIE-OI
1.54I1E-02
2.215E-OI
.7000
8.1124
34.1113
3115. 13
3.88111-01
1.1711E-OI
11.8421-02
2.034E-02
1.188E-OI
.8000
10.888
311.273
341.81
3.443E-Ol
1.181E-Ol
1I.005E-02
2.0471-02
1.10IIE-OI
.8000
12.245
37.1134
328.411
3.238&.-01
1.1411-0'
8.2115E-02
2.052E-02
1.0321-01
1.0000
13.8011
38.11115
317.1111
3.01121-01
1.12U-OI
7.11101-02
2.01lIE-02
11. Ile lE -02
2.0000
27.212
52.1100
2311.71
1.8541-01
11. 181 E-02
3.7871-02
1 .81171 -02
5.84I1E-02
RH IX
10P
EO'
1.0111131+00 (RYD)
No'
8.51155
MU'
1 .4045
E IRYDl
1
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(L/R/L-l)
(L/R/L+' )
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L+l
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(M8)
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.000
14.11111
831.20
1.04I1E+00
I.081i-Ol
3.4171-01
7.084E-03
3.488E-OI
.2000
2.721
17.838
702.1111
7.1I12E-Ol
, .214E-Ol
2.313E-OI
1.0811E-02
2.422E-OI
.8000
10.885
25.801
480.54
4.11I3E-Ol
'.157E-Ol
11.50 lE -02
1.447E-02
1.01lIlE-OI
.11000
12.245
27.1112
4511.47
3.847E-OI
'.128E-OI
8.4221-02
1.44I1E-02
1I.87IE-02
1.0000
13.11011
28.1122
434.70
3.11451-01
1.01lIlE-Ol
7.50IlE-02
1.442E-02
8.1I52E-02
2.0000
27.212
42.128
2114.31
1.844E-OI
8.2118E-02
3.000E-02
1.215E-02
4.215E-02
3.0000
40.818
55.734
222.411
1. 153E-Ol
Il.45I1E-02
1.55lE-02
1I.73lE-03
2.524E-02
4.0000
114.424
1111 . 340
178.81
7.1I87E-02
5.211 E -02
SI. 288E -03
7.88I1E-03
1.715E-02
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AH IX
12P
EO· 7.2105E·Ol
(AYD 1
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10.511811
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Il.811
1283.80
1 . 5117E+00
1l.1I80E -02
5.0"IIE-Ol
1 .1111 1E·03
5.0811l-01
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5 ..... 2
15.253
812.87
7.505E-Ol
1.18I1E·01
1.800E-Ol
Il. 032E -03
1 . 8110E-0 1
. 11000
8. , ...
17.117 ..
1188.80
5.702E-Ol
1.1110E-Ol
1.22.. E-Ol
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1.3251-01
. 7000
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111.335
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1. 031 E-0 1
1.03I1E-02
1.1311E·01
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10.8a5
20.111115
51111. 10
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1. oll1E-Ol
8.78AE-02
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Il.828E-02
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8.11021-02
1.0000
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23."'11
5211."8
3.115111-01
1.025E-Ol
Il.51151-02
1.0311-02
7.511I1E-02
2.0000
27.212
37.022
33".110
1.111131-01
7.2311E-02
2.223E-02
8.127E-03
3.03I1E-02
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AH IX
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(RYD1
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1.31182
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SlaMA L.-l
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5.11111
23118.70
2.81131-00
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Il.05111-01
1.070E·03
Il.0701-01
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2278.73
2.115I1E-00
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2071.53
2.2115E-00
Il. 7711E-03
Il.''331'01
1.152E·05
Il.''331'01
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1,3111
Il.5211
18118.811
1.115I1E-00
3.82H-02
5.2"IIE-Ol
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5.253E-Ol
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2.721
7.8110
1571 ... 2
1."281-00
8.011111-02
3.311I1E-01
2.152E-03
3.3111E-OI
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5.720E-03
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10.885
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Il.2322-02
Il.3221-02
5.7322-03
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711.118
3.781 E-a 1
8.813E-02
5.215E-02
5.11117E-03
5.782E·02
1.0000
13.11011
18.775
11110.311
3.33IE-01
8,"02E-02
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111.7311
135. III
1.1I08E-02
7.408E-02
8.lIII1E-04
1.80BE-02
1 . 8118E-02
8.0000
108.847
118.1148
104.24
1. 1111 E-02
4.808E-02
4. 544E -04
lI.874E-03
1.033E-02
PD X
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(RYD)
N·- 15.11058
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SIGMA L+l
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22111.32
1.438E+00
2.383E+00
3.112E-Ol
1.13I1E-00
1.451E+00
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Il.803
12.3110
1000.73
3.874E-Ol
8.1115E-Ol
5.0011E-02
3.302E-OI
3.803E-Ol
1.0000
13.11011
111.1113
5411.01
1.870E-Ol
4.7IIIIE-OI
1.808E-02
1.587E-Ol
1.7118E-Ol
2.0000
27.212
32.7811
378.02
7.5114E-02
2.213E-Ol
5. 054E -03
Il.084E-02
Il. 5811E-02
Il.0000
81.1135
87.222
142.15
1.3117E-02
5.138E-02
4.3110E-04
8.211I1E-03
8.708E-03
10.0000
138. 0511
141.11411
87.53
5.112I1E-03
2.278E-02
1 . 20llE -04
2.540E-03
2. 711 lE ·03
PD X
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2.1110E-00
3.144E+00
4.571E-Ol
1.257E-00
1. 714E+00
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2.721
8.2111
11180.33
8.802E-Ol
t , 520E +00
1.248E-OI
5.1114E-Ol
8.4421-01
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8.184
11.703
101111.42
3.07lE-Ol
Il.8111E-Ol
2.1173E-02
1.88lE-Ol
2.I1I1E-OI
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11.148
723.14
1.828E-Ol
4.001E-Ol
1.223E-02
Il.8115E-02
1.10IE-Ol
2.0000
27.212
30.752
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8.073E-02
1.772E-Ol
3.055E-03
3.488E-02
3.77U-02
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54.424
57.11113
213.110
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8.1138E-02
8.421E-04
1.002E-02
1 . OIlIlE- 02
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81.1135
es.175
145.57
I.023E-02
3.78I1E-02
2.400E-04
4.383E-03
4. 823E -03
10.0000
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1311.51111
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4. 1311E-03
1.857E-02
Il.441E-05
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1.441 E-03
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1.0811E-Ol
2.0000
27.212
181.375
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8.885E-02
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8.008E-02
8.008E-02
12.0000
183.271
2117.434
41.811
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3.1I44E-02
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AG XI
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80.3315
154.34
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1.1S73E-Ol
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1 .4 13E -01
1.413E-Ol
2.0000
27.212
107.1548
115.211
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8.833E-02
8.833E-02
8.0000
108.847
1811.182
815.54
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5. 187E-02
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3.11111E-02
3.11111E-02
AC Xl
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2.8273E+00 (!IYO)
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322.31
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3.051E-Ol
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2.2150E-Ol
2.250E-Ol
2.0000
27.212
815.880
188.77
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1.433E-Ol
.000
8.477E-02
8.477E-02
8.0000
81 .8315
120.103
103.23
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8.0015E-02
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2.722E-02
2. 722.E -02
AC XI
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22.538
5150.17
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4.782E-Ol
.000
3.212E-Ol
3.212E-Ol
2.0000
27.212
411.748
249.23
.000
1.511E-Ol
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7.141E-02
7. 141 E-02
8.0000
81.8315
104.172
1 Ill. 02
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15.087E-02
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1.1S1I4E-02
1.8114E-02
10.0000
138.0511
1158.151115
78.18
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2.743E-02
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7.499E-03
7.488E-03
AG XI
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1.0872E+00 (AYO)
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1 .415015
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14.783
838.15
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15.783E-Ol
.000
4.277E-Ol
4.277E-Ol
2.0000
27.212
42.005
2S115.17
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1.4157E-Ol
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5.808E-02
15.808E-02
8.0000
108.847
123.040
100.28
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2.817E-02
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8.81 1E- 03
8.81lE-03
AC XI
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1.170E+00
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15.888E-Ol
8.888E-Ol
2.0000
27.212
34.887
354.38
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1.2111E-Ol
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3.288E-02
3.288E-02
8.0000
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138.87
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2.857E-02
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4.1I11E-03
AC XI
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18.151525
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21582.18
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1.772E+00
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1.443E-Ol
1I.443E-Ol
1.0000
13.1S08
18.388
874.24
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15.082E-02
8.082E-02
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154.424
1511.207
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5.528E-03
15.528E-03
AC XI
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121.518
102.03
1.308E-Ol
1I.82lE-02
4.31515E-02
5.01 1E -02
1.388E-02
1.0000
13.1S08
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1.102E-Ol
9.182E-02
3.438E-02
4.773E-02
8.211E-02
10.0000
138.0151
257.1575
48.14
3.878E-02
4.181E-02
8. 104[-03
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3.488E-02
AC XI
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188.17
2.120E-Ol
1.218E-Ol
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1.0000
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141.12
1.8ooe-Ol
1.0715E-Ol
4.782E-02
4.2155E-02
8.01BE-02
8.0000
108.847
183.103
87.71
4.798E-02
5.24I5E-02
8.833E-03
2. 1 lIE -02
2.884E-02
AC XI
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4.288E-01
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8.728E-02
3.1524E-02
1. 025E-Ol
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154.424
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138.154
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7.2115E-02
1 . 883E - 02
1.880E-02
3.e43E-02
8.0000
81.8315
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5.405E-02
8.883E-03
1.444E-02
2.343E-02
10.0000
138.0158
172.440
71.80
3. 115E-02
3.488E-02
3.887E-03
8.788E-03
1.248E-02
AC XI
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2.8518E-Ol
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315.190
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1.394E-Ol
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2.8815E-02
1.028E-Ol
4.0000
154.424
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183.12
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15.300E-02
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2.488E-02
8.0000
81.8315
103.220
120.12
5.18eE-02
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8.15211E-03
1.4351-02
AC XI
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3.427E-Ol
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3.273E-02
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7.842E-02
5.358E-02
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AG XI
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AG XI
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113.8211
108.113
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1.173E-Ol
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AG XI
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2.733E-Ol
8.711I1E-02
7.1170E-02
1.1112E-02
8.8112E-02
1.0000
13.11011
~1l.2115
2117.82
2.213E-Ol
1.11555,-02
!l.5118E-02
1.ll27E-02
7.325E-02
2.'5000
3~.015
1l5.70~
185.88
1.112E-Ol
Il.!l21E-02
2.381E-02
2.280E-02
~ . 1151 E-02
3.0000
40.818
73.!l07
1118.117
1 .01 OE -0 1
Il.120E-02
1.885E-02
2.3015E-02
~.110E-02
~.OOOO
54.424
iii 7 .112
1~2.33
7.5112E-02
iii. 251lE-02
1.252E-02
2.23I1E-02
3.41i11E-02
!l.0000
118.030
100.718
123.10
5.1I00E-02
7.437E-02
8.813E-03
2. IOlE -02
2.1182E-02
AG XI
100
EO·
1 . ~1I02E +00
(RYD)
N··
Il.1032
MU'
.811118
E (AYD)
E (EV)
E PHOT (EV)
~AMIIDA
(A)
(~/R/~-I)
(~/A/~+ll
SIGMA ~ - 1
SIGMA ~+1
SIGMA (Mil)
.0000
.000
111.8117
1124.011
5.545E-Ol
-3.1I07E-02
2.13I1E-01
1.144E-03
2.15U-Ol
.01500
.1180
20.547
803.43
Il.185E-Ol
-2.437E-02
1.117I1E-Ol
~. 1101 E-04
1.1180E-Ol
.1000
1 .3111
21.227
58~.01l
5.855E-Ol
-1.143E-02
r , 82I1E-O 1
1.04IlE-04
1. 830E-0 1
.2000
2.721
22..588
548.81
5.27~E-Ol
1.005E-02
1.57I1E-Ol
8.1I0IlE-0!l
1.580E-Ol
.3000
4.082
23.11.8
517.72
4.780E-Ol
2. 588E -02
1.375E-Ol
5.5241-04
1.382E-Ol
.4000
5.442
25.3011
4811.811
4.311I1E-Ol
~.013E-02
1. 201E -01
1. !l3SE -03
1.222E-Ol
.8000
8.184
28.030
442.33
3.8116E-Ol
5.888E-02
Il.48I1E-02
3.882E-03
Il.83I1E-02
1.0000
13.11011
33.~73
370.41
2.718E-Ol
7. 77IE -02
8.20IlE-02
7.535E-03
8.1172E-02
2.0000
27.212
47.0111
2113.35
1.523E-Ol
8.454E-02
2.7~IIE-02
1.21lIlE-02
~. 014E-02
3.0000
40.818
110.584
20~. 31
Il.8831-02
7.711 a-02
1.41101-02
1.31101-02
2.850E-02
~.OOOO
54.42~
74.2110
11111.811
Il.11112E-02
Il.824E-02
Il.12I1E-03
1.305E-02
2.217E-02
AG XI
!2D
EO· Il.80114E-Ol
(AYD)
N·. 11.1053
MU'
.8837
E (AYD)
E (EV)
E PHOT ([V)
~AM8DA (A)
(~/A/~-1)
(~/A/~+ll
SIGMA ~ - 1
SIGMA ~+ 1
SIGMA
(M8)
.0000
.000
13.347
1128.117
Il.118U-Ol
-1.1157E-Ol
3.134E-Ol
1.381E-02
3.272E-Ol
.0500
.1180
1~.027
883.112
8.8I1U-Ol
-1.317E-Ol
2.787E-Ol
Il.17lE-03
2.87I1E-Ol
.2000
2.721
111.0118
771.115
7.077E-Ol
-5.807E-02
2.023E-Ol
2.043E-03
2.0~3E-Ol
.3000
4.082
17.~28
711. 41
Il.173E-Ol
-2.51I1E-02
1.IlIlIE-Ol
~. IIlU-04
1.1173E-Ol
.4000
5.442
18.7811
11511.811
!5.43llE-Ol
-7.203E-0~
1.3117E-Ol
3.117U-07
1.3117E-Ol
.5000
Il.803
20. 150
1115.33
4.835E-Ol
I.1115E-02
1.184E-Ol
2.3115E-0~
1.188E-Ol
.11000
e. 111~
21.510
5711.41
4.330E-Ol
3.15I1E-02
1.01~E-Ol
8. 011E -04
1.02U-Ol
.8000
10.8815
24.231
511.118
3.!l42E-Ol
5.027E-02
7.1140E-02
2.30lU-03
7.87U-02
1.0000
13.11011
211.1153
4110.02
2.11158E-Ol
Il.118E-02
5.11301-02
3.804E-03
Il.310E-02
2.0000
27.212
40.11118
305.70
1.~7I1E-Ol
7.1115E-02
2. 2211E -02
7.1117E-03
3.02U-02
3.0000
40.818
54. la.
228.111
Il.027E-02
Il.~78E-02
1.10gE-02
8.571E-03
1.11117E-02
~.OOOO
54.424
117.770
182.115
Il.14I1E-02
5 .1I40E -02
Il. ~41 E -03
8.121[-03
1 . 451E -02
51
AG XI
180
EO' !l. 3003E - 01
IRYD)
Na.
HI. 10112
"'U·
.81108
E IRYD)
E (EV)
E PHOT
lEV)
LAM8DA (A)
(L/R/L-l)
(L/R/L+I)
SIG"'A L - 1
SIG"'A L+l
SIGIICA
(IIC81
.0000
.000
7.212
17111.28
1.748E+00
-5.213E-Ol
5.5371:-01
7.388E-02
8.278E-Ol
.2000
2.721
Il.1133
1248.28
I.022E+00
-1.1137E-OI
2.807E-Ol
1.405E-02
2.H7E-Ol
.3000
4.082
11.2.3
10117.87
8.237E-Ol
-1. 187E-Ol
1.1128E-Ol
5.8031-03
1 .1184 E-0 1
.5000
8.803
14.015
884.70
5.728E-Ol
-3.140E-02
r . 158E-0 1
5.210E-04
t . 181 E -01
.8000
8.184
15.375
808.41
4.90lE-Ol
-7.23lE-03
Il.28lE-02
3. 03 lE -0&
Il.284E-02
.8000
10.888
18.0a8
885.1!1
3.7231-01
2.231lE-02
8.303E-02
3.420E-04
8.338E-02
1.0000
13.a08
20.817
5115. !Ill
2 .1I38E-0 1
3.802E-02
4.518E-02
1.135E-03
4.82I1E-02
2.0000
27.212
34.423
380.18
1.25lE-Ol
5.274E-02
1.354E-02
3.810E-03
1.71!1E-02
3.0000
40.818
48.0211
258.1!1
7.083E-02
4.885E-02
8.058E-03
3.1140E-03
Il.1I117E-03
4.0000
54.424
81.83!1
201.18
4.817E-02
3.117I1E-02
3.303E-03
3.87I1E-03
8.1182E-03
AG XI
200
EO' 3.3132E-Ol
(RYD)
N.·
Ill. 1 105
IICU'
.88.5
E IRYD)
E (EV)
E PHOT (EV)
LA"'8DA
(A 1
CL/R/L-l)
CL/R/L+ 1)
SIGIICA L-l
SIGIICA
L+l
SI GIICA
(IIC8>
.0000
.000
4.!I08
27!10.45
2.728E-00
-1.007E+00
8.438E-Ol
1.722E-Ol
1.01lIE+00
.1000
1.381
!I.888
2112.78
1 . 755E - 00
-5.2118E-Ol
4.542E-Ol
8.208E-02
5.183E-Ol
.4000
5.442
Il.1150
1248.07
7.238E-Ol
-1. 03lE-Ol
1.310E-Ol
3.1I111E-03
1.350E-Ol
.8000
8.184
12.871
1178.47
4.817E-Ol
-2.88I1E-02
7.3112E-02
3.403E-04
7.428E-02
.7000
Il.524
14.032
883.80
4.058E-Ol
-8.22I1E-03
5.803E-02
2.0!l3E-05
5.808E-02
.8000
10.8815
15.3113
8015.411
3.470E-Ol
7.1114E-03
4.858E-02
3.835E-015
4.1582E-02
.11000
12.245
18.753
740.08
3.007E-Ol
1.785E-02
3.808E-02
2.013E-04
3.82I1E-02
1.0000
13.808
18.114
1584.411
2.1535E-Ol
2.4110E-02
3.182E-02
4.234E-04
3.204E-02
2.0000
27.212
31.720
3110.88
1.018E-Ol
3.III1I1E-02
8.2154E-03
1.1113E-03
1.018E-02
3.0000
40.818
45.3215
273.55
5.533E-02
3.500E-02
3.488E-03
2.0113E-03
5.581 E - 03
4.0000
54.424
58.1132
210.311
3.5215E-02
2.11152E-02
I.UlE-03
1 .1I38E -03
3. 778E -03
8.0000
81.835
88.143
143.113
1.832E-02
2.1150E-02
7.270E-04
1.515E-03
2.242E-03
AG XI
4F
1l0' Il.248lE+00 (RYD)
Na.
3.15171
"'U·
.38211
E (RYD)
E (EV>
E PHOT (EV)
LAM8DA ~A )
(L/R/L-l)
(L/R/L-l1
SIGIICA L-l
SIG"'A
L+l
SIGIICA
(IIC8>
.0000
.000
125.8211
118.54
4.817E-02
3.388E-Ol
7.2241 -03
5.11I1E-Ol
'.ll1lE-Ol
2.0000
27.212
153.041
81.02
3. 33 lE - 02
2.317E-Ol
4.574E-03
2.1151E-Ol
2.11915E-Ol
8.0000
108.847
234.8715
52.83
1.580E-02
Il.1I115E-02
1.5781-03
8.287E-02
8.445E-02
12.0000
183.271
2811. 100
42.111
1.075E-02
15.4541-02
Il.0021-0-
4.324E-02
4. 414E -02
A!= XI
5F
EO' 5.154115E-00
(RYDI'
Na.
4.15312
IICU'
.3888
E (RYD 1
E (EV)
E PHOT (EV)
LAM8DA (A)
(L/R/L-I)
tL/R/L+ 1)
SIGMA L- 1
SIGMA
L+l
SIG"'A
("'81
.0000
.000
715.7511
18 1 . 53
Il.23)1-02
4.700E-Ol
1.7151E-02
15. 08eE-0 1
15.2154E-OI
2.0000
27.212
103.1171
1 111 . 25
5.508E-02
2.871E-01
8.4114E-03
3.077E-Ol
3.115lE-Ol
15.0000
81.835
158.3114
78.28
2.834E-02
1.375E-Ol
2.115I1E-03
1.075E-Ol
i , 105E-Ol
8.0000
108.847
185.15015
158.80
1.1178E-02
1.027E-Ol
1 .1I15E -03
7.03IE-02
7.230E-02
12.0000
1153.271
240.030
51.155
1.227E-02
15.308E-02
Il. 7311E-04
3.430E-02
3.527E-02
AG XI
15F
EO' 3.8187E+00
(RYD)
Na.
5.8305
IICU'
.38111
E CRYDI
E (IV)
E PHOT (EV 1
LAMIDA
(A)
CL/R/L-l)
(L/R/L-l)
SIGMA L- 1
SIGMA
L+ 1
SIGMA
(MIl
.0000
.000
51.1130
238.78
1.524E-OI
8.03d-Ol
3.250E-02
8.7110E-Ol
7.115E-Ol
2.0000
27.212
711.142
158.1115
7.413E-02
3.210E-Ol
1.17lE-02
2.1128E-Ol
3.0451-01
4.0000
54.424
1015.353
1115.58
4.422E-02
1.9alE-Ol
5.800E-03
1. !I14E-0 1
1.570E-Ol
8.0000
81.835
133.585
112.83
2.1145E-02
1.353E-Ol
3. 1 IllE -03
8.785E-02
Il. Oll7E - 02
10.0000
138.0511
187.989
IIS.9!1
1.574E-02
7.3721-02
1.2!15E-03
3.1588E-02
3. 7114E -02
12.0000
1113.271
215.201
57.81
1.22lE-02
5.744E-02
8.843E-04
2.51501-02
2.838E-02
AG XI
8F
EO'
2.0793E+00
(RYD)
N.·
7.15285
MU'
.3715
E (RYD,
E (EV)
E PHOT
(EV)
LAMIDA
(A 1
(L/R/L-l)
(L/R/L-l)
SIGMA L- 1
SIGMA L-l
SIGMA
(IIC8)
.0000
.000
28.2110
438.27
3.081E-Ol
8.733E-Ol
7.233E-02
7.748E-Ol
8.471E-Ol
2.0000
27.212
55.502
223.39
Il. 755E-02
3.410E-Ol
1.422E-02
2.318E-Ol
2.480E-Ol
4.0000
54.424
82.714
149.110
4.1491-02
1.851E-Ol
5.238E-03
1.018E-Ol
1.070&-01
8.0000
8 1 . 1535
1011.1128
112.79
2.914E-02
1.1158E-Ol
2.513E-03
5.385E-02
5.838E-02
10.0000
1315.059
184.3411
75.44
1.3110E-02
15.874E-02
8.558E-04
2.038&-02
2.122&-02
AG XI
lOF
10'
1.3055E+00
(RYD)
N··
'.8274
"'U·
.37215
E (RYD)
E (EV)
E PHOT
(EV)
LAM8DA ( Al
(l./R/L-l)
(L/R/L-l)
SIGMA L- 1
SIGMA L+ 1
SIGMA
(M8l
.0000
.000
17.782
1598.04
15.053E-Ol
1. 154E-00
1.22lE-Ol
8.41141-01
9.715E-Ol
2.0000
27.212
44.974
275 . 811
1. 043E-Ol
3.280E-Ol
1.3181-02
1.718E-Ol
1.848E-Ol
4.0000
54.424
72.188
171.78
4.5158E-02
1 . 802E -0 1
4.03I1E-03
8.1558&-02
7.0150E-02
8.0000
108.847
1211.15011
17.113
1.851E-02
Il.453E-02
Il. 293E-04
1.8931-02
1 .1I815E - 02
12.0000
1153.271
181.033
158.411
8.4151E-03
3.473E-02
3.482E-04
7.1421-03
8. UIOE-03
AG XI
12F
10' 8.11508E-Ol
(R'rDl
Na.
11 .82811
MU'
.3731
E (RYD)
E (EV)
E PHOT (IlV)
LAM8DA
( A)
(L/R/L-l)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA
(M8i
.0000
.000
12.178
1018.011
7.399E-Ol
1.448E+00
1. 7111E-0 1
Il.173E-Ol
1 . 01l7E -00
2.0000
27.212
311.3110
314.78
1.017E-Ol
2.975E-Ol
1.0117E-02
1.252E-Ol
1.3152E-Ol
4.0000
54.424
1511.802
1815.111
4.05I1E-02
1.382E-Ol
2.955E-03
4.438E-02
4.7341-02
8.0000
108.847
121.0215
102.45
1.379E-02
5.225E-02
8.19111-04
1.18111-02
1 . 248E -02
10.0000
138.059
148.238
83.84
Il. 4154E -03
3.7031-02
3. 58eE -04
7.298E-03
7.8551-03
AG XI
ll1F
EO' 4.11553E-Ol
(RYD)
Na.
15.152153
. MU'
.3737
1
(RYD)
1
lEV)
E PHOT
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LAMIDA (A 1
(L/R/l.-l)
IL/R/L-l)
SIGMA L-l
SIGMA
L-l
SIGMA
(M81
.0000
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8.742
1838.118
1.3121-00
2.081 E+OO
3.127E-Ol
1.048E-00
1.3811+00
1.0000
13.808
20.348
8011.33
2.0751-01
4.847E-Ol
2.380E-02
1.718E-Ol
1.9121-01
2.0000
27.212
33.1154
385.18
8.889E-02
2.388E-Ol
8.8721-03
8.83111-02
7.5271-02
4.0000
54.424
81.188
202.71
3.102E-02
Il.1133E-02
1.5851-03
2.1157E-02
2.325E-02
8.0000
81.835
88.378
140.211
1.11041-02
5.5881-02
8.12151-04
Il.1I0IlE-03
1.0521-02
10.0000
138.0511
142.801
88.82
8.8251-03
2.5215E-02
1. 818E-04
3.2721-03
3.441E-03
52
AG XI
20F
EO. 3. l~l~E-Ol IRYD)
No.
111.112110
MU-
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E 1RYD)
E (EV)
E PHOT (EV)
I.AMBDA
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(I./R/I.-n
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SIGMA 1.- 1
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SIQMA
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.0000
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~.27.
2900.85
2.012E+00
2.771 E+OO
~.1I110E-Ol
1. 171li+00
1.a~5E+00
.!looo
Il.803
11.077
11111.30
~. 152E-Ol
7 .1I28E -01
5.1 •• E-02
2.500E-Ol
3.015E-Ol
1.0000
13.11011
17.880
e83.~3
1.8111 E-O 1.
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1 . all8E - 02
1.102E-Ol
1. 2118E-0 1
2.0000
21.212
31 .•811
3113.78
7.10.E-02
1.878E-Ol
•. 21I1E-03
3.1187E-02
•. ~15E-02
•. 0000
5..... 2.
58.1188
211.23
2.3117E-02
7.505E-02
Il.081 E-O.
t.187E-02
1.27U-02
Il.0000
81.1135
85.1110
1.... 32
1.212E-02
4.147E-02
3.311I1E-04
5.305E-03
5. Il''!U- 03
10.0000
1311.0511
140.333
811.35
4.8112E-03
1.845E-02
Il.045E-05
1.7 IllE -03
1.80lSE-03
53
CD XII
5S
EO'
1.1358E+Ol
(AYDI
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3.5810
MU'
1 .43110
E (AYD 1
E (EV)
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LAMBDA
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SIGMA L-,
SIGMA L+l
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154.505
80.25
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1.008E-Ol
.000
Il.828E-02
Il.825E-02
2.0000
27.212
181.717
58.23
.000
8.154E-02
.000
7.5111E-02
7.5111E-02
14.0000
1110.483
344.1188
35.114
.000
3.455E-02
.000
2.51101-02
2.5110E-02
CD XIl
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(AYD)
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4.58411
MU'
1 .4151
E (RYD)
E (EV)
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(L/R/L-l)
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SIGMA L- 1
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(Mil)
.0000
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113.203
133.03
.000
1.487E-Ol
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I.2115E-Ol
1.2115E-Ol
2.0000
27.212
120.415
102.117
.000
1.05IE-Ol
.000
8.358E-02
8.3118E-02
8.0000
108.847
202.050
51.35
.000
5.133E-02
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3.348E-02
3.348E-02
CD lUI
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SI GlU
L - 1
SIGMA L+l
SIGMA
(Mil)
.0000
.000
44.11711
275.88
.000
2.8117E-Ol
.000
2.051SE-Ol
2.058E-Ol
2.0000
27.212
72.1110
171.75
.000
1.378E-Ol
.000
8.511E-02
8.81 1E-02
8.0000
81.835
128.814
117.112
.000
8.II8E-02
.000
2.1178E-02
2.1178E-02
14.0000
1110.483
235.481
52.88
.000
2.48I1E-02
.000
Il.187E-03
Il.187E-03
CO XII
lOS
10.
1 ."~71+00
(RYO)
N··
8.8051
MU'
1 .311411
E (RYD)
E (EV)
E PHOT ( EV)
LAMIIOA
lA)
(L/R/L-l)
(L/R/L+11
SIGMA L-,
SIGMA L+l
SIGMA (Mil)
.0000
.000
28.4511
488.80
.000
4.202E-Ol
.000
2.1138E-Ol
2 . Il3 ISE - 01
2.0000
27.212
53.871
231.01
.000
1.500E-Ol
.000
7.8112E-02
7.5112E-02
8.0000
81.535
108.0114
114.70
.000
5.331E-02
.000
1.11301-02
1 .1I30E -02
10.0000
138.01111
152.518
78.211
.000
2.1120E-02
.000
8.70IlE-03
8.70U-03
CD XII
12S
EO'
1.27118E+00
(RYD)
N•• 10.8078
MU'
1 .31124
E (AYD)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/R/L-l)
(L/R/L-l)
SIGMA L-l
SIGMA L+l
SIGMA
(Mill
.0000
.000
17.412
712.08
.000
5.117I1E-Ol
.000
3.1112E-Ol
3.1112E-Ol
2.0000
27.212
44.824
277.85
.000
1.4881-01
.000
8.188E-02
8.188E-02
8.0000
108.847
128.280
118.20
.000
3.1381-02
.000
7. 802E -03
7.802E-03
18.0000
217.585
235.107
52.74
.000
1.250E-·02
.000
2.310E-03
2.310E-03
CD XII
18S
EO' 8.7485E-Ol
(RYD)
N••
14.80118
MU'
t .3802
E (RYDI
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-I)
(L/R/L-l)
SIGMA L- 1
SIGMA L+I
SIGMA (Mill
.0000
.000
Il. 1711
1350.73
.000
1.031 E+OO
.000
8.128E-Ol
8.128E-Ol
2.0000
27.212
38.381
340.71
.000
1.288E-Ol
.000
3.711I1E-02
3.71181-02
8.0000
81 .835
110.815
138.53
.000
3.222E-02
.000
5.1128E-03
5.1128E-03
CD XII
20S
EO'
4.15781-01
(llYD)
N•• 18.8107
MU'
1.3883
E (AYO)
E (EV)
E PHOT (EV)
LAMIIDA
(A)
(L/R/L-l)
(L/R/L+1 )
SIGMA L' 1
SIGMA L+l
SIGMA (Mill
.0000
.000
5.857
21111 .84
.000
1 .581 E -00
.000
8.881E-Ol
8.881E-Ol
1.0000
13.808
111.283
843. se
.000
2.40111-01
.000
7.024E-02
7.024E-02
4.0000
54.424
80.080
208.37
.000
4.2276-02
.000
8.748E-03
8.748E-03
10.0000
138.01111
141.718
87.411
.000
1. 153E-02
.000
1.1851-03
1.188E-03
CD XII
5P
EO'
1.0348E+Ol
(RYD)
N••
3.7308
MU'
1 .28112
E (llYD)
E (EV)
E PHOT lEV)
LAMIIOA
(A)
IL/R/L-I)
(L/R/L+I)
SIGMA L - 1
SIGMA L-l
SIGMA
(Mil)
.0000
.000
140.783
88.08
1.122E-Ol
Il.547E-02
3.712E-02
5.374E-02
Il. 08 ISE - 02
1.0000
13.808
154.3811
80.32
Il. 887E-02
8.8401 -02
3.022E-02
5.054E-02
8.07151-02
10.0000
138.0511
278.823
44.711
3. 750E -02
4.1118E-02
8. 1531-03
2.802E-02
3.8181-02
CD XII
8P
EO'
8.3511~1+00 (AYD)
N...
4.7885
MU'
1.2415
1
(RYD)
1
(EV)
1 PHOT (EV)
LAMBDA
lA 1
(L/R/L-l)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA
(Mil)
.0000
.000
88.528
143.211
1.80111-01
1.11181-01
5.11321-02
5.200E-02
1.1131-01
1.0000
13.808
100.132
123.82
1.4231-01
1 .0571 -0 1
4.24111-02
4.88111 - 02
8.1138E-02
8.0000
108.847
1115.373
83.48
4.73IE-02
5.31IE-02
Il. 158E-03
2.3081-02
3.2241-02
CD Xli
8P
10' 3. J3541+00
(RYD)
N••
8.77811
MU'
1.2231
1
(RYD)
1 (IV)
E PHOT (IV 1
LAMBDA
(A)
(L/R/L-t)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA (Mil)
.0000
.000
42.881
2110.83
3.8481-01
1.81171-01
1.18111-01
5.1481-02
1.704E-Ol
r . 0000
13.1108
511.287
220.38
2.3021-01
1.3271-01
8.2481-02
4. 152E-02
1. 0401-01
8.0000
81.835
124.298
1111.75
Il.1181-02
5. lIaU-02
Il.747E-03
l.lSlS7E-02
2.842E-02
10.0000
138.01111
178.720
lSlI. 37
3. 3211E -02
3.11821-02
4. 14111-03
1.0151-02
1.4301-02
CD XII
10P
10'
1.881151+00 (RYD)
N••
8.78311
MU.
1.2185
1
(RYD)
1
(EV)
E PHOT (IV)
LAMIIDA
lA)
(L/R/L-t)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA
(M8)
.0000
.000
25.3115
488.22
8.0701-01
2.1881-01
1.1180E-Ol
Il.01121-02
2.48111-01
1.0000
13.808
311.002
317.110
.2.88eE-Ol
1.4771-01
7.187E-02
3.588E-02
1. 0751 -0 1
4.0000
54.424
711.8111
1!l5.33
8.11021-02
8.7471-02
1.3251-02
1.5221-02
2.8471-02
8.0000
81.835
107.031
115.84
5.4281-02
4.7731-02
8.805E-03
1 . 022E -02
1.8821-02
8.0000
108.847
134.243
112.38
3.7041-02
3.8321-02
3.858E-03
7.418E-03
1.1281-02
CD XII
12P
10'
1.23781+00 (RYD)
N•• 10.7888
MU'
1.2134
1
(RYD)
E 1IV)
1
PHOT (IV)
LAMIIDA
(A)
( L/A/L-O
(L/R/L+1)
SIGMA L-l
SIGMA L+l
SIGMA
(Mil)
.0000
.000
111.8311
738.30
Il.048E-Ol
2.8821-01
2.8881-01
4.1111111-02
3.388E-Ol
1.0000
13.808
30.445
407.25
3.3801-01
1.5281-01
7.2001-02
2.11791-02
1.0181-01
4.0000
54.424
71.283
173.118
8.012E-02
5.85111-02
Il.5831-03
1. 025E -02
1 .1I83E -02
8.0000
81.83!5
118.475
12!5.91
4. 83!5E -02
3.11701-02
4. 432E -03
8.503E-03
1.01141 -02
CD XII
18P
EO' 8.5U5E-Ol
(RYD)
N.' 14.78a4
MU-
1.2108
E lRYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/Lol)
SIGMA L- 1
SIGMA LOI
SIGMA (MB)
.0000
.000
8. U8
1384.18
1. B5aEoOO
3.557E-Ol
5.18lE-Ol
4.74aE-02
5.838E-Ol
1.0000
13.808
22.583
548.50
3.52aE-Ol
1. '152E-0 1
5,BS7E-02
l.aUE-02
7.880E-02
4.0000
54. '24
83.381
1as . 82
a.158E-02
4.347E-02
5.03tE-03
5.018E-03
1.0015E-02
10.0000
138.05a
145.017
815 .50
1.51lE-02
1.557E-02
a.a3IE-04
t.'73E-03
2. 188E - 03
CD XIl
20P
EO' 4.0783E-Ol
(RYD)
N·. 18.7a08
MU-
1 .201i14
E \\AYD)
E 1 EV)
E PHOT (!V)
LAMBDA
(A)
lL/R/L-l)
(L/A/Lol)
SIGMA L- 1
SIGMA LoI
SIGMA (MB)
.0000
.000
5.54a
2234.43
2.818EoOO
4.378E-Ol
7.a52E-OI
4.458E-02
8.3a7E-Ol
1.0000
13.808
la. 15!l
847.2a
3.277E-Ol
1.283E-Ol
4.310E-02
1.322E-02
5.832E-02
2.0000
27.212
32.781
378.4B
1. 324E-Ol
a. 88U - 02
1.202E-02
8.475E-03
1.850E-02
4.0000
54.424
5a.a73
208.74
4.748E-02
3.300E-02
2.830E-03
2.738E-03
!l.585E-03
8.0000
108.847
114.3'8
108.38
1 . !l83 E- 02
1.478E-02
a.008E-04
1.044 E-03
1. &44E-03
10.0000
138.059
141.808
87.58
1.102E-02
1.127E-02
3.800E-04
7. 53llE -04
1.114E-03
CD XII
40
EO'
1.810aE·OI
(RYO)
N.·
2. Il8 lUI
MU'
1.0101
E (RYOI
E lEV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-ll
(L/R/L·')
SIGMA L- 1
SIGMA L·l
SIGMA 1MB)
.0000
.000
2111.171
58.57
5.8a8E-02
1.21aE-OI
1. 788E -02
1.228E-OI
1. 407E-0 1
1.0000
13.808
232.777
53.28
5.159E-02
1.178E-Ot
1.557E-02
1.214E-Ol
1.370E-Ol
8.0000
81 .835
300.808
41.22
3.372E-02
Il.510E-02
8.5117E-03
1.028E-Ol
1. 112E-0 1
8.0000
108.847
328.018
37.80
2.aI8E-02
8.700E-02
7.012E-03
Il.380E-02
1.008E-Ol
CD XIl
50
EO'
8.83851·00
( RYO)
N··
4.0833
MU'
.1187
E lRYD)
E ( EV)
PHOT (EV)
LAMBOA
(A 1
IL/R/L-l)
lL/R/L·l)
SIGMA L-1
SIGMA L·l
SIGMA 1MB)
.0000
.000
117.507
105.51
1.070E-Ol
1. 2B4E-0 1
3.38IE-02
7.079E-02
1.048E-Ol
.8000
8. t84
125.871
118.88
Il.588E-02
1.23I1E-Ol
2.8110E-02
7.288E-02
1.018E-OI
1.0000
13.808
131.113
114.58
8.912E-02
1.217E-Ol
2.817E-02
7.327E-02
Il.1I44E-02
2.0000
27.212
144,71a
85.87
7.555E-02
1. 1157E-0 1
2.078E-02
7.302E-02
Il.378E-02
4.0000
5•. 424
171.1131
72. Il
5.81l7E-02
1.027E-OI
1.383E-02
8.83I1E-02
a.222E-02
8.0000
al.835
1911.143
82.28
4.414E-02
9.087E-02
Il. 754E-03
a.I72E-02
7.148E-02
CO XII
80
EO' 5,SIS3E·OO
lRYO)
N••
5.10117
MU'
.8903
-E
(RYO)
E (EV)
E PHOT (IV)
LAMBDA
(A)
(L/A/L-l)
(L/R/Loll
SIGMA L- 1
SIGMA L·'
SIGMA (MB)
'.0000
.000
75,041
185.23
1.715E-01
1.288E-Ol
5.S4U-02
4.1577E-02
1.022E-01
1.0000
13.808
88.8'7
1311.87
1.2a5E-OI
1.24I1E-01
3. 738E -02
5.212E-02
8.950E-02
1.5000
20.4011
115.450
12a.1I0
1.143E-Ol
1 . 213E -0 1
3.138E-02
5.2114E-02
8.430E-02
2.0000
27.212
102.25.2
121.211
1.018E-Ol
1.172E-Ol
2.1182E-02
5.2117E-02
7.980E-02
2.5000
34.015
loa.055
113.811
Il.127E-02
1.129E-Ol
2.2a3E-02
5.245E-02
7.528E-02
8.0000
81.835
158.878
79.14
4.a2I1E-02
8. 530E-02 .
Il.58I1E-03
4,29aE-02
5.255E-02
CD XII
80
EO'
2. 8344E"'00
(RYO)
N·'
7.1277
MU'
.a723
E lRYO)
E (EV)
E PHOT (EV 1
LAMBDA
(A 1
(L/R/L-l)
lL/A/L.,)
SIGMA L-I
SIGMA L·l
SIGMA (MB)
.0000
.000
38.585
321.50
3.417E-Ol
1 . 148E- 0 1
1.132E-Ol
1.1I18E-02
1.324E-Ol
.2000
2.721
41.288
300.31
3.048E-01
1.11I8E-OI
9.828E-02
2.228E-02
1.185E-Ol
1.0000
13.808
52. 171
237.85
2.050E-Ol
1.223E-OI
5.512E-02
2.1141E-02
a.d3E-02
1.5000
20.40a
58.174
210.24
1. 885E -0 1
1.18lE-01
4.lllE-02
3.IOlE-02
7.211 E-02
2.0000
27.212
115.777
188.41
1.3i3E-Ol
1.125E-01
3.183E-02
3.137E-02
8.300E-02
2.5000
34.015
72.580
170.83
1.170E-01
1.084E-01
2.4118E-02
3. 1OOE -02
5.5115E-02
8.0000
81.835
120.201
103.15
4.927E-02
7.147E-02
7.334E-03
2.315E-02
3. 04aE -02
CO XII
100
EO'
1 . 7258E .00
(RYO)
N.'
B.1342
MU'
.885e
E lRYDJ
E lEV)
E PHOT (EV)
LAMeDA
lA)
(L/A/L-ll
(L/A/L·')
SIGMA L-l
SIGMA L·l
SIGMA (M8 )
.0000
.000
23.483
527.1111
5.830E-Ol
7.582E-02
1.871E-Ol
5.083E-03
1.922E-01
.4000
5.442
28.925
428.85
3.118IE-01
1.048E-Ol
t.14lE-Ol
1.1a4E-02
1.2801-01
,8000
8.184
31.84l5
3111.79
3.403E-Ol
1.100e-01
a.209E-02
1. 443E -02
1.085E-OI
1.0000
13.808
37.0811
334.30
2.801E-Ol
1.124E-Ol
8.305E-02
1,788E-02
8.073E-02
1 .5000
20.409
43.8111
282.48
t.1I54E-Ol
1.085E-Ol
4.21 1E- 02
1.1I50E-02
8.180E-02
2.0000
27.212
50.8114
244.58
1.52I1E-Ol
1.020(-01
2.1177E-02
1 . 9110E -02
4.1187E-02
2.5000
34.015
57.4117
215.84
1.233E-Ol
9.49I1E-02
2.197E-02
1 . 158E -02
4.153E-02
8.0000
81.835
105.118
117,115
4. 37lE -02
5.833E-02
5.047E-03
1.34I1E-02
1.8!53E-02
CO XII
120
EO-
1.180IlE-00 (RYO)
N.· Il.1374
MU'
.8U8
E (RYO)
E ( EV)
E PHOT (Ev)
LAMBDA
(A)
(L/A/L-I)
(L/A/L-l)
SIGMA \\,-1
SIOMA L-l
SIGMA (MB)
.0000
.000
15.711$
784.117
8.325(-01
1.208E-02
2.751E-OI
8.8113E-05
2.752E-Ol
.2000
2.721
18.51&
8U. 81
8.370E-Ol
5.125E-02
1.88I1E-Ol
2.3B9E-03
1 .1I12E-0 1
.8000
8.184
23 .•sa
517.50
4. 124E-ol
9.337E-02
1.024e-01
7.875E-03
1.1031-01
.8000
10.885
28.880
484.72
3.437E-Ol
Il. 888E-02
7.924e-02
a.7111E-03
8.1I03E-02
1.0000
13.808
29.401
421. 71
2.918e-Ol
1.003e-Ol
8.283E-02
1. 118i-02
7. 311lle -02
1.5000
20.40a
38.204
312.47
2.048E-Ol
Il.71U-02
3.815E-02
1.288E-02
5.103E-02
2.0000
27.212
43.007
288.2a
1.527E-Ol
Il.03IE-02
2.520E-02
1. 323E -02
3.843E-02
2.5000
34.015
4a.810
248.112
1.118E-Ol
8.295E-02
1.787E-02
1.2an-02
3.080E-02
4.0000
54.424
70.219
1711.57
&.5.,E-02
8.424E-02
7. 887E -03
1.093E-02
1. 8111E-02
8.0000
81.835
97.431
127.215
3.744E-02
4.775E-02
3.433E-03
8.377E-03
1.18lE-02
55
CD XII
180
EO'
8.2818E-Ol
(RYD)
N·· 15.104004
MU-
.8588
E (RYD)
E (EV)
E PHOT (EVI
LAMBDA
(A 1
(L/R/L-O
(L/R/L+1 )
SIGMA L- 1
SlaMA L+ 1
SI QfIIA
(MB)
.0000
.000
8.5047
10450.83
1.508E+00
-1.8043E-Ol
04.887E-Ol
1.0804E-02
04.888E-Ol
.OBOO
.880
8.227
13043.88
1.328E+00
-1.2804E-Ol
04.080E-Ol
5.738E-03
04. 138E-Ol
.2000
2.721
Il.288
1100.31
8.0481E-Ol
-.2.571 E-02
2.5048E-Ol
2.807E-004
2.5048E-Ol
.3000
04 .082
12.828
.81. 77
7.828E-Ol
1.187E-02
1. 80404E-0 1
8.712E-05
1 .s 045E-Ol
.04000
5.04042
13 .••8
888.28
8.587E-Ol
3.815E-02
1.528E-Ol
8.885E-004
1.533E-Ol
.5000
8.803
15.350
807.73
5.833E-Ol
5.2004E-02
1.2204E-Ol
1.587E-03
1.2040E-Ol
.8000
10.885
' •• 0432
838.08
3.782E-Ol
7.373E-02
8.885E-02
3. 883E -03
7.3804E-02
1.0000
13.808
22.153
5!l1l.8a
3.02.E-Ol
7.78lE-02
5.10.E-02
5.057E-03
5.8104E-02
1.5000
20.04011
28.858
0428.18
1.822E-Ol
7.80U-02
2.8811E-02
8.320E-03
3.321E-02
2.0000
27.212
35.758
3048.73
1.304lE-01
8.855E-02
1.817E-02
8.522E-03
2.270E-02
2.5000
304.015
042.582
281.31
8.880E-02
8.287E-02
1.08IE-02
8.303E-03
1.882E-02
3.0000
040.818
048.385
251.18
7.7204E-02
5.8048E-02
7.04004E-03
5.833E-03
1 . 3304E -02
8.0000
81.835
.0.183
137.048
2.731E-02
3.331E-02
1.88lE-03
3.772E-03
5. 0453E -03
CD XII
200
EO.
3.8301E-Ol
(RYD)
te.· 18.10418
MU-
.85804
E (RYD)
E (EV)
PHOT (EV)
LAMBDA
(A)
(L/R/L - 1)
(L/R/L+I)
SIGMA L- 1
SIGIU
L+l
SIGMA
(MB)
.0000
.000
5.3047
2318.88
2.358E+00
-04.885E-Ol
7.0473E-Ol
04.0425E-02
7 .• 15E-Ol
.2000
2.721
8.0e8
1538.88
1.183E+00
- 1. 0304E-0 1
2.837E-Ol
3.253E-03
2.18.E-Ol
.3000
04.082
8.042.
13104.804
8.101E-Ol
-3.888E-02
1.883E-Ol
04.777E-004
1 .•88E-Ol
.04000
5.04042
10.780
11048.12
7.2504E-Ol
2.2045E-03
1.0427E-Ol
2.051E-08
1. 0427E -01
.5000
8.803
12. ISO
1020.0404
5.838E-Ol
2.5.0E-02
1.077E-Ol
3.073E-004
1.080E-Ol
.8000
8.1804
13.511
817.88
04.885E-Ol
04.058E-02
8. 37lE -02
8.380E-004
8.0455E-02
.8000
10.8.5
18.232
783.804
3.8041E-Ol
5.5045E-02
5.0408E-02
1.882E-03
5. 588E -02
1.0000
13.808
18 .•53
IUi04.17
2.801E-Ol
8.077E-02
3.737E-02
2.838E-03
04.001E-02
1.5000
20.0408
25.758
0481.3.
1. 8804E -0 1
5 .•87E-02
1.7.2E-02
3.04.3E-03
2. 1041 E - 02
2.0000
27.212
32.558
380.80
r , 118E -0 1
5.0421 E-02
1.01U-02
3.808E-03
1 . 380E -02
2.15000
304.015
38.382
3104 .•8
8.0118E-02
04.828E-02
8.0437E-03
3.045.E-03
•. 888E-03
8.0000
81.835
88 .•83
1042.504
2.058E-02
2.0458E-02
Il.204 lE -004
1.878E-03
2.803E-03
CD XII
04F
EO.
1.1137E+Ol
(RYD>
N·· 3.5858
MU-
.040042
E (RYD)
E (EV)
E PHOT (EVI
LAM8DA
( Al
(L/R/L-l)
IL/R/L+\\)
SlaMA
L - 1
SlaMA
L+ 1
SIGMA
<M8)
.0000
.. 000
151.521
81.82
04.103E-02
2.8004E-Ol
8.872E-03
04.27BE-Ol
04.3047E-Ol
2.0000
27.212
178.7.0
18.37
3.0.0E-02
2.004lE-01
04.587E-03
2.8704E-Ol
8.0000
10a.8047
280.378
047.82
1.57.E-02
Il. 8043E -02
1.7048E-03
8.8804E-02
~.: ~~~~:g~
104.0000
180.0483
3042.011
38.25
8.04042E-03
15.0482E-02
8.212E-004
3.880E-02
3.7721-02
CD XII
5F
EO' 8.704048E+00
(RYD)
N·· 04.8208
MU-
.37904
E (RYD)
E (EV)
E PHOT 1 EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+I)
SIGMA L- 1
SIGMA L+l
SIGMA
IM8)
.0000
.000
81.7e.
135. Il
8.255E-02
3.83lE-01
1.8804E-02
5.082E-Ol
5.281E-Ol
2.0000
27.212
1111.881
1004.21
5.280E-02
2.578E-Ol
8.888E-03
2.&35E-Ol
2.8204E-Ol
8.0000
81.835
173.0405
71.50
2.888E-02
1 . 337E -0 1
3.378E-03
1. II04E-O 1
1.1047E-Ol
8.0000
108.8047
200.817
81.80
2.059E-02
1.025E-Ol
2.28IE-03
7.570E-02
7.7'8(-02
104.0000
1.0 .•83
282.252
043.83
1. 082E -02
5.385E-02
8.883E-004
2.818E-02
3.007E-02
CD XII
8F
EO.
04.5552E+00
(RYD)
N·· 5.8225
MU-
.3775
E IRYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+I)
SIGMA L- \\
SIGMA
L+I
SICMA
(MB)
.0000
.000
81.878
200.05
1.370E-Ol
5.088E-Ol
3.132E-02
5.718E-Ol
8.028E-Ol
2.0000
27.212
88.188
138.01
7.275E-02
2.837E-Ol
1.271E-02
2.7152E-Ol
2.880E-Ol
04.0000
504.04204
lIB.0401
108.52
04.538E-02
1.818E-Ol
8.04504E-03
1.535E-Ol
1.58ge-Ol
8.0000
81.835
1043.813
88.33
3.105E-02
1.304 7E- 0 1
3.728E-03
8.357E-02
8.730E-02
10.0000
138.058
188.037
82.81
1.71d-02
7.858E-02
1.587E-03
04.171E-02
04.32BE-02
104.0000
180.0483
252.0480
048. Il
1.080E-02
04 .• 00E-02
7.825E-004
2. 178E-02
2.258E-02
CD XIl
8F
EO'
2.04788E+00
(RYD)
N.· 7.8221
MU'
.3778
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(Al
(L/R/L - 1)
(L/R/L+I)
SI CMA L - 1
SIGMA
L+l
SIGMA
(MB)
.0000
.000
33.7204
387.85
2.783E-Ol
7.382E-Ol
7.083E-02
8.588E-Ol
7.307E-Ol
2.0000
27.212
80.838
203.047
1.005E-Ol
3.233E-Ol
1.8I58E-02
2.287E-Ol
2.0453E-Ol
04.0000
504.04204
88.1047
1040.88
5.225E-02
1.8047E-Ol
8.048IE-03
1.080E-Ol
1.1045E-Ol
8.0000
81 .835
1115.3511
107.048
3.213E-02
1.20lE-01
3.207E-03
5.878E-02
8.300E-02
12.0000
183.271
188.8g5
82.1104
1.185E-02
04.825E-02
7.04048E-004
1.8047E-02
1.722E-02
18.0000
217.8815
251.0418
048.31
7.387E-03
3.103E-02
3.705E-004
8.88IE-03
8.082E-03
CD XII
lOF
EO.
1.5555E+00
(RYD)
N·· Il.8217
MU'
.3783
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+ 1 )
SIGMA L-l
SIGMA L+l
SIGMA
1MB)
.0000
.000
21. le3
585.85
04.813E-Ol
8.800E-Ol
1.213E-Ol
7. 28U-0 1
8.512E-Ol
2.0000
27.212
048.375
258.30
1.118E-Ol
3. 180E-Ol
1.82IE-02
1.757E-Ol
1.818E-Ol
04.0000
504.04204
75.587
1804.03
5.072E-02
1.53U-Ol
5.237E-03
7.287E-02
7.811E-02
8.0000
108.8047
130.011
85.37
1. 880E-02
8.885E-02
1.25IE-03
2.218E-02
2.3045E-02
10.0000
138.058
157.223
78.88
1.325E-02
5.008E-02
7.0432E-004
1.0415E-02
1 . 0488E -02
12.0000
153.271
1804.04304
87.23
8.788E-03
3.788E-02
04. 758E-004
8.558E-03
1.003E-02
CD JIIl
12F
EO.
1.08B2E+00
(RYD)
N.· 11.82104
MU-
.3788
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA
(Al
(L/R/L-I)
(L/R/L+II
SIGMA L- 1
SlaMA L+l
SIGMA
(MB)
.0000
.000
104.507
8504.88
8.7.8E-OI
1.235E+00
1. 8004E-0 1
7 .•040E-OI
Il.7045E-Ol
2.0000
27.212
041.718
287.20
I.IIIE-OI
2.887E-Ol
1.0405E-02
1.31QE-Ol
1.0458E-Ol
04.0000
504.04204
88.130
178.87
04.8104E-02
1.0418E-Ol
3.1152E-03
04. 88llE -02
5.3BOE-02
8.0000
108.8047
123.3504
100.51
1.801E-02
5.e.2e-02
8.511E-004
1.0410E-02
1.0485E-02
10.0000
138.05.
150.5ee
82.35
1.103E-02
04. Oo404i -02
04. 83 lE -004
8.8042E-03
8.33llE-03
18.0000
217.8.5
232.201
53.040
04.803E-03
1. 885E -02
1.04042E-004
2.8.04E-03
3.138E-03
55
CO XII
15F
1<0· 5.11012&-01
IAYD)
No.
15.11211
MU·
.31811
& (AYD)
& (IV)
E PHOT (EV)
LAM.OA
(Al
(L/R/L-l)
(L/R/L-l)
SlaMA L- 1
SIGMA L-1
SIGMA (MB)
.0000
.000
8.0211
Hl44 . 22
1.217E-00
1.784E-00
3.203E-Ol
II. 175E-Ol
1.238E--00
1.0000
13.11011
21.535
513.08
2.28I1E-Ol
4.798E-Ol
3.052E-02
1.78I1E-Ol
2.0114E-Ol
2.0000
21.212
35.241
311.83
Il.889E-02
2.43IE-Ol
II. 282E-03
7.481&-02
8.40IlE-02
4.0000
54.424
52.413
188.53
3.1115E-02
1.053E-Ol
2. 1118E -03
2.48I1E-02
2.705E-02
Il.0000
81.535
811.585
138.28
1. 883E -02
5.0281-02
8.55/5&-04
1.110E-02
1.25I1E-02
8.0000
108.841
1111.8715
105.08
1.151E-02
3.1140E-02
4.213E-04
Il. !l14 E- 03
Il.93!lE-03
14.0000
1110.483
1118.512
152.411
4.245&-03
1.1104&-02
Il.1134E-05
1.8315E-03
1.931E-03
CD XIl
20F
EO· 3.74041-01
IAYD)
No'
111 . 11210
MU·
.31110
E IAYD)
E <EV)
E PHOT IIV)
LAMIDA
(A)
(L/R/L-ll
1L/R/L-I)
SIGMA L-l
SIGMA L- 1
SIGMA 1MB)
.0000
.000
5.0811
24311.21
1.880E--00
2.38I1E--00
4.844E-Ol
1. 041E--00
1.5215E--00
.5000
5.803
11.812
1042.11
4.541E-Ol
1.1111&-01
5.1121 &- 02
2. 51lSE -0 1
3.238&-01
1.0000
13.505
18.1I1!l
1153.20
2.115&-01
4.203E-Ol
2.2!l3E-02
1.18I1E-Ol
1.4IIE-01
2.0000
21.212
32.301
383.85
8.278&-02
1.115IE-Ol
5.9110E-03
4.4158E-02
5.01!lE-02
Il.0000
81.835
811. 725
142.11
1. 435E -02
4.5011&-02
4.812E-04
Il. 323E -03
Il.804E-03
12.0000
183.271
1118.3110
73. B4
4. l1111E -03
, .51111-02
7.882E-05
1.388E-03
1.4118E-03
14.0000
1110.483
lU.!l72
113.40
3. 1211E-03
1.111111-02
5.148E-05
9.5112E-04
1 .011 E-03
57
IN
XIII
55
EO'
1.2110:a+01
IRYDI
N-'
3.15192
MU'
1.3808
E IRYD)
E (EV)
E PHOT lEV)
L.AM80A
CA)
(L./RI L. - 1 )
1L./R/L.+I)
SIGMA L. - 1
SIGMA L.+l
SIGMA IM8)
.0000
.000
175.!M8
70.153
.000
9.02I1E-02
.000
8.11113E-02
8.11113E-02
2.0000
27.212
202.780
81.15
.000
7 .• 79E-02
.000
7.1271-02
7.127E-02
18.0000
217.8118
3113.2.3
31. 53
.000
3.0821 -02
.000
2.317E-02
2.3171-02
IN
XIII
85
EO'
7.8.28E+00
IRYD)
N--
•. 15.20
MU-
1.3580
E (RYD 1
(EV)
1 PHOT
(EV)
L.AM8DA
lA 1
1L./R/L.-1)
IL./R/L.+I)
SIGMA L. - 1
SIGMA L. + 1
SIGMA (M8)
.0000
.000
1015.7011
Ile. III
.000
1.32I1E-Ol
.000
1. 18.E - 0 1
1.18.E-Ol
2.0000
27.212
133.1120
112.5.
.000
Il.7.8E-02
.000
7.11118E-02
7.1I118E-02
10.0000
1315.0511
2.2.7"
51 .07
.000
•. 25BE-02
.000
2.7eeE-02
2.78ee-02
IN
XIII
85
EO' 3.813I1E+00
IRYO)
N*=
15.85157
MU'
1.3.33
E 1 RYD)
E (EV)
E PHOT lEV)
L.AM80A
(A)
1L./R/L.-1I
(L./R/L.+ 1 )
SIGMA L.-!
SIGMA L.+ 1
SIGMA (M8)
.0000
.000
51 .8112
238.113
.000
2.3118E-Ol
.000
1.875E-Ol
1.875E-Ol
2.0000
27.212
711.10.
158.7.
.000
1.315E-Ol
.000
8.5111E-02
8.511IE-02
15.0000
81 .l535
133.528
92.85
.000
e.155E-02
.000
3.17I1E-02
3.179E-02
18.0000
217.8115
2811.587
.5.1111
.000
2.2181-02
.000
8.321E-03
e.3211-03
IN
XIII
lOS
EO' 2.2528E+00
IRYD)
N-'
8.8817
MU'
1.3383
E (AYDI
E (EV)
E PHOT (EV)
L.AM80A
(Al
(L./A/L. - 1)
(L./A/L.+ 1 )
SIGMA L. - 1
SIGMA L.+I
SlaMA
IM8)
.0000
.000
30.848
.0•. 55
.000
3.727E-Ol
.000
2.e75E-Ol
2.875E-Ol
2.0000
27.212
57.880
21 •. 211
.000
1 .• 73E-Ol
.000
7. 88BE -02
7.888E-02
8.0000
81.835
112.28.
110 .• 2
.000
5.515E-02
.000
2. '.8E -02
2.1.8E-02
10.0000
138.0511
1815.707
7 •. 37
.000
3.07IE-02
.000
Il.878E-03
Il.878E-03
18.0000
217.15115
2••. 3.3
.11.113
.000
1.7071-02
.000
•. 5.IIE-03
•. 5.9E-03
IN
XIII
125
EO'
1 .•8elE+00
IRYDI
N--
,0.158.,
MU'
1 .33811
E IAYD)
E 1EV)
E PHOT
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L.AM80.
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1L./AIL.+ll
SIGMA L. - 1
SIGMA
L. + 1
SIGMA (M81
.0000
.000
20.21'
813.21
.000
5.21171-01
.000
3.S85E-Ol
3.585E-Ol
2.0000
27.212
.7 .• 31
2151 .• 0
.000
1 .•1I.E -0 1
.000
8.e55E-02
e.855E-02
8.0000
81 .835
101.855
121.73
.000
•. 7.8E-02
.000
1 .•• 21-02
1 .•• 21-02
8.0000
'108.8.7
129.088
118.08
.000
3.32I1E-02
.000
8.9110E-03
8.1I110E-03
1•. 0000
1110.• 83
210.702
58.8..,
.000
l.e05E-02
.000
3 .• 11 E -03
3 .• ' 1E- 03
IN
XIII
185
EO' 7.8588E-Ol
IAYDI
N-·
1•. 88153
MU'
1.3337
E (AYD)
E (EV)
PHOT
lEV)
L.AM8DA
lAI
(L./AI L. - 1 )
lL./A/L.+I)
SIGMA L. - 1
SIGMA
L.+l
SIGMA
(M81
.0000
.000
10.8110
11511."
.000
Il.118E-Ol
.000
5.585E-Ol
5.5851-01
2.0000
27.212
37.1102
327.13
.000
1.3.3E-Ol
.000
•. 211.e - 02
•. 251.E-02
15.0000
81.835
1I2.32!5
13 •. 211
.000
3 .• 88E-02
.000
8.977E-03
8.977E-03
12.0000
183.271
173.11151
71.27
.000
1 . 335E -02
.000
1 . 9.IIE -03
1 .1I.IIE -03
IN
XIII
20S
EO' •. 8.III1E-Ol
IAYD)
N-.
18.8872
MU'
1.3328
E (AYOI
1
(EV)
PHOT lEV)
L.AM80A
lA)
(L./R/L.-l)
(L./A/L.+ 1 )
SIGMA L.-l
SIGMA
L. + 1
SIGMA
IM8)
.0000
.000
8.51111
187•. 11.
.000
1.3801+00
.000
7.1I02E-Ol
7.1I02E-Ol
2.0000
27.212
33.811
388.71
.000
1.13lE-Ol
.000
2.718E-02
2.718E-02
•. 0000
5 • . • 2 •
. , .022
203.18
.000
•. 575E-02
.000
8.025E-03
8.025E-03
8.0000
108.8.7
115 .•• &
107 .• 0
000
1.7321-02
.000
2. 177E-03
2.177E-03
IN
XIl 1
5P
10' '4.. 1812E+Ol
IRYD)
N-'
3.7828
MU'
1. 2 17.
E IAYD)
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IL./A/L.-1)
(L./A/L.+ Il
SIGMA L.-l
SIGMA L.+l
SIGMA IM8)
.0000
.000
180.707
77.15
Il.751E-02
Il. 05. E - 02
3.201E-02
5.51111-02
8.71I1E-02
2.0000
27.212
187.11111
85.1I8
7.571E-02
7.828E-02
2.25eE-02
•. 82.e-02
7.080E-02
10.0000
138.0511
21115.715&
.'.78
3.e03E-02
•. 8211-02
8.070E-03
2.88I1E-02
3.8I1eE-02
IN
XIII
ep
EO'
7.30&IIE+00
IAYD)
N-·
•. 80113
MU'
1 . 11107
E IRYD)
lEV)
E PHOT
(EV)
L.AM80A
lA'
IL./R/L.-l)
IL./A/L.+I)
SIGMA L. - 1
SIGMA L.+ 1
SIGMA (M8)
.0000
.000
1I11 .• 17
12 •. 71
1 . 5ellE -0 1
1.1531-01
5. 1OOE- 02
5.53.E-02
1.053E-Ol
2.0000
27.212
1215. 828
117.111
1 .051 E-0 1
li. 13l5i-02
2.1132E-02
• . • 28E-02
7.35eE-02
8.0000
108 .•• 7
208.215.
511.53
•. 8251-02
5.312E-02
Il.330E-03
2 .• 82E-02
3.3115E-02
18.0000
217.1585
3'7.111
38.10
2.308E-02
3.2201-02
3.5321-03
1.371l-02
1.731E-02
IN
XIII
8P
EO' 3.825I1E+00
IAYDI
N··
15.8271
MU'
1. 17211
E IAYD)
E lEV)
E PHOT (EV)
L.AM80A
lA)
IL./A/L-n
(L./A/L.+ 1 )
SIGMA L. - 1
SIGMA
L. + 1
SIGMA IM8)
.0000
.000
.11.333
251 .32
3.1.0E-Ol
1.87I1E-Ol
1.01I1E-Ol
5.830E-02
'1.8021-01
2.0000
27.212
78.545
'15 1 .118
1.51lE-Ol
1.0771-01
3.8eoE-02
3.718E-02
7.371E-02
8.0000
108.8.7
158. ,.0
78.38
•.• 781i-02
•. eS3E-02
e.e•• E-03
1·.35E-02
2.01lIlE-02
12.0000
183.271
212.804
58.32
2.7211E-02
3.23I1E-02
3.310E-03
Il.3.3E-03
1.2e5E-02
IN
XIII
10P
EO' 2.le58E+00
IAYO)
N-'
8.8335
MU'
1. 188lS
E 1 RYD)
E (EV)
E PHOT (EY)
L.AMIIOA
lA)
(L./R/L.-l)
IL./R/L.+I)
SIGMA L.-I
SIGMA L.+l
SIGMA (1'18)
.0000
.000
211 .• 158
420.75
5.21H-Ol
2.2251-01
l.e78E-Ol
8.1121-02
2.287E-OI
2.0000
2;.212
f1iS.8711
218.7lS
1.7.5E-Ol
1.120E-Ol
3.815E-c/2
2.1178E-02
e.5113E"C2
8.0000
81.1535
111. 103
111.80
5.81.E-02
5.0.111-02
7.338E-03
1.187E-02
1. 1I201-0Z
8.0000
108.8.7
138.315
811.84
3.878E-02
3.85.1-02
•. 3571-03
8.80111-03
t. 2117E-02
18.0000
217.8115
2.7.182
50. 18
1 .• 55E-02
1 .8541 -02
1.01171-03
3.S8tE-03
•. 857E-03
IN
XIII
12P
10·
1 .• 3I1tE+00
(AYD)
N-.
10.83815
MU'
1.183.
E (RYD)
1
1EV)
PHOT
(EV)
L.AM8DA
(A)
1L./R/L.-1)
1L./A/L.+I)
SIGMA L.-l
SIGMA L.+l
SIGMA (M81
.0000
.000
111.581
833.21
7.7531-01
2.782E-OI
2 .• 85E-Ol
8.3.111-02
3. 1OOE-0 1
2.0000
27.212
.15.7112
28•. 117
1. 80lE-Ol
1. 087E-Ol
3.17BE-02
2.318E-02
5 .• 98E-02
8.0000
8' .835
101.218
122.50
•. 888E-02
•. 27tE -02
5.0851-03
7.7331-03
1. 280E -02
1•. 0000
1110 .• 83
210.083
59. 02
1 .• IIIE-02
1.8118E-02
8.858E-0.
2.532E-03
3 .• '7E-03
58
IN XIII
ll1P
EO'
7.IIUllE-Ol
(RYDI
N••
14. 83ll'"
MU'
1 . 111011
E (RYD)
E ( EV)
E PHOl
(EV 1
l.AMIIDA
lAI
(l./R/L-I)
(L/R/L>I)
SIGMA l.-I
SIGMA L+l
SlaMA
1Mil )
.0000
.000
10.442
1187.3ll
1.41llE+00
3.ll22E-Ol
4.404E-Ol
Il.727E-02
5.077E-Ol
2.0000
21.212
37.1154
329.28
1.6418E-Ol
Il.33U-02
2 .• 4IE-02
1.31I1E-02
3.ll17E-02
4.0000
54.424
84.8118
Ul1.14
15. 55llE-02
4I.778E-02
5.U5E-03
15.203E-03
1.20llE-02
10.0000
1315.0159
148.501
.... 153
1 .1I43E -02
1.700E-02
8.282E-04
1.774E-03
2.1503E-03
115.0000
217.8ll5
228.137
54.35
7.7415E-03
Il.1501E-03
2.815I5E-041
8.810E-041
1 . 188E- 03
IN XIII
20P
EO- 4I.11510E-Ol
(RYD)
N••
18.84015
MU'
1.15941
E (RYD)
E lEV)
E PHOT (EV)
l.AMtSOA
(A)
(LIR/L-ll
(L/R/L+I)
SIGMA L- 1
SIGMA L+ 1
SIGMA (Mlli
.0000
.000
8.418
19141.03
2.23I5E"00
5.08BE-Ol
15.782E-Ol
7.02I5E-02
7.485&-01
2.0000
21.212
33.15.0
3118.03
1.401E-0.
7.70I5E-02
1.38llE-02
8.382E-03
2.223E-02
41.0000
ll4.4241
80.ll01
203. ll9
5. 132E -02
3.1574E-02
3.359E-03
3.4I44E-03
15.804(-03
8.0000
108.847
11ll .32ll
107.ll.
1.732E-02
1.1528E-02
7.2413E-041
1. 280E -03
2.004E-03
10.0000
1315.05.
142.537
115.••
1.201E-02
1.23llE-02
4I.352E-041
Il.110E-04
1.352E-03
IN XIII
40
EO'
1. 8414E-Ol
(RYDI
N·.
3.02ll5
MU'
.9705
E lRYDI
E ( EV,)
PHOT
i EV)
LAMIIDA
(A)
lL/RIL-I)
lL/R/L+11
SIGMA L- ,
SIGMA L+ 1
SIGMA 1Mll)
.0000
.000
250.535
4Ill.4Ill
4I.llI8E-02
1.155E-Ol
1. 523E -02
1.280E-Ol
1.41 12E-Ol
1.0000
13.808
2154.141
4115 .•'"
4.50I5E-02
i , 110E-0 1
1.348E-02
1.228E-Ol
1.38IE-01
41.0000
54.424
304.lltS8
410.1515
3.5417E-02
ll.713E-02
Il.1548E -03
i . 0.8E -0 1
1.1ll5E-Ol
8.0000
108.847
35ll.382
341.50
2. I5ll2E-02
8.22I5E-02
15.54I5E-03
s , 188E-02
•. 823t: - 02
IN XIII
50
EO' •. 91542E+00
IRYD)
N·.
41.1183
MU-
.8811
E lRYD)
1EV)
E PHOT (EV)
LAMtlDA
lA)
(l./R/L-l)
(L/R/l.+11
SIGMA L- 1
SlaMA
L+ 1
SlaMA
1Mil)
.0000
.000
135.512
lll.45
Il.2151E-02
1.27I1E-Ol
2.ll23E-02
8.324E-02
1. 125E-OI
1.0000
13.11015
149.178
83. II
7.888E-02
1.20U-Ol
2.333E-02
8.22IE-02
1.055E-Ol
Il.0000
81.1535
217.208
51.08
4. 181 E-02
8.884E-02
Il.542E-03
15.484E-02
7.4I18E-02
12.0000
1153.271
2118.843
41 1 .4ll
2.4I2IE-02
15.2ll4E-02
4I.4I03E-03
4.483E-02
4I.903E-02
IN XIII
150
EO'
15.381511E"00 (RYDI
N"
5.1441
MU'
. 85l1ll
E IRYD)
(EV 1
E PHOT (EV)
LAMBOA
(A)
<LlR/L-' }
IL/R/L-1 )
SIGMA l.' 1
SIGMA L+l
SlaMA
1M15)
.0000
.000
815.885
1412.158
1.485E-Ol
1.3811E-Ol
4I.81llE-02
15.28.E-02
1. 111 E-O 1
.5000
15.803
ll3.l5ll8
132.32
1.308E-Ol
1.343E-Ol
4I.028E-02
15.3158E-02
1.04l0E-Ol
.11000
8. 1841
ll5.05ll
130.413
1.27I5E-Ol
1.333E'-01
3.8ll2E-02
15.37IE-02
1.028E-OI
.7000
Il.524
1115. "'20
128.5ll
1.24I5E-Ol
i , 3241E -01
3.7152E-02
8.371E-02
1.013E-Ol
1.0000
13.11011
100.501
123.37
1.1111 E-0 1
i . 2ll5E -0 1
3.4I08E-02
15.351E-02
Il.75llE-02
15.0000
81.1135
1158.531
73.57
4.8141E-02
8.581E-02
Il.817E-03
41 .U8E -02
5.15157E-02
IN XIII
80
EO'
3.2ll50E"00 IRYDI
N"
7. 11517
MU-
.8383
E 1AYD)
E 1EV1
PHOT (EV 1
LAM8DA
(A 1
(L/R/L-ll
(l./R/L'"
)
SIGMA l. - 1
SIGMA L+l
SIGMA (Mil)
.0000
.000
4141.131
218. li 15
2.llI53E-Ol
1.4I87E-Ol
Il.8ll4E-02
3. 13U -02
1.3153E-Ol
.llOOO
12.245
57.077
217.23
1 . ll88E - 0 1
1.38U-Ol
ll.55l1E-02
4.151E-02
Il.70I5E-02
1.0000
13.8015
58.4137
212. Il
1. 8110E - 0 1
1.313E-OI
5.250E-02
4.15I5E-02
•. 4I05E-02
2.0000
27.212
72.043
112. 10
1.323E-Ol
1. 213E-Ol
3.172E-02
3.lIll4E-02
7 .• 88E-02
3.0000
40.818
85.l5d
144.78
Il.8415E-02
i . 08llE -0 1
2.087E-02
3. 88H - 02
5.751 E-02
15.0000
81.535
128.487
ll8.04
5. 034IE -02
7.4178(-02
a.01l5E-oa
2.158I5E-02
3.41IE-02
IN XIII
100
EO'
2.010IlE-00
(AYD)
Nu
Il.1882
MU'
.8318
E IRYDI
(EV)
PHOT (EV)
LAMIIOA
1A)
ILIAIL-ll
(LIA/L-l)
SI GllIA l.- 1
SIGMA L+ 1
SIGMA (Mill
.0000
.000
27.358
4153.241
41 . 887E -0 1
1.4I20E-OI
1. 842E -0 1
2.078E-02
1 . S50E -0'
.8000
a. 184
35.51.
34111.01
3.141E-Ol
1.427E-Ol
8.810E-02
2.12llE-02
1.154E-Ol
1.0000
13.8015
410.1182
302.8.
2.4158E-Ol
1.357E-Ol
II. 282E-02
2 .• ~5E-02
Il.10U-02
1.5000
20.40.
41.7115
25 •. 5a
1. all.E -0 1
1. 252E-Ol
4.327E-02
2. 822E -02
7. 14.E -02
2.0000
27.212
541.588
227.22
1.512E-Ol
1.14U-Ol
3.138E-02
2.71 1E- 02
5.841E-02
5.0000
88.030
1lS.3e5
129 .•8
5.191E-02
7. 13U -02
8.040E-03
1.833E-02
2.1537E-02
IN XIII
120
EO'
1.35412E-00 (RYD1
N·.
11. 1713
MU.
.8287
E tRYDI
E (EV)
PHOT lEV)
LAMtlDA
(A 1
( L/R/L-l1
1l./A!.L+l )
SIGMA l. - 1
SIGMA L+ 1
SlaMA
(M8)
.0000
.000
18.425
872.113
7.231E-Ol
1.188E-Ol
2.42IE-01
Il.805E-03
2.51I1E-Ol
.2000
2.121
21.148
'88.33
5.732E-Ol
1.325E-Ol
1.148E-Ol
1.3.lIe-02
1.eaU-Ol
.SOOO
8. 184
28.5eB
4158.32
3.8111E-Ol
1.381 E-Ol
1.012E-Ol
1.858(-02
1.111IE-Ol
1.0000
13.1508
32.031
387.08
2.131E-Ol
1.28llE-Ol
8.4I81E-02
2.00IlE-02
8.4I87E-02
1.5000
20.40ll
38.134
3111.21
2.044E-Ol
1.181E-Ol
4I.07I1e-02
1.lIll4e-02
Il.073E-02
2.0000
27.212
45.837
211. 88
1.552E-Ol
1.04llE-Ol
2.7153E-02
1.8ll2E-02
41 . 1555E -02
41.0000
54.41241
72. Ull
110.20
8.1I150E-02
1.103E-02
8.848e-03
1. 318E -02
2.270E-02
1" XIII
180
EO' 7.33.8E-Ol
(RYDI
N••
15.1742
MU'
.a2!!8
(
(RYQI
(EV)
E PHOT (EV)
LAMBDA
lAI
(l./R/l.-l)
(L/R/l.+I)
SIGMA L- 1
SlGIIIA l+1
SICMA (Mil)
.0000
.000
•. ll811
1241.57
1.312E-00
2. 5113E-02
4I.31.e-Ol
2. '31 E-04
4.321E-Ol
.2000
2.721
12.707
.,5.10
8.745E-Ol
9.039E-02
2.443E-Ol
3.915e-03
2.482(-01
.&000
8. 184
18. ISO
883.13
4.792E-Ol
I.lI10E-Ol
1. 041E -0 1
9.205(-03
1.13.e-Ol
1.0000
13.tl08
23.5.2
525.54
3.072E-Ol
1.100E-Ol
5.598E-02
I.071E-02
8.1575E-02
1.5000
20.4109
30.3l1!!
401.ll2
1.1I111E-Ol
Il. 88U -02
3.048E-02
1.010E-02
4.118E-02
2.0000
27.212
37. , ••
333.31
1.41 '4IE-OI
8.""8e-02
1.870E-02
Il.1I3I1E-03
2.8.,..E-02
3.0000
40.118
50.804
2441.05
8.287E-02
15.532E-02
8.770E-03
8.174E-03
I.894E-02
5.0000
81.030
7•. 018
15•. 9~
3.1152E-0%
4.3531-02
3.082E-03
5.57I1E-03
8.1537e-03
511
IN XIl 1
200
EO' •. 511112E-Ol (RYD)
N••
19.1755
MU'
.82.5
E IRYD>
E (EV)
E PHOT (EV)
LAMIIDA
(A)
(L/R/L-l)
(L/R/L-l)
SIGMA L- 1
SIGMA L-l
SIGMA
(Mil)
.0000
.000
Il.253
1982.118
2.053E+OO
-1.2110E-Ol
Il.1122E-Ol
3.7.5E-03
Il.1I110E-Ol
.01100
.8111
7.070
1753.7.
1.1171E-00
- •. 888E-02
•. 1I110E-Ol
Il.311I1E-0.
..III1I1E-Ol
.1000
1 .3111
7.111.
11128.38
1 .• 75E-00
- 1 . 351E -02
•. 111.E-Ol
5.2.'E-05
•. 1115E-Ol
.2000
2.721
8.1175
1381 .51
1.119E+OO
•. 185E-02
2.82.E-Ol
5.1128E-0.
2.830E-Ol
. 11000
8. Ill •
' •.• ,7
8110.00
s. 032E-0 1
9.581E-02
9.175E-02
•. 1I8I1E-03
9.117.E-02
1.0000
13.11011
111.8511
112•. 32
2.925E-Ol
9.172E-02
•. 271E-02
Il.2118E-03
•. 1I01E-02
1.5000
20 .• 011
211.11112
.115.02
1.172E-Ol
7.877E-02
2.10IlE-02
Il.238E-03
2.72I1E-02
2.0000
27.212
33 .• 1115
370 .•11
1.203E-Ol
Il.720E-02
1.21I1E-02
5.11118E-03
1.78I1E-02
3.0000
.0.818
.7.071
2113 .• 0
Il.III1I1E-02
5.0113E-02
5.30IlE-03
•. !I150E-03
Il.8110E-03
IN XIII
.F
EO'
1.3072E"01
(RYD)
N··
3.511511
MU'
.• 0••
E (RYD)
E lEV)
E PHOT (EV)
LAMI5DA
lAI
(L/R/L-l)
(L/R/L-l )
SIGMA L-l
SIGMA L- 1
SIQMA
(M151
.0000
.000
177.853
1111.71
3.517E-02
2.3118E-Ol
Il. 127E-03
3.580E-Ol
3.1I.2E-Ol
2.0000
27.212
205.01115
110 .• 11
2.78I1E-02
1.7118E-Ol
•. 287E-03
2.381E-Ol
2 .• 2.E-Ol
8.0000
108.8.7
2811.701
.3.25
1.517E-02
9.213E-02
1 . 7711E· 03
8.73I1E-02
8.1I1I1E-02
1•• 0000
1110 .• 83
3118.3311
33.1111
9 .• '0E-03
5 .• 1I0E-02
8.78.E-0.
3.118n-02
•. 075E-02
IN XIII
5F
EO' 7.1I081E-00 IRYD)
N••
•. 8228
MU'
.3172
E (RYD)
E (EV)
E PHOT lEV)
LAMIlDA
(A)
(L/R/L-l)
IL/R/L-l)
SIGMA L- 1
SIGMA L+l
SIG/IIIA
(Mill
.0000
.000
107.15117
115.23
7.28I1E-02
3.3.IIE-Ol
1.53I1E-02
•. 32I1E-Ol
•.• 80'E-Ol
2.0000
27.212
13 •. 8011
111.117
•. 8118E-02
2.31I1E-Ol
8.70IlE-03
2.511I1E-Ol
2.1183E-Ol
Il.0000
81.U!
1811.232
115.52
2.IIS.E-02
1. 2811E-Ol
3.5111E-03
1.12.E-Ol
1.1110E-Ol
8.0000
108.8.7
2111 .•••
57.28
2.070E-02
1.008E-Ol
2 .• 118E-03
7.1I05E-02
8. nl.E-02
111.0000
217.11115
_325.2111
38.12
Il.501 E-03
•. 1l115E-02
7.1I0n-0•
2.5.2E-02
2.1121E-02
IN XIII
IlF
EO' 5.3.0.E+OO (RYD)
N.·
5.525.
MU'
.37.11
E (RYD)
E (EVI
E PHOT
(EV)
LAMIIDA (A)
(L/R/L-f)
(L/R/L-l)
SIGMA L- 1
SIGMA L- 1
SIGMA (Mil)
.0000
.000
72.11111
170.~
1.217E-Ol
•. 331E-Ol
2.8117E-02
•. 811!11-01
5.1UE-Ol
2.0000
27.212
1111.873
12•. ,.
15.1150E-02
2.1188E-Ol
1.211I1E-02
2.587E-Ol
2.717[-01
•. 0000
5•.• 2.
127.01l!l
117.511
•. 512E-02
1.82I1E-Ol
Il.1187E-03
1.52I1E-Ol
1 . 51111E -0 1
Il.0000
81 .1135
.15•. 2117
80.311
3.1117E-02
1.32.E-Ol
•. 1118E.-03
Il.71!1E-02,
1.013E-Ol
10.0000
1311.0511
208. '1'20
511 .• 0
1.803E-02
7.83IE-02
1.827E-03
•. 511I1E-02
•. 17!tE - 02
1•. 0000
1110 .• 83
2113.1 ••
.7, 12
1.157E-02
5,1.0E-02
·11 .• 8.E-0.
2 .•llllE-02
2.5111E-02
IN XIII
8F
EO'
2.1I0113E-00 (AYD)
N··
7.112511
MU'
.37••
E (AYD)
E (EV)
E PHOT (EV)
LAMI5DA
(A)
(L/R/L-l)
(L/R/L-l)
SIGMA L- 1
SIGMA LOo 1
SIGMA
CMI5)
.0000
.000
311.!l.3
313.55
2.500E-Ol
Il.3 •• E-Ol
Il.1157E-02
5.71.E-Ol
Il.380E-Ol
2.0000
27.212
1111.7515
185.73
1.003E-Ol
3.0S1E-Ol
1.808E-02
2.23lE-Ol
2 .• '2E-0'
•. 0000
5•.• 2•
113.11117
131.115
5 .•• H-02
1.823E-Ol
7.50H-03
1.121E-Ol
1.1117E-Ol
Il.0000
81.635
121 . 1711
102.32
3 .• 2eE-02
1. 2111E-Ol
3. 83!1E-03
Il .• 70E-02
Il.U.E-02
12.0000
1113.271
202.lil.
III . 13
1.30!lE-02
5.12U-02
Il. 305E-0~
1.1I1!1E-02
2.008E-02
IN XIII
lOF
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9.11253
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(L/R/L-l)
SIQMA L- 1
SIG/IIIA L.. l
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(Mil )
.0000
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•. 153E-Ol
8 .• !II1E-Ol
1.153E-Ol
Il.373E-Ol
7.52I1E-Ol
2.0000
27.212
52.031
238.211
1.1S3E-Ol
3.080E-Ol
1.811~E-02
1. 173E-0 1
1.115I1E-Ol
•. 0000
5 •.• 2~
79.2~3
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5.~SIIE-02
1,1I57E-Ol
Il.3110E-03
7.808E-02
8 .• ~~E-02
8.0000
108.8~7
133.111111
ll2 . 711
2.01lIlE-02
7.211~E-02
1.582E-03
2.533E-02
2.1191E-02
10.0000
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1110.878
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1 .• 80E-02
5. 3~OE -02
Il. ~1l5E -o.
1.1I~7E-02
1.7.2E-02
1•. 0000
11110. ~83
215.302
57.51l
8 .• 7.E-03
3.235E-02
~, 1113E -o~
8.08111-03
8.50IlE-03
IN XIII
12F
10' 1.21505E-00 (RYD)
N•• 11.11251
MU'
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E CRYD)
E (EVI
E PHOT lEV)
LAMIlOA (A)
(L/A/L-l)
(L/R/L-l )
SICMA L-l
SIQ/lilA LOo 1
SIGMA (Mill
.0000
.000
17.0115
728.71
Il. I~H-Ol
1.0llIlE-00
1.731E-Ol
Il.1178E-Ol
8.70IlE-Ol
2.0000
27.212
~~.2211
280.3.
1.188E-Ol
2.113~E-Ol
1.11801-02
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1. 538E-0 1
•. 0000
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173.511
5.075E-02
1.~5111-01
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5 .• 37E-02
5.1132E-02
10.0000
1311.0511
153.07.
81.00
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•. 355E-02
Il .• 23E-0~
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12.0000
1113.271
180.285
118.17
Il. 1~3E-03
3.303E-02
•. 05U-0~
7. OIl~E -03
7 .• 11111 -03
IN XIII
ll1F
EO' Il.11223E-Ol
CRYDI
N·. 15.112~1
MU'
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1 (RYD>
E (EV)
E "HOT (EV)
LAMIlDA
(A)
(L/R/L-l1
CL/R/L-l)
SIGMA L-l
SIG/IIIA L-l
SIGMA
CM151
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Il.~18
13111.~2
1.108E"00
1.5152E+OO
3.11I1E-Ol
8. 1~!IE-Ol
1.1211E+OO
2.0000
27.212
311.1530
338.~8
1.08IlE-Ol
2,~7!1E-Ol
1.170E-02
8 . O!lU - 02
9.2251-02
~.OOOO
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113.842
11l~.21
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1. 10~E-Ol
2.8112E-03
2.7Il!ll-02
3.081i-02
8.0000
108. 8~7
118.21111
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1.32~E-02
•. 2~8E-02
5.58~E-0~
7.III1~E-03
8.223E-03
1~. 0000
1110.~83
11l1l.1I01
112.02
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1. 71111E -02
1,287E-0~
2.2~7E-03
2. 37SE -03
re . 0000
217 . IIIlI5
227.113
5~.!I11
3.812E-03
1 .• 1!lE-02
8.88eE-O!l
1.11331-03
1.722E-03
IN XIII
20F
EO- ~.3'81E-Ol
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N·. 111.112~8
MU'
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E IRYD)
E (EV)
E PHOT CEV)
LAMBDA
(A)
(L/A/L-l)
(L/R/L-l)
SIGMA L-l
SIG/IIIA Lo.I
SIGMA CMIl)
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5.1170
207e.1I8
1.721E+O,O
2.08~E+OO
~.7~E-01
Il.310E-01
1.407E+OO
2.0000
27.212
33.1'2
373.115
Il.31 lE -02
2.030E-Ol
7.7~8E-03
•. 1I11E-02
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•. 0000
5~ .• 2~
1I0.31l~
2015.30
3.23I1E-02
8.!lIQE-02
1 _703E-03
1.57~E-02
1.7~~E-02
Il.0000
81.1135
87.1I0e
1~1.53
I.II!1lE-02
•. 8~ lE -02
Il .• 3~E-0~
7.372E-03
8.01I1E-03
12.0000
1113.271
11111.2.1
73.211
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1.6118E-02
1. OIlOE - O~
1.11111 E-03
1 . 7117E -03
1~. 0000
11l0.483
11I1I.d3
113. 11
3.1118E-03
1.2113E-02
Il.112I1E-0!l
1.17IlE-03
1.2.8E-03
110
SN XIV
55
EO-
1.~527E-Ol
(RYD)
N··
3.11732
MU·
1 .32118
E (RYD)
E CEV 1
E PHOT (EVI
LAMBDA (A)
CL/AIL-l)
(L/R/L+I)
SIGMA L- 1
SIGMA L+ 1
SlaMA
CMil)
.0000
.000
11'7 .1I~7
112.73
.000
8. 185E-02
.000
8.320E-02
a.320E-02
2.0000
27.212
22~.8511
55. 1~
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Il .1I0~ E-02
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B.73I1E-02
Il. 7311E-02
20.0000
272.118
~ 1111 . 7SIS
211.311
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2.!l3I1E-02
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r . 8118E-02
1. 11I8E -02
SN XIV
liS
EO· 8.81113E-00 ( RYDI
N··
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MU·
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SlaMA L+ 1
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1 . Oll~ E-0 1
1 . OIl~E -0 1
2.0000
27.212
1~8. 1811
83.B7
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Il.082E-02
.000
7.1180E-02
7.1180E-02
12.0000
163.271
2a~ . 2~!l
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.000
3.1I~8E-02
.000
2.377E-02
2.377E-02
SN IllV
as
EC. ~.3!s~IE-00 ( RYDt
N··
Il.70113
MU'
1.21107
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E (EV)
E PHOT (EV)
LAMBDA (AI
(L/R/L-Il
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SIGMA L- 1
SlaMA L+l
SlaMA
CMB)
.0000
.000
!l1l.2~2
2011.211
.000
2.1!lIlE-Ol
.000
1.730E-Ol
1.730E-OI
2.0000
27.212
811.~!l3
1~3.~1
.000
1.2!l~E-Ol
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8.!l!lOE-02
a.!lIlOE-02
Il.0000
81.113!l
1~0.877
88.01
.000
Il. ll1llE -02
.000
3. 31111E.- 02
3.311I1E-02
111.0000
217.lIl1S
2711.11311
~4.77
.000
2.300E-02
.000
Il.20IlE-03
Il . 2 OllE- 03
SN XIV
lOS
EO. 2.!l810E-00 ( RYDI
N··
8.7143
MU·
1.28!l7
E (RYD)
E (EV)
E PHOT (EV 1
LAMBDA (AI
CL/R/L-l)
(L/R/L+1 )
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
3!l. 117
353.011
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3.3~3E-Ol
.000
2.~III1E-Ol
2.4I1SE-Ol
2.0000
27.212
112.3211
l11B.1I2
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1.~~IE-Ol
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a.13I1E-02
a.13I1E-02
Il.0000
81.113!l
1111.7!l3
1011.20
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2.3112E-02
2.3112E-02
12.0000
1113.271
1118.388
112.!l0
.000
2.!lalE-02
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8.30!lE-03
8.30!lE-03
SN XIV
12S
EO- 1.701lIlE-00 ( RYDI
N·· 10.71S11
MU·
1.2834
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E (EV)
E PHOT (EV)
LAMBDA (A)
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SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
23.210
533.lI11
.000
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.000
3.2BIIE-Ol
3.28I1E-Ol
2.0000
27.212
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7.088E-02
7.088E-02
Il.0000
81 . 113S
10~.8!l8
118. 2~
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1.112I1E-02
1 . 11211E - 02
10.0000
1311.0511
1!l1l.2711
77.8~
.000
2.1I!l4E-02
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7. 0!l1 E-03
7.0111 E-03
SN XIV
ll1S
EO· Il.0~72E-Ol
(RYD)
Ne:
1~. 7188
MU·
t .2812
E (RYDI
E (EV)
E PHOT (EV)
LAMeDA
(A)
(L/R/L-T)
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SIGMA L- 1
SIGMA L+l
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.0000
.000
12.310
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.000
8.180E-Ol
.000
5. 1!l1 E-Ol
!l. 1!l1 E-Ol
2.0000
27.212
311.521
313.72
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1.3110E-Ol
.000
4.711I1E-02
~. 7l1llE-02
1.0000
81.113!l
1I3.1I~5
131.118 .
.000
3.710E-02
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8. 127E -03
8.127E-03
12.0000
1113.271
17!l.!l81
70.112
.000
1 . 4~OE-02
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2.28I1E-03
2.28I1E-03
SN XIV
20S
EO' !l.!l1l32E-Ol
(RYDI
N··
18.71117
MU·
1.2803
E (RYD)
E (EV)
E PHOT (EVI
LAMBDA
(A)
(L/R/L-l)
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA (MIl
.0000
.000
7.1110
111211.24
.000
1.23I1E-00
.000
7.2112E-Ol
7.2112E-Ol
2.0000
27.212
34.822
3511.011
.000
1.II1I1E-Ol
.000
3.128E-02
3.128E-02
4.0000
!l~.~2~
112.034
11111.87
.000
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.000
Il.~~IE-03
a. 441 E- 03
8.0000
108.847
1111. ~!l7
1011.411
.000
t .87I1E-02
.000
2.!l83E-03
2.583E-03
SN XIV
!lP
EO'
1.3312E"01
(IIYD1
Naa
3.8300
MU-
1.1700
E (AYD)
E (EV)
E PHOT (EV)
LAMBDA (AI
(L/R/L-t)
(L/R/L+ 11
SIGMA L- 1
SIGMA L+ 1.
SIGM... (MB)
.0000
.000
181.71111
118.20
8.!l4lSE-02
8. 5aH -02
2.78IE-02
!l.!l73E-02
8. 354E-02
2.0000
27.212
2011.011
!l1l.32
Il.81I1E-02
7.454E-02
2.034E-02
4.811I1E-02
Il.1I00E-02
8.0000
108. 8~7
2l10.11~7
~2.1I11
3.1187E-02
5.222E-02
Il.117111-03
3.321E-02
~. 2811E-02'
18.0000
2~~.1I011
4211.70'
211.00
2. 128E-02
3.31I1e-02
4.0~IIE-03
t .III1I1E-02
2.373E-02
SN lliV
IIP
EO· 8.3132E"00 (RYDI
N··
~ . USII
MU-
1. 1~~~
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA (A)
(L/R/L-II
(L/R/L+I)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
113.108
1011.112
1.311I1e-Ol
r , 101 E-O 1
~.422(-02
!l.7~~E-02
1.017E-OI
2.0000
27.212
1~0.320
88.311
'.!l81E-02
a . u 1E-02
2.11118E-02
4.!lll5E-02
7.2113E-02
8.0000
101.847
221 .lIlS!l
5!l.811
~.4111E-02
5. 2811E-02
a.378E-03
2.5118E-02
3.5311(-02
111.0000
217.119!l
330.803
37.~8
2.318E-02
3.2I1U-02
3.722E-03
1.47SE-02
1.8~8E-02
SN XIV
8P
EO. ~. 1492E-00 ( RYDI
".. Il.8730
MU·
1.1270
E (IlYD)
E lEV)
E PHOT (EV)
LAMBDA
(A)
IL/R/L-I)
(L/R/L+I)
SIGMA L-l
SIGMA L"1
SIGMA (MB)
.0000
.000
!l1l.483
. 2111.113
2.72IE-Ol
1.113I1E-Ol
8.808E-02
S.333E-02
1.5 14E-0 1
2.0000
27.212
83 .1I11!l
148. III
1.417E-Ol
1.074E-Ol
3.520E-02
~.0~3E-02
7. 5UE- 02
1.0000
108.1147
111!l.301
75.01
4.!l2I1E-02
~.7113E-02
7.0112E-03
1.5111E-02
2.300E-02
14.0000
1110.~83
2411.11311
50.21
2.305E-02
2.102E-02
2.74IE-03
8.710E-03
1.14I1E-02
SN XIV
10P
EO. 2. 48110E-00 (RYDI
N.·
8.87113
MU·
1.1207
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA (A)
( L/R/L-I)
(L/R/L"1 )
SIGMA L-l
SIGMA L-l
SIGMA (Mil)
.0000
.000
33.82~
3110.!l1l
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2.20IlE-Ol
1. ~47E-Ol
Il.1115E-02
2.138E-Ol
2.0000
27.212
111.0311
203. 1~
1.1184E-Ol
1. l~al-Ol
3.112!lE-02
3.3118E-02
Il . lUlU - 02
Il.0000
81 . 113!l
11!l.~80
107.3a
5. 7!l1 E-02
!l.2I1U-02
8.000E-03
1 . 3!lIlE -02
2.1!lIlE-02
8.0000
108.8~7
142.1172
811.110
4.022E-02
~.01l0e-02
4. 833E -03
Il.853E-03
1.~III1E-02
111.0000
217.1I11!l
2!l1 . !l111
411.30
1.54\\E-02
1 .1I115E -02
1.252E-03
~. 070e-03
!l.322E-03
18.0000
2~~.1I011
27a.731
4~.48
1.211I1E-02
1 . 720E -02
Il.a03E-0~
3.4!!lE-03
~.43!lE-03
81
SN XIV
12P
EO'
1.8551 E+OO (RYOl
N··
10.8823
MU'
1.1177
E (RYO)
E (EV)
E PHOT (EV)
LAM80A (A)
(L/R/L-l )
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
22.51;
550.5;
8.715E-Ol
2.812E-Ol
2.127E-Ol
7.457E-02
2.872E-Ol
2.0000
27.212
49.730
24;.32
1.780E-Ol
1.140E-Ol
3.302E-02
2.70eE-02
8.001E-02
8.0000
81.535
104.154
11;.04
5.102E·02
4.554E-02
5.880E-03
;.04;E-03
1.473E-02
12.0000
183.271
185.7;0
ISIS. 73
1 .; 11 E-02
2.188E-02
1.422E-03
3.8S7E-03
5.079E-03
18.0000
217.81JS
240.213
51.82
1.238E-02
1.552E-02
7. 88;E-04
2.424E-03
3. 1;3E-03
SN XIV
18P
EO' 8 .... 82E·Ol
(RYO)
N··
14.8851
MU'
1.1149
E (RYO)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L·,)
SIGMA L- 1
SIGMA L-l
SIOMA (MB)
.0000
.000
12.0S8
10S0.13
1.227E-00
4.0;SE·01
3.797E-Ol
8.457E-02
4.043E-Ol
2.0000
27.212
3;.248
3,5.;,
1.888E-Ol
1.011 E-0 1
2.342E·02
1. 882E -02
4.02SE-02
4.0000
54.424
88.480
188.58
8.;17E-02
5.198E-02
8. 1SIS1E -03
7.518E-03
1.418E-02
8.0000
108.847
120.883
102.57
2.502E-02
2.403E-02
1.585E-03
2.923E-03
4.508E-03
10.0000
138.05;
148.0;8
83.72
1.771E-02
1 . 8411E-02
;.72eE·04
2. 111 E-03
3.084E·03
14.0000
1;0.483
202.51;
81.22
1.03;E-02
1 . 225E -02
4.584E-04
1.273E-03
1.731E-03
18.0000
244.;08
258.;42
48.25
8.U5E·03
8.955E-03
2.588E-04
8.831 E-04
1.122E-03
SN XIV
20P
EO' 5.4;150E-Ol
(RYDl
N··
18.8882
MU'
1.1138
E (RYD)
E (EV)
E PtlOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+')
SIGMA L- 1
SlaMA L+l
SIGMA (MBI
.0000
.000
7.478
1858.37
1. ;32E-00
5.475E-Ol
5.8415E-Ol
; . 388E -02
8.784E-Ol
1.0000
13.500
21.012
588.11
3.401E·01
1 . 5;5 E- 0 1
!l.107E-02
2.2471!-02
7.S54E-02
4.0000
54.424
81.;00
200.S0
15.4;4E-02
4.050E-02
3.;14E-03
4.254E-03
8.188E-03
8.0000
108.847
118.324
108.5;
1.877E-02
1. 783E -02
8.584E-04
1.54;E-03
2.407E-03
12.0000
103.271
170.747
72.81
;.757E-OS
1.078E-02
3.405E-04
8.310E-04
1.172E-03
SN XIV
40
EO' 2.0853E+Ol
(RYOl
N··
3.0858
MU'
.;342
E (RYO)
E (EV)
E PHOT (EV)
LAMIDA
(A)
(L/R/L-l)
(L/R/L-l)
SlaMA L- 1
SIOMA L+l
SI aMI.
(MB)
.0000
.000
283.730
43.70
4.283E-02
1.074E-Ol
1.308E-02
1.234E-Ol
1.381E-Ol
2.0000
27.212
310.;42
3;.87
3.878E-02
; . U7E-02
1.0581-02
1.1481!-01
1.2114E-Ol
4.0000
54.424
338.154
38.87
3.1UE-02
;.107E-02
8. 888.- 03
1.0117E-Ol
1 . 144E -0 1
8.0000
81.835
3811.30S
33.;3
2.803E-02
8.383E-02
7.2141-03
1.080E-02
1.040E-Ol
SN XIV
50
EO'
1.137IE+0'
(RYO)
N··
4.1503
MU'
.84;7
E (RYO)
E (EV)
E PHOT (EV)
LAMIOA
(A 1
(L/R/L-l)
( L/R/L+\\)
'SIOMA L- 1
SIGMA L+l
S1Q/U
(M8)
.0000
.000
1!l4.820
80 .•08
8.082E-02
1.235E-Ol
2.542E-02
8.908E-02
1.141lE-Ol
2.0000
27.212
182.032
88. 11
Il.14IE-02
1.015E-Ol
1 . 730E -02
8.225E-02
1.;85E-02
S.OOOO
8 1 .1135
238.4511
!l2.44
3.941 E-02
8.580E-02
SI.233E-03
S.583E-02
7.488E-02
14.0000
1S10.483
345.303
3!l.ll
2.053E-02
5.57S1E-02
3. &!l8E-03
4.0153E-02
4.41;E-02
SN XIV
110
EO'
7.3177E-00
(RYOI
N··
5. 1784
MU'
.824S
E (RYD)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+I)
SIC/U L- 1
SlQMA L+l
SlaMA
(M8)
.0000
.000
;9.514
124.53
1.2117E-Ol
1.311E-Ol
4.211 E-02
7.2S7E-02
1.148E-OI
2.0000
27.212
12S.77S
Sl7.80
8.1I03E-02
1.178E-Ol
2.35;E-02
8.830E-02
8.Sl8;E-02
8.0000
81 . 8:15
181.1;;
88.43
4.888E-02
8.48IE-02
SI.SllSI!-03
4.;23E-02
5.;I!lE-02
12.0000
183.271
2112.835
47.17
2.480E-02
5.823E-02
3.SlS81-03
3. 134E-02
3.530E-02
SN XIV
80
EO' 3.7887E-00 (RYD)
N··
7.1;28
MU'
.8074
E (RYO)
E (EV)
E PHOT (EV)
LAMIDA
(A l
(L/RIL-l)
(L/R/L-I)
SIGMA L- 1
SI aMI. L-l
SIOMA (MS)
.0000
.000
51.548
240.53
2.510E-Ol
1.S2;E-Ol
8.8S14E-02
5.157E-02
1.385E-Ol
.2000
2.721
54. ZSSI
228.47
2.374E-Ol
1.5S121-01
7.887E-02
5.18U·02
1 . 287E -0 1
.3000
4.082
5!l.830
222.88
2.278E-OI
1.573E-Ol
7.244E-02
5.18U-02
1.243E-Ol
.4000
5.442
!5lS.tSlO
217.88
2. 184E-0 1
'.5113E-Ol
8.838E-02
5.183E-02
1.202E-Ol
1.0000
13.S08
S5.1!l4
1;0.30
1.73IE-Ol
1.433E-Ol
4.Sl551!-02
5.0481!-02
1.0001!-01
8.0000
81 .835
133.184
;3.0;
5.010E-02
7.8501-02
8.874E-03
2.UIE-02
3.807E-02
12.0000
183.271
214.81S1
87.72
2.211E-02
4.478E-02
2.8311-03
1.823E-02
1.887E-02
20.0000
272.118
323.888
38.31
1 .071 E-02
2.8751!-02
;.3311-04
8.734E-03
SI. 888E -03
SN XIV
100
EO' 2.3182E+00 (RYD)
N··
;.1;;0
MU'
.B010
E (RYD)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L·,)
SIGMA L- 1
SIGMA L-l
SIQMA (MB)
.0000
.000
31.1114
3;3.43
4.275E-Ol
1.753E-Ol
1.448E-Ol
3.852E-02
1.813E-Ol
.4000
5.442
38.1117
335.4S1
3.284E-Ol
1 .858E-0 1
9.U7E-02
3.82S1E-02
1.373E-Ol
.8000
8.803
38.317
323.58
3.0701!-01
1. 82;l!-0 1
1.0781!-02
3.83n-02
1.2;IE·Ol
.8000
8. 184
3; .•78
312.48
2.813E·01
1.800E-Ol
8.3481-02
3.831E-02
1.218E-Ol
1.0000
13.808
411.120
274.7;
2.32IE·01
1.483E-Ol
8. 1301!-02
3.741E-02
SI.871E-02
8.0000
81.835
113.150
101.58
4.781E·02
8.545E-02
8.5011!·03
1 . 8UE -02
2.4781!·02
12.0000
183.271
1S14.785
83.115
1 .848E-02
3.533E-02
1 . 8731! -03
SI. 18;E '03
1.084E-02
18.0000
217.8S15
2411.20;
4;.78
1.1;8E-02
2.808E·02
8. ;881! '04
8.383E-03
7.27;('03
SN XIV
12D
EO'
1.881.E-00 (RYD)
N··
11.2021
MU'
.7lJ711
1
(RYO)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L- 1 )
SIQMA L'1
SIGMA L+l
SIQMA 1MB)
.0000
.000
21.251
1183.43
8.331E·01
1.787E-Ol
2.1411'01
2.502E·02
2.3.,E·01
.8000
8.803
28.084
441 .15
3. Sl57E -0 1
1.1SIllE-Ol
1.104E-Ol
2.884l-02
1.3UE-Ol
.8000
8. 184
2;.415
421.51
3.852E-Ol
1.815E-Ol
1.881E-02
2. U2E -02
1.275E-Ol
.7000
;.524
30.778
402.87
3.382E-Ol
1.57n·01
8.84IE-02
2.887E-02
1.174E-01
1.0000
13.1108
34.857
3811.70
2.737E-Ol
1.4115E·01
Il.583E-02
2.821E-02
SI.384E-02
4.0000
114.424
78.875
163.1Ô4
7.244E·02
7.51IE·02
; .Ia a'03
r , 848E -02
2.84I1E-02
8.0000
81.835
102.887
120.51
4.282E·02
15.5211!·02
4.875E-03
1.185E·02
1.182E·02
8.0000
108.847
130.011
15.30
2.823E·02
4.284E-02
2.808E·03
8.llIE-03
1.153E-02
14.0000
110.483
211.734
58.58
1 . 1181! '02
2.3.21!-02
7 . 831E - 04
4.51'E-03
5.333E-03
52
SN XIV
f50
EOa 8.477I1E-Ol
IRYO)
N·a
15.20411
MU-
.71151
E (RYOI
E (EV)
E PHOT (EV)
L...MSD ... (A)
(I.IRII.-I)
(L/R/L+l)
SIaM... L'1
SIaM... L+l
SIaM'"
(MSI
.0000
.000
11.535
1074.87
1.150E+00
1.481E-Ol
3.832E-Ol
Il.534E-03
3.1128E-Of
.1000
1.351
12.811S
118f .47
II. 5211E - 0 1
1. 5110E -01
2.1143E-Ol
1.22I1E-02
3.08SE-Ol
.8000
I.1U
111.81111
5211.42
4.85I1E-Ol
1.521E-Ol
1.075E-Ol
1.718E-02
1.247E-Ol
.7000
Il.524
21.0511
1588.7!
4. 181 E-Ol
1.473E-Ol
9.183E-02
1.723E-02
1.08I1E-Ol
.8000
10.885
22.420
553.02
3.7 .. 1E-Ol
1.425E-Ol
7.888E~02
1.71!E-02
Il.80'' E-02
1.0000
13.808
25.1"1
4113.17
3.080E-Ol
1.32I1E-Ol
5.11114E-02
1 . 873E -02
7.887E-02
".0000
54."24
85.1511
117.118
5.8115E-02
5.753E-02
5.781E-03
8.230E-03
1. 31111E -02
10.0000
138.0511
147.511"
8".00
1 ... 48E -02
2.384E-02
7.757E-0"
3. IllE -03
3.887E-03
18.0000
21'7.885
2211.230
5" .011
8.838E-03
1.377E-02
2.538E-04
1.83I1E-03
1. 8113E -03
SN XIV
200
EO-
5.3134E-Ol
(RYO)
N··
111.2081
MU-
.711311
E (RYO)
E (EV)
E PHOT (EV)
L...M8ll... f"')
(I.IR/L-l)
(L/VL+ 1 )
SIaMA
L- 1
SIaM'" L+ 1
SIaM... (M8)
.0000
.000
7.2211
1715.02
1.801E+00
7.II!17E-02
5.8112E-Ol
1.728E-03
5.1I0IlE-Ol
.2000
2.721
Il.1151
12"8.02
1 . 052E +00
1. 388E-Ol
2.770E-Ol
7.228E-03
2.842E-Ol
.5000
8.803
14.032
883.57
5.8113E-Ol
1."07E-Ol
1.225E·01
1.047E-02
1.32I1E-Ol
.8000
1.18"
15.3113
805.47
5.03I1E-0\\
1.382E-Ol
II. 82 .. E·02
1.078E-02
1.01l0E-Ol
.7000
Il.52''
18.754
740.08
".388E-Ol
1.310E-Ol
8. 028E -02
1.084E-02
Il. Il t E-02
.8000
10.885
18.11"
81".47
3.824E-Ol
1.257E-Ol
6.880E-02
1 . 0711E -02
7. 7311E-02
1.0000
13.808
20.835
5115.08
3.018E-Ol
1.154E-Ol
".783E-02
1 . 045E-02
15.80IlE-02
2.0000
27.212
34 ..... 1
3511.1111
1.210E-Ol
7.771 E-02
1."18E-02
7.842E-03
2.202E-02
4.0000
54.42"
81.853
201.10
".8111E-02
..... 32E-02
3. "2IE-03
".588E-03
7.1187E-03
'.0000
101.847
111.077
108.81
1 .581 E- 02
2.220E-02
7.108E·04
2. 15SE -03
2.887E-03
1".0000
1110."83
1117.712
82.71
6. 103E -03
1.172E-02
1.851E-0"
1 . 024E-03
1.208E-03
SN XIV
4F
EO-
1.5130E+Ol
(AYO)
N.·
3.511112
MUa
... 001
E (RYO)
E (EV)
E PHOT (EV)
L...MBo... (A)
(L/RII.-l)
(L/A/L+l)
SiaM... L- 1
SIliM... L+l
SiaM... (MSI
.0000
.000
205.158
80.23
3.128E·02
2.01I1E-Ol
5,"23E-03
3.012E·01
3.0seE·01
2.0000
27.212
233.071
53.20
2.508E-02
1.585E-Ol
3.1I"3E-03
2.103E-Ol
2.1"2E-Ol
8.0000
108.8"7
314.707
38 ... 0
1 ..... 3E -02
'.888E-02
1.788E-03
8.528E-02
8.702i-02
1".0000
1110.483
3118.342
31.28
Il.274E-03
5.3112E-02
9. 180E-04
4.138E-02
".22I1E-02
SN XIV
5F
EO-
Il.1501E+00
(AYO)
N··
4.8282
MU'
.3718
E (AYO)
E (EV)
E PHOT (EoV 1
L...MSO... (A)
(L/A/L'- 1 )
(L/A/L+l)
SiaM... L- ,
SIOM ... L+l
SiaM... (MS)
.0000
.000
12".4118
1111.511
8."34E-02
2.882E-Ol
1.38BE-02
3.714E-Ol
3.853E-Ol
2.0000
27.212
151.708
Bl.73
".522E-02
2.083E-OI
8.358E-03
2.383E-Ol
2."47E-Ol
8.0000
108.847
233.3"3
53.13
2.0521-02
9.787E·02
2.8 .. 7E-03
8.025E-02
8.2110E-02
18.0000
2f7.81l5
3 .. 2. 1111
38.23
Il. 8311E-03
".780E-02
8.1I21E-0"
2.78"E-02
2.874E-02
SN XIV
8F
EOa 8. 1803E+00 (AYO)
N··
5.8315
MU'
.388'
E (AYO)
E 1EV)
E PHOT (EV)
L...MBO ... (A 1
(L/A/L-ll
(L/A/L-' )
SIaM... L - 1
SI DM'" L+l
SIaM ... (M81
.0000
.000
U.0811
1.. 7."5
1.078E-Ol
3.750E-Ol
2.833E-02
".248E-Ol
".510E-Ol
2.0000
27.212
111.301
111 ... 0
8.554E-02
2 ... 55E-Ol
1 . 287E -02
2."08E-Ol
2.537E-Ol
4.0000
5 ..... 2..
138.513
811.51
..... 1.. e-02
1.732E-Ol
7.288E-03
1."1l2E-Ol
1.585E-Ol
8.0000
".835
185.124
74 .81
3.178E-02
1.287E-Ol
".501E-03
Il.858E-02
1.031E-Ol
12.0000
183.271
2"7.380
50.12
1."1I3E-02
8.31lIlE-02
1."8I1E-03
3.837E-02
3.788E-02
18.0000
217.811!1
301.784
"1.01
1 . 0 I .. E -02
......... e·02
8.38"E-0"
2.1"01-02
2.22"E-02
SN XIV
8F
EO. 3.38"IIE+00 (RYOl
N··
7.8321
MU'
.38711
E (RYO)
E (EV)
E PHOT 1EV)
L...M8D... ( ... )
(I.IA/L- 1)
(I./A/I.+ 1)
SIOMA 1.-1
SIaM... L+l
SIaM... (Mel
.0000
.000
.. s. 7&:3
270.82
2.227E·Ol
5.531E-Ol
6.118E-02
5.030E-Ol
5.8"2E-Ol
2.0000
27.212
72. IlIl''
181l.88
Il.81li1E-02
2.87a-Ol
1.8li15E-02
2.1S0E-Ol
2.350E-Ol
".0000
54."2"
100.208
123.73
5.581E-02
1.7."E-Ol
8.3"5E-03
1 . 1"5E-0 1
1.22I1E-Ol
8.0000
81.835
127."18
117.31
3.585E-02
1.223E-Ol
..... 0111 - 03
8.8 .... 1-02
7.2851-02
14.0000
180."83
231.285
52.48
1.118E-02
".327E-02
7.1123E-0"
1.588E-02
1.887E-02
18.0000
2"4.1108
2li10.8811
"2.85
7. "3IE-03
2.1183E-02
".323E-0"
Il. 288E-03
Il.71I1E-03
SN XIV
lOF
EO-
2.1128E+00
(AYOI
N.a
Il.8320
MU'
.3880
E (AYD)
E (EV)
E PHOT (EV)
I....MBO ... ( ... )
(I./A/L-l)
( I./R/I.+1)
SIaM... L-l
SIOM ... 1.+1
SIaM... (MSI
.0000
.000
28.7 ....
"31.34
3.714E-Ol
7."lIE-Ol
1.0881-01
5.870E-Ol
8.737E-Ol
2.0000
27.212
!I5.lIse
221.58
1.185E-Ol
2.1172E-Ol
2.0"7E-02
1.775E-Ol
1.1I7I1E-Ol
".0000
5 ..... 2 ..
83.188
'''11.08
5.7"5E-02
1.880E-Ol
7.3li12E-03
'.227E-02
•. lIe8E-02
8.0000
108.847
137.5112
110. 1 1
2.280E-02
7.55IE-02
1.1127E-03
2.817E-02
3.00IlE-02
12.0000
183.271
lli12.015
84.57
1.214E-02
... 3311E-02
7.820e-04
1.2118E-02
1.374E-02
1".0000
1110.483
2111.227
58.58
Il. "01E-03
3.455E-02
5.218E-0"
Il.3115E-03
8.1117E-03
20.0000
272.118
300.8S3
"1.21
5.0"21-03
1 .1I87E -02
2. 051lE -0"
4. 1711E-03
".385E·03
SN XIV
12F
EOa
1 .....88E +00
IRYDI
N··
Il.83111
MU'
.3881
E (RYO)
E (EV 1
E PHOT (EV)
LAM80'"
(A)
(I./A/L-l)
(L/A/L+l)
SiaM... L-l
SIaM... L+l
SlaMA
(MB)
.0000
.000
111.710
lS211.05
5.51"E-OI
Il.404E-Ol
1.81"E-Ol
8.280E-OI
7.873E-Ol
2.0000
27.212
"8.1122
2~.2"
1 . 231 E-O 1
2.88I1E-Ol
1.1114E-02
1.408E-Ol
1.5117E-Ol
4.0000
54.424
7".13"
187.25
5."55E-02
1 . "831-01
5 .UIE -03
5.8571-02
8.451E-02
10.0000
138.0511
f55.7811
7li1.80
1.388E-02
".823E-02
8.078E-04
1.1I1U-02
1.278E-02
12.0000
183.271
182.1181
87.78
1.021E-02
3.534E-02
5.1"IE-0"
8.20<lE-03
8.718E-03
20.0000
272.118
2111.828
42.411
... OllllE - 03
1.583E-02
1. 32 1E-0<1
2.55I1E-03
2.8111E-03
SN XIV
18F
EOa 8.0212E-Ol
(RYO)
N··
15.8317
MU'
.3883
E (RYO)
E (EV)
E PHOT (EV)
L....1I0... ( ... )
(L/R/L-l)
(L/R/I.+ 1)
SiaM... L-l
SlaMA L+l
SIGMA
(MS)
.0000
.000
10.1114
1138.07
Il.1I110E-Ol
1.374E+00
2.1133E-Ol
7."00E-Ol
1 . 033E +00
2.0000
27.212
38.125
325.21
1.18I1E-Ol
2.507E-Ol
1 ... 02E -02
8.803E-02
1.001E-Ol
".0000
5" ."2"
115.337
1811.78
..... liIIIE-02
1.1"IlE-Ol
3.582E-03
3.0115E-02
3 ... 51 E-02
8.0000
101.8.. 7
1 1liI . 781
103.53
1."87E-02
... 528E-02
7. 131 E-04
8.8 Il E-03
Il.524E-03
12.0000
183.271
174.185
71.18
7.332E-03
2. <l54E-02
2.522E-0"
3.78ae-03
4.020E-03
18.0000
2..... 1108
255.820
"8."7
3."71E-03
1 . 288E-02
8.2118E-0!\\
1."73E-03
1.558E-03
SN XIV
20F
EO·
5.0855E-Ol
(AYD)
N··
19.5317
MU·
.3583
E ( IlYDI
E (EV)
E PHOT (EV)
LAMBDA
lA)
(L/A/L-I)
(L/A/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
8.ala
17al.88
1.557E+00
1.8504E+00
".517E-Ol
8.5"lE-Ol
1 . 308E.00
2.0000
27.212
3".131
383.215
1.021E-Ol
2.0a3E-Ol
9.575E-03
5.371E-02
5.328E-02
".0000
5" ... 2 ..
81.3"3
202. 12
3.51aE-02
8.aUE-02
2. 15.. E- 03
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1.a88E-02
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5.150E-02
8.288E-~"
8."35E-03
a.282E-03
10.0000
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3.213E-03
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1.82115E+Ol
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(L/A/L+ 1 )
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L- 1
S II1MA L+ 1
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221 .703
55.112
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7.453E-02
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7. 7311E-02
7.738E-02
2.0000
27.212
248.815
411 .• '
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8.3111E-02
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8.38I1E-02
8.388E-02
20.0000
272.118
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2.508E-02
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1.853E-02
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1.0023E+Ol
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138.387
110.82
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1.088E-Ol
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2.0000
27.212
1113.578
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8 .•67E-02
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7. 3UE -02
7. 388E -02
1•. 0000
1110.•83
328.848
37.83
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3.188E-02
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2.102E-02
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XV
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N·· 8.7525
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2.558E-02
18.0000
2 ••. 808
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8 .• 83E-03
8 .•113E-03
SB XV
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38.1117
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3.01!SE-Ol
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2.280E-Ol
2.280E-Ol
2.0000
27.212
87.128
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1.404E-Ol
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8. 3ilE -02
8.311 E -02
8.0000
8 1 . 835
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5.788E-02
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2.511I1E-02
2 .5UE -02
12.0000
183.271
203.188
81.02
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2.887E-02
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8.2111E-03
8.281 E-03
20.0000
272.118
312.035
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1 .• 28E-02
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4.008E-03
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5.172E-02
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1.817E-02
10.0000
138.058
182.501
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128.58
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8.345E-03
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150.107
82.80
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3.727E-03
3.727E-03
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8.31112E-Ol
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315.1108
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1.25.E-Ol
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3.5"'8E-02
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81.835
80.331
137.28
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SB XV
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8.023E-02
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5.522E-02
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7.058E-02
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•. 838E-02
8.885E-02
8.0000
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313.848
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5.055E-02
8.355E-03
3.358E-02
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118.83
1.201E-Ol
1.0.0E-Ol
3.888E-02
5.7115E-02
8.881E-02
2.0000
27.212
155.128
78.83
8.7.8E-02
8 .• 78E-02
2 .• 88E-02
4.888E-02
7. 154E -02
8.0000
108.847
238.781
52.37
4.350E-02
5.221E-02
8.383E-03
2.703E-02
3.842E-02
111.0000
217.8115
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35.87
2.323E-02
3.287E-02
3.805E-03
1.585E-02
1.1155E-02
SB XV
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84.121
1113.38
2.3110E-Ol
1.58n-Ol
7.875E-02
8.58se-02
1.427E-Ol
2.0000
27.212
81.333
135.75
1.3211E-Ol
1.057E-Ol
3.385E-02
4.2731-02
7.83'E-02
8.0000
108.847
172.8e8
71.88
4.54'E-02
4.888E-02
7 .•8I1e-03
1. 731 E -02
2.481E-02
14.0000
1110.483
254.804
48.70
2.37.e-02
2.8871-02
3.00ee-03
Il.583E-03
1.258E-02
SB XV
10P
10· 2.8304E+00 (AYD)
N·· 8.8158
MU·
1.0841
E (AYD)
E (EV)
E PHOT (EV)
LAM8DA
(AI
(L/Il/L-I)
tL/A/L+l )
SII1MA L- 1
SII1MA L+l
SIGMA (MB)
.0000
.000
38.510
321.1111
3.851E-Ol
2.1.3E-Ol
1.258E-Ol
7.410E-02
2.000E-Ol
2.0000
27.212
115.722
188.115
1.1118E-Ol
1.157E-Ol
3. 587E -02
3. 88SE -02
7.283i-02
8.0000
81.1135
120.14B
103.20
5.851E-02
5. 488E -02
8.815E-03
1.515E-02
2.378E-02
10.0000
1311.058
174.5B8
71.02
3.110E-02
3.403E-02
3.538E-03
8 .• 71E-03
1. 201E-02
58
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1.8872E+00 (AYD)
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E (EV)
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LAMBDA
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(L/A/L-l)
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SIQIIIA (MB)
.0000
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25.877
482.87
5.8B5E-Ol
2.7I1lE-Ol
1.850E-Ol
8.186E-02
2.870e-Ol
2.0000
27.212
52.8811
234.43
1.748E-Ol
1.173E-Ol
3.385E-02
3.050E-02
8 .• 35E-02
8.0000
81.835
107.313
115.54
5.288E-02
•. 711I1E-02
8.288E-03
1.034e-02
1. BB3E-02
8.0000
108.847
134.524
82.17
3.B04E-02
3.581E-02
3.B81E-03
7.227E-03
1.0'8E-02
18.0000
217.8115
243.372
80.115
1.317E-02
1.848E-02
8.847E-04
2.770E-03
3.855E-03
155
S15
XV
115P
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I.Ol05E+00
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1.0782
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13.7411
1101.711
1,071E+00
4,10BE-Ot
3.301E-Ol
Il,71I1E-02
4.273E-Ol
2.0000
27.212
40.11151
302.70
1.714E-Ol
1.074E-Ol
2.522E-02
1 .1I80E -02
4.502E-02
4.0000
54.424
158.173
181.87
7.237E-02
5.5158E-02
7.480E-03
8.853E-03
1,1533E-02
8.0000
108.847
122.5115
101.13
2.1515IE-02
2.582E-02
1 , 821E -03
3.423E-03
5.253E-03
12.0000
1153.271
177.020
70,04
1,428E-02
1.58IE-02
7,557E-04
1.873E-03
2.152IE-03
18.0000
244.1015
258.1555
47.13
7, 4815E -03
Il.1503E-03
3,0315E-04
Il.1I12E-04
1.303E-03
58
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1.0770
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LAM150A
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14150.24
1 .1585E+00
5.5113E-Ol
5.082E-Ol
1.120E-Ol
S.202E-Ol
2.0000
27.212
35.7S1
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1.523E-Ol
Il.232E-02
r . 738E -02
1.277E-02
3.015E-02
4.0000
54.424
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5.838E-02
4,401E-02
4.4113E-03
5. 1OllE -03
Il.802E-03
10.0000
1315.0511
144.1508
8S.74
1.417E-02
1.4155E-02
8,078E-04
1.300E-03
1.1I08E-03
12.0000
1153.271
171.820
72.115
1.0515E-02
1.1155E-02
4,011E-04
Il.7157E-04
1.378E-03
S15
XV
40
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2.3574E+Ol
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320.752
38.155
3.7153E-02
Il.1I113E-02
1.141E-02
1.208E-Ol
1.322E-Ol
2.0000
27.212
347.11.4
35.53
3.282E-02
Il.217E-02
9.422E-03
1.115E-Ol
1.20IlE-Ol
15.0000
81.15315
402.388
30.81
2.5157E-02
7.855E-02
15.888E-03
Il.3152E-02
1.003E-Ol
SB XV
50
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1 . 2112 1 E + 01
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N.· 4.1730
MU'
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E (AYD)
E (EV)
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LAM15DA
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SICMA
L - 1
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L+l
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175.7118
70.53
7.118E-02
1,18I1E-Ol
2.237E-02
Il.375E-02
1. 181 E-Ol
2.0000
27.212
203.010
81.07
5. 577E -02
1,051 E-O 1
1.587E-02
8.481E-02
1.005E-Ol
8.0000
81.1535
257.43~
48.115
3.720E-02
8.2II2E-02
8.1157E-03
8,874E-02
7,570E-02
14.0000
1110.483
388.281
33.85
2.024E-02
5.488E-02
3.771E-03
4,158E-02
4.538E-02
S15
XV
150
EO' 1.32515E+00
(RYO)
N·· 5,11188
MU'
.8014
E (RYO)
E (EV)
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LAMeOA (A)
(L/R/L-I)
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L-l
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L+l
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,0000
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113,277
1011.45
1.141E-Ol
1,378!-01
3,70llE-02
8.113E-02
1.182E"01
2.0000
27.212
140.4811
88.25
7.1I10E-02
1.157E-Ol
2.2101-02
7,08I1E-02
1.211I1E-02
15.0000
81,1535
1114.1113
153.151
4.510E-02
8.3S21-02
Il.1I.5E-03
5,1154E-02
15,1150E-02
12.0000
1153.271
2715.548
44.83
2.458E-02
5.1522E-02
4,200E-03
3.2SJ15E-02
3. 71l5E-02
58
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80
EO. 4.3210E+00
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158.7111
210.811
2.27I1E-Ol
1.718E-Ol
7.1577E-02
15.524E-02
1.420E-Ol
2.0000
27,212
88.003
144,17
1. l111E-Ol
1,274E-Ol
3.015.E-02
5.2152E-02
1. 32l1E -02
8.0000
81 ,1535
140,427
88.211
5.113E-02
7.810E-02
Il. 2211E-03
3.22SJE-02
4.1152E-02
10.0000
138,0511
1114.850
153.153
2.888E-02
5.384E-02
4.087E-03
2. 130E -02
2.538E-02
515 XV
100
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2.8454E+00
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35.11113
344,48
3.7154E-Ol
1.984E-Ol
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5.342E-02
r , 6115E-0 1
2.0000
27.212
153.201S
11115. 17
1.442E-Ol
1.287E-Ol
3.303E-02
3.1I1S0E-02
7.2531-02
15.0000
81 .1535
117.1528
105,41
4.1133E-02
15.8351-02
7.11151-03
2.072E-02
2.7111 E - 02
12.0000
1153.271
11111.2154
152.22
1 , 11150E - 02
3.15113~-02
1.9241-03
1.025E-02
1 ,2 17E -02
14,0000
1110.483
228,478
54,75
1.51531-02
3,150E-02
1.3112E-03
8.474E-03
Il.8815E-03
S8 XV
120
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1.715ISE+00
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.0000
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24.2114
510.37
5.51151-01
2.184E-Ol
1.811111-01
4,3701-02
2.338E-Ol
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24.51515
504.71
5.4 72E -0 1
2.172E-Ol
1.84I1E-Ol
4,311E-02
2.28U-Ol
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24.636
41111.18
5.371E-Ol
2, 1150E- 0 1
1.S01E-Ol
4.311E-02
2.238E-Ol
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8. 1154
32.457
382.00
3.413E-Ol
1.828E-Ol
Il.50U-02
4,088E-02
1.35I1E-Ol
1.0000
13,15015
37.81111
327,15
2.1522E-Ol
1.1522E-Ol
15.550E-02
3.758E-02
1 .031 E -0 1
4.0000
54,424
78,711
151.51
7.41I1E-02
8.100E-02
1.107E-02
1.114'71-02
3.0541-02
15.0000
81.1535
105.lI211
111.05
4.4158E-02
5.81511-02
5.315E-03
1.372E-02
1 .1I03E -02
10.0000
1315.0511
180.353
77.32
2.1153E-02
3.151111-02
1.885E-03
7.1I1I1E-03
Il.8041 -03
58
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Il.70221-01
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L-l
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L+l
SICMA
(M8)
.0000
.000
13.201
11311.24
1.0141+00
2.3SJOE-Ol
3.410E-Ol
2.842E-02
3.SSJ41-01
.1000
1.3151
14.5151
851.48
8.SSJ31-01
2.314E-Ol
2.7031-01
2.11401-02
2.111171-01
.2000
2.721
15.1122
778,12
7.3111E-Ol
2,223E-Ol
2.18151-01
2.111571-02
2.483E-Ol
.15000
8. 1154
21 .3154
580.35
4.414E-OI
1.8521 -0 1
1.081S1-Ol
2.7153E-02
1.3811 -0 1
1.0000
13 . •015
215.801
4152.52
3.0571-01
1.550E-Ol
15.21171-02
2.42BE-02
8.72151-02
4.0000
54.424
157,1524
183.35
S.252E-02
15.27U-02
8.8441-03
1 .0051 -02
1 .15701 -02
S.OOOO
8 1 . 1535
114.8315
130,74
3.4751-02
4,313E-02
2.87BE-03
8.15511-03
1.52I1E-03
10.0000
1315.0511
1411.2150
83.07
1.15101 -02
2.5301-02
Il.2441-04
3.15021-03
4.5271-03
SIS XV
200
EO·
S.08481-01
(RYO)
N·· 111.22117
MU'
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1
(RYO)
E (EV)
t
PHOT
(EV)
L.AMISOA
( A)
(L/A/L-l)
(L/A/L+I)
SIGMA
L-l
SIGMA
L+l
SICMA
(MIS)
.0000
.000
8.2711
14111. lS5
1.515li1E+00
2.3411-01
5.254 E -0 1
1.71I1E-02
5.42.E-Ol
,2000
2.721
11.000
1127,115
Il.84I1E-Ol
2.2251-01
2.1582E-Ol
2.053E-02
2.8881-01
.3000
4.082
12.31S0
1003.011
8.0811-01
2.1015E-Ol
2,034E-Ol
2. 087E -02
2.241E-Ol
.4000
5.442
13.121
1103.152
15.183E-Ol
1.1184E-Ol
1.581E-Ot
2.035E-02
1.1110E-OI
1.0000
13.15015
21 .885
515S.54
3.07151-01
1. 31115E-0 1
5.201E-02
1.1S08E-02
!5. 80llE -02
4,0000
54.424
152.102
1111.14
5.058E-02
4.11011-02
4.032E-03
5. 880E -03
Il.111 E -03
8.0000
108.841
117, t215
1015.88
1.703E-02
2.402E-02
8 .537E -04
2.5481-03
3.402E-03
1111
Sil XV
4F
la' 1.7503E+Ol IRYD)
Na.
3.5853
MU'
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1 IIllYDI
1 lEV)
E PHOT (EV)
LAMIDA
lA)
(L/R/L-l)
(L/R/L+1)
SIGMA L- 1
SIGMA L+'
SIGMA IM8)
.0000
.000
238.14.
52.011
2.7114E-02
1.731E-Ol
4.900E-03
2.583E-Ol
2.1112E-Ol
2.0000
27.212
2115.381
48.72
2.273E-02
1. 31111E-0 1
3.1I111E-03
1.815E-Ol
1.1I02E-Ol
8.0000
108.847
3411.t11111
35.73
1.380E-02
8. 1311E-02
1.781E-03
8.254E-02
8.432E-02
14.0000
1110.483
428. lia 2
28.13
Il.17I1E-03
5.24I1E-02
Il.725E-04
4.23I1E-02
4.333E-02
S8 XV
5F
EO'
1 . 0528E+0 1 IAYD)
Na.
4.11228
MU'
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E (RYD)
E 1EV l
i. PWOT
(EV)
I.AMBDA
(A)
IL/R/L-1)
lL/R/L+l)
SIGMA L·l
SlaMA L+l
SIQIllA 1MB)
.0000
.000
143.250
811.lUi
5.71I1E-02
2.411I1E-Ol
1.2110E-02
3.213E-Ol
3.331lE-Ol
2.0000
27.212
170.4112
72.74
4.1801-02
1.874E-Ol
8.023E-03
2.14I1E-Ol
2.22I1E-Ol
8.0000
108.847
252.0117
411. 18
2.030E-02
8.422E-02
2.788E-03
8.037E-02
8.31I1E-02
111.0000
217.11115
3110.ll4.
34.35
1.017E-02
4.801E-02
r , OOIIE -03
2.t18U-02
3. 08U -02
18.0000
244.11011
388.158
31.114
8.811 E-03
4.1118E-02
8.11I1E-04
2.422E-02
2.503E-02
SB XV
IIF
EO' 7. 10211E +00
(AYD)
Na.
5.11284
MU'
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E ( AYDl
E (EV)
E PHOT lEV)
LAMIDA lA)
(L/A/L - 1)
lL/R/L+l)
SIGMA L- 1
SIGMA L+ 1
SlaMA
(MIl
.0000
.000
1111.1137
128.30
9.IIIIIIE-02
3.270E-Ol
2.3118E-02
3.711E-Ol
3.1150E-Ol
2.0000
27.212
123.848
100.11
Il. l1111E-02
2.242E-Ol
1.2115E-02
2.235E-Ol
2.3111E-Ol
4.0000
54.424
151.0110
82.08
4.2114E-02
1. 1133E -0 1
7.500E-03
1.4411-01
1.52lE-Ol
Il.0000
81,1135
178.272
118.55
3.11141-02
1. 242E-Ol
4.807E-03
Il.811I1E-02
1. 035E-Ol
12.0000
1113.271
21511.1108
47.70
1.553E-02
Il.450E-02
1.1I88E-03
3.883E-02
4.0l2E-02
111.0000
217.11115
314.331
311.44
1.073E-02
4.5111E-02
8.751E-04
2.348E-02
2.448E-02
SB XV
8r
EO' 3.81144E+00 IRYO)
Na.
7.11305
MU-
.31115
E IRYD)
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E PHOT lEV)
LAMBDA
lA)
IL/RlI.-I)
lL/R/L+l)
SIGMA 1.-1
SIQIllA L+l
SlalllA
(1II11)
.0000
.000
112.578
2315.81
1 . 1111 lE -0 1
4 .1lI3E - 0 1
5.II11E-02
4.4115E-Ol
5.02I1E-Ol
2.0000
27.212
711.7110
155.311
Il.534E-02
2.11I1I5E-Ol
1.11153E-02
2.080E-Ol
2.27I1E-Ol
4.0000
54.424
107.002
115.87
5.1120E-02
1.735E-Ol
Il.102E-03
t . 1511E-0 1
1.247E-Ol
Il.0000
81.1135
134.214
112.38
3.711E-02
1.217E-Ol
4.9781-03
7.134E-02
7.11321-02
sa XV
lOF
la- 2.4258E+00 IAYD)
Na.
Il.113011
MU'
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E 1RYD)
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E PHOT lEV)
LAMBDA
lA)
(L/R/L- Tl'
II./A/L+ll
SIGMA L- 1
SI QllIA L-1
SlalllA
CMI)
.0000.
,000
33.005
375.1111
3.331E-Ol
Il:554E-Ol
Il.8114E-02
5.0111E-Ol
Il.077E-Ol
2.0000
27.212
110.2111
205.110
1.1115E-Ol
2.85I1E-Ol
2.111I1E-02
1.7114E-Ol
1.1I84E-Ol
4.0000
54.424
87.428
141.81
5.1175E-02
1.1152E-Ol
8.40IlE-03
8.5114E-02
9.405E-02
8.0000
108.847
141 .852
87.41
2.411I1E-02
7.777E-02
2.304E-03
3.08lE-02
3.311E-02
12,0000
1113.271
1811.2711
113.17
1. 3211E -02
4.553E-02
Il.338E-04
1.4111E-02
1 . 555E -02
SI XV
12F
EO'
1.1I1132E+00 IRYD)
N*E
11.11311
MU'
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E lRYD)
E (IV)
PWOT lEV)
LAMIDA
(A)
(L/A/L-1)
(L/R/L-l)
SIGMA 1.- 1
SIGMA L-l
SIGMA (MI)
.0000
.000
22.1129
547.110-
4.1I110E-Ol
8.35I1E-Ol
1,49I1E-Ol
5.I72E-Ol
7.171E-Ol
2.0000
27.212
49.841
248.711
1 . 2511E - 0 1
2.831E-Ol
2.12I1E-02
1.435[-01
1 . ~U-Ol
4.0000
54.424
77.053
1110.111
5.7111 E-02
1.501E-Ol
Il.1I110E-03
Il. 2311E-02
Il.1132E-02
8.0000
108.847
131.477
114.30
2.175E-02
Il.588E-02
1.117I1E-03
2.04I1E-02
2.217[-02
10.0000
1311.01511
15&.1188
78.13
1.52U-02
4.8112E-02
Il.1183E-04
1.347E-02
1.447E-02
12.0000
1113.271
185 .•00
1111.70
1.131E-02
3.742!-02
Il.407E-04
Il.34111-03
8.987E-03
S8 XV
20F
EO- 5.83831-01
(RYDl
N··
18.5312
MU'
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E (ÀYD)
E ( EVI
E PHOT (EV 1
LAMIDA
lA)
(I./R/L-l)
(I,./R/I.-l)
SIGMA L- 1
SIQMA 1.-1
SlalllA
(M8)
.0000
.000
7.844
1'15110.84
1.412E-00
1 . 11117E +00
4.214E-Ol
7.930E-Ol
1.21I1E-00
2.0000
27.212
315.1515
352.118
t.l04E-Ol
2.1481-01
1.154E-02
5.832E-02
Il.888E-02
4.0000
54.424
112.3117
1118.80
4.000E-02
Il.378E-02
2.11881-03
1.870E-02
2. 238E -02
117
TE XVI
!lS
ID'
1.801171+01
(RYD)
N·· 3.71142
MU'
1 . 23!l8
1
(RYD)
1
CIV)
1 PHOT (IV)
LAMBDA
(Al
(L/R/L-l)
(L/RIL-l)
SIGMA L - 1
SIGMA L- 1
SIGMA
(Mil)
.0000
.000
24!l.818
!l0.44
.000
8.8011-02
.000
7. 14!l1-02
7.14111-02
2.0000
27.212
273.030
4!l.41
.000
5.11101-02
.000
5.111131-02
5.111131-02
20.0000
272.118
!l17.1137
23.114
.000
2.4!l7E-02
.000
1 . 118!l1 -02
1.11851-02
TE XVI
8S
ID.
1.118lE+Ol
(RYD)
N·· 4.78411
MU'
1.21!l1
1
(RYO)
1
IIV)
1 PHOT
(IV)
LAMBDA
(A)
(L/R/L-O
(L/RIL-l)
SIGMA L- 1
SIGMA
L- 1
SIGMA
(M8)
.0000
.000
1!l2.133
81.!l0
.000
Il.1I01E-02
.000
Il.3711-02
Il.371E-02
2.0000
27.212
1711.34!l
811.13
.000
7.882E-02
.000
7.002E-02
7.0021-02
111.0000
217.11815
3811.828
33.153
.000
2.837E-02
.000
1. 870E-02
1.8701-02
TE XVI
85
EO' 5.!l387E+00
(RYD)
N·· 8.7118!l
MU'
1, 2015
E (RYO)
1
(IV)
1 PHOT
(EV)
LAMBDA
(A)
(L/RIL-l)
(L/RIL-l)
SIGMA
L- 1
SIGMA L- 1
SI GllIA
(MB)
.0000
.000
7!l.3511
184.!l3
.000
1.78!lE-Ol
.000
1.4781-01
1.4781-01
2.0000
27.212
102.571
120.88
.000
1.1321-01
.000
8.2.57E-02
8.2!l1E-02
8.0000
108.847
184.207
117.31
.000
4,80111-02
.000
2.877E-02
2.1177E-02
18.0000
244.1108
320.288
38.71
.000
2.13111-02
.000
Il.17I1E-03
Il. 1711E- 03
TE XVI
lOS
ID. 3.30331+00 (RYD)
N·· 8.8034
MU'
1.11188
E (RYD)
1
( IV)
1 PHOT «IV)
LUIIiDA
(Al
(L/RIL-l)
(L/RIL+l)
SIGMA
L- 1
SIGMA
L+l
SIGMA
CMIII
.0000
.000
44.1144
275.8~
.000
2.728E-Ol
.000
2.102E-Ol
2.1021-01
2.0000
27.212
72.158
171.83
.000
1.3!l7E-Ol
.000
8.355E-02
8.3!l51-02
Il.0000
81.1135
128.5711
117. Il!l
.000
5.8701-02
.000
2.74lE-02
2.7411-02
14.0000
1110.483
23!l.427
!l2.1111
.000
2.3241-02
.000
7.111111-03
7.111111-03
TE XVI
12S
10- 2. 11125E +00
CRYD)
N·· 10.80!l7
MU'
1. 11143
1
(RYO)
E (IV)
1 PHOT (EVI
LAMBDA
(A)
IL/RIL-o
(L/R/L-l)
SIGMA L-l
SIGMA
L- 1
SIGMA
(MI)
.0000
.000
28.831
415.83
.000
3.81151-01
.000
2.8001-01
2.800E-Ol
2.0000
27.212
57.043
217.311
,000
1.411!l1-01
.000
7.11118E-02
7.111181-02
8.0000
81.83!l
111.488
111.23
.000
5.3281-02
.000
1.11871-02
1.1187E-02
10.0000
138.0!l1l
1115.800
74.74
.000
2.1122E-02
.000
8.11011-03
8.1I0tE-03
18.0000
244 .11011
274.737
45. 13
.000
1.370E-02
.000
3.2'421 -03
3.2421-03
TE XVI
1liS
ID'
1.1875E+00
(RYD)
N·· 14.8077
MU'
1.11123
1
(RYOI
1
(EV)
1 PHOT (IV)
LAMBDA
(AI
(L/R/L-l)
(L/RIL+ 1 )
SIGMA L - 1
SIGMA
L- 1
SIGMA
(M8)
.0000
.000
1!l.885
780.52
.000
8.11331-01
.000
4.31121-01
4.31121-01
2.0000
27.212
43,0117
287.118
.000
1.44111-01
.000
5.1185E-02
5.885E-02
8.0000
108.847
124.732
118.40
.000
2.8481-02
.000
8.3!l81-03
8.35llE-03
20.0000
272.118
288.003
43.05
.000
8.023E-03
.000
1.1811-03
1. 11111 -03
TE XVI
20S
EO'
7.23851-01
1 RYD)
N·· 18.80811
MU'
1 . 11114
E (RYD)
E (IV 1
1 PHOT
(EV)
LAMIDA (A)
(L/RIL-l1
(L/R/L+l)
SIGMA
L- 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
Il.8411
1258.27
.000
1.0031+00
.000
8.223E-Ol
Il.2231-01
2.0000
27.212
37.0!l8
334.58
.000
1.3001-01
.000
3.11341-02
3.11341-02
8.0000
81.835
111.481
13!l.53
.000
3.224E-02
.000
5.1173E-03
5.11731 -03
n
XVI
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EO.
1.117471+01
(RYD)
N·· 3.110117
MU'
1.0803
1
(RYOI
1
(EV)
E PHOT
(EV)
LAMIIDA
(A)
(L/RIL-l)
(L/RIL- 1 )
SIGMA
L - 1
SIGMA
L- 1
SIGMA
(MBI
.0000
.000
227.8112
!l4.41
8.72lE-02
7.5221-02
2.15I1E-02
5.402&-02
7. 557E -02
2.0000
27.212
255.074
48.111
!l.5881-02
8.88llE-02
1 .8731 -02
4.7521-02
Il.4281-02
8.0000
108.847
3311.710
38.82
3.55111-02
4.8701-02
8.11341-03
3.3481-02
4.23111-02
20.0000
272.118
41111.881
24.80
1.81111-02
3.0111-02
3.8271-03
1.81181-02
2.21111-02
TE XVI
8P
ID.
1.05181+01
(RYOI
N·· 4.11340
MU'
1.01180
E IRYO)
1
aV)
1 PHOT (IV)
LAMBDA
lA)
(L/R/L-l1
(L/RIL+l)
SIGMA L - 1
SIGMA L- 1
SIGMA
(MB)
.0000
.000
143.074
88.88
1.087E-Ol
9.8131-02
3.413E-02
!l,772E-02
Il. 1851 - 02
2.0000
27.212
170.2811
72.81
8.01 1E-02
8.10IlE-02
2.28111-02
4.1188& -02
8.1177[-02
8.0000
108.847
251.1121
411.22
4. 11111 -02
!l.127E-02
Il.2811[-03
2.7741-02
3.70lE-02
14'.0000
217.8115
380.7811
34.37
2.3081-02
3.2871-02
4.028E-03
1.8331-02
2.0381-02
TE XVI
8P
EO. 5.21188E+00
(RYD)
N·· 8.11508
MU'
1 .04112
E (RYO)
1
(EV)
E PHOT (EV)
LAMIIDA
(Al
IL/R/L-l )
IL/R/L+l)
SIGMA
L- 1
SlaMA L+l
SIGMA
(MI)
.0000
.000
72.0115
171.118
2. , 1111-01
1.4a41-01
Il. 78lE-02
Il. 74lE-02
1.3501-01
2.0000
27.212
1111.307
124.85
1.2411-01
1.034E-Ol
3.20!lE-02
4.448&-02
7.853E-02
'.0000
108.847
180.1142
88.52
4.5381-02
4.ll4I1E-02
7.807&-03
1.817E-02
2.838E-02
111.0000
217.8115
2811.7811
42.78
2.0531-02
2.704E-02
2.55111-03
8.878E-03
1.143E-02
TE XVI
10P
EO. 3.11110E+00 (RYD)
N·· 8.a588
MU'
1.0432
E (RYD)
E (EV 1
E PHOT
(IV)
LAMBDA
(A)
IL/R/L-l)
IL/R/L+l1
SIGMA L-l
SlaMA L+l
SIGMA
(MB)
.0000
.000
43.417
285.57
3.4110E-Ol
2.0821-01
1.1081-01
7.7351-02
1. 8B 11-01
2.0000
27.212
70.8211
17!l.55
1.547E-Ol
1.1!l71-01
3. !l4lE-02
3.1180E-02
7.5001-02
6.0000
81.e35
12!l.052
1111. 15
5.110111-02
5.&3111-02
Il. 145E-03
1. 1188E -02
2.!l81E-02
10.0000
1311.01111
1711.478
811.08
3.20IlE-02
3.!l34E-02
3.8841-03
Il.38IE-03
1.325E-02
18.0000
244.11011
288.323
43.00
i . 435E -02
1.81141-02
1.244E-03
4.3331-03
!l.5771-03
TE XVI
12P
EO.
2.1313E+00
(RYD)
N·· 10.9598
MU'
1.0402
E (RYD)
E (EV)
E PHOT
(Ev 1
LAMBDA
(A)
(L/R/L-n
IL/R/L+1)
SIGMA 1.- 1
SIGMA 1.+1
SICMA
(MBI
.0000
.000
28.9lil8
427.57
5.175E-Ol
2.878E-Ol
1.fl2f1E-Ol
8.715E-02
2.498E-Ol
2.0000
27.212
58.210
220.58
1.708E-Ol
1.198E-Ol
3.434E-02
3.387E-02
8.800E-02
8.0000
81.l!I35
110.l!I33
112.07
5.438E-02
5.0 Il E -02
8.1154E -03
1.ll!14E-02
1. 84lilE -02
8.0000
108.847
137.845
89.95
3.745E-02
3.757E-02
4. 049E -03
8.15lE-03
1.220E-02
Il!1.0000
217.l!I95
24f1.l!I92
50.28
1.392E-02
1.738E-02
1.0021-03
3.123E-03
4.125E-03
18.0000
244.90l!l
273.1104
45.27
1.1l!15E-02
1.512E-02
7.7111 E - 04
2.l!I23E-03
3. 402E -03
TE XVI
Il!1P
EO.
1.1435E+00
lRYDI
N.· 14. lill!l25
MU'
1.0375
E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA
(A)
(L/R/L-I)
(L/R/L+1 )
SIGMA 1.- 1
SIGMA 1.+ 1
SIGMA
(M8)
.0000
.000
15.558
7.l!I.92
Il.433E-Ol
4.044E-Ot
2.1I00E-Ol
1.0el!lE-Ol
3.lIl!1l!1l-01
2.0000
27.212
42.770
289.811
1.729E-Ol
1.128E-Ol
2.879E-02
2.278E-02
4.9117E-02
4.0000
54.424
l!IlI.982
177.17
7.515E-02
5.1112E-02
8.279E-03
1.02BE-02
t. 853E -02
l!I.OOOO
81.l!I35
117.194
127.57
4.30lE-02
3.82l!1E-02
3.787E-03
5.1I8lE-03
Il.728E-03
12.0000
Il!I3.271
178.8211
l!I9.33
1.522E-02
1 . 89l!1E -02
8.877E-04
2.154E-03
3.022E-03
18.0000
244.808
2l!10.4l!1ll
47.80
8.014E-03
1.023E-02
3.504E-04
1.142E-03
1.493E-03
20.0000
272.118
287.l!I77
43.10
8.78IU-03
8.948E-03
2.758E-04
9.l!I51E-04
1.241E-03
TE XVI
20P
EO.
7. 118l!1E-Ol
(RYD)
N.· 18.lIl!138
MU'
1.03l!14
E (IIYDI
E (EV)
E PHOT
(EV)
LAMIDA
(AI
(L/A/L-l)
(L/A/L+ 1 )
SIGMA 1.- 1
SIGMA 1.+1
SIGMA
(M8)
.0000
.000
9.l!I18
1280.12
1.483E+00
5.573E-Ol
4.482E-Ol
1. 2l!10E-Ol
5.723E-Ol
2.0000
27.212
38.897
338.03
1.570E-Ol
9.884E-02
1.1I05E-02
t .510E-02
3.415E-02
4.0000
14.424
84. 1011
1113.40
Il.155E-02
4.738E-02
5.087E-03
1!1. 030E -03
1.112E-02
10.0000
138.059
145.745
85.07
1.51I1E-02
i . 575E -02
7.041E-04
1. 515E-03
2.2111E-03
14.0000
180.483
200.1l!18
81.94
8.833E-03
t .027E-02
3.272E-04
8.84I1E-04
1. 212E -03
TE ltVI
40
EO. 2.811111E+Ol
(RYDI
N.· 3.12511
MU'
.8741
E (RYDI
E (EV)
E PHOT
(EV 1
LAMIOA (A)
(L/A/L-l)
(L/A/L+I)
SIGMA 1.-1
SlaMA 1.+ 1
SIGMA
(MI)
.0000
.000
35f1.457
34.78
3.330E-02
9.235E-02
Il.1I34E-03
1.14l!1l-01
1. 24l!1E-Ol
2.0000
27.212
383.8811
32.32
2.114 1 E-02
8.5441-02
8.343E-03
1. Oel!lE -01
1. 139E -01
4.0000
54.424
410.881
30.18
2.81I1E-02
7.1112E-02
7.084E-03
9.IIII.E-02
1.041E-Ol
TE XV 1.
50
EO.
1.4483E+Ol
(RYDI
N.&
4.2043
MU'
. 711B7
E (RYDi
E (EV)
E PHOT
(EV'
LAMBDA
lA)
(L/A/L-l)
IL/A/L+l)
SIGMA 1.-1
SIGMA 1.+1
SI Q/IIIA
(M8)
.0000
.000
1117.048
fl2.112
8.2.8E-02
1.125E-Ol
1.1If15E-02
9.398E-02
1.13f1E-Ol
2.0000
27.212
224.2f10
55.211
5.055E-02
9.U2E-02
t .440E-02
8.408E-02
Il.8481-02
8.0000
81.l!I35
278.l!I84
44.49
3.485E-02
7.1142E-02
8.50flE-03
fI.fl27E-02
7.478E-02
18.0000
217.8115
414.743
2 •. 811
1.748E-02
4.9041-02
3. 184 E -03
3.780E-02
4.079E-02
TE XVI
80
EO. a.3&<12E+00
(RYDI
N·· 5.2288
MU'
.7714
E IAYD)
E (EV)
E PHOT
lEV)
LAMBDA
(A)
(L/A/L-l )
1L/A/L+ 1 )
SlaMA 1.- t
SIGMA 1.+1
SIGMA
(M8)
.0000
.000
127.40.
117.31
t.OllE-Ol
1.3211E-OI
3.274E-02
8.4.0E-02
1.178E-Ol
2.0000
27.212
154.821
80. III
7.284E-02
1.11SE-Ol
2.0IllE-02
7.28.1-02
9.3401-02
8.0000
81.835
2011.044
5a.31
4.3221-02
8.1821-02
Il.8131-03
5.2110E-02
8.271E-02
12.0000
183.271
2110.880
42.81l
2.435E-02
5.574E-02
4.331E-03
3.4051-02
3.838E-02
TE XVI
80
EO. 4.8788E+00 (RYD)
N.· 7.2454
MUa
.7548
E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA
(A)
(L/R/L-I)
(L/A/L+ 1 )
StGMA
1.- 1
SIGMA 1.+ 1
SIGMA
(M8)
.0000
.000
lllS.351
188.8l!1
2.021E-Ql
1.718e-Ol
8.811E-02
7.385E-02
1.420e-Ol
2.0000
27.212
93.5l!13
132.52
1.123E-Ot
1.271E-Ol
2.a85E-02
5.7021-02
8.887E-02
8.0000
81.835
147 .•87
83.78
5. 083E -02
7.874E-02
9.81IE-03
3.480E-02
4.421E-02
10.0000
138.0511
202.410
81.25
2 .•41E-02
5.4711-02
4.4001-03
2.285E-02
2.72!SE-02
TE XV 1
100
EO.
2 .•1I10E+00
(RYD)
N·· Il.2515
MU'
.7485
E tRYD)
E lEV)
E PHOT
(EV)
LAMIIDA
(A'
IL/A/L-ll
(L/A/L+1 )
SIGMA 1.-1
SI caMA 1.+ 1
SIGMA
(M8)
.0000
.000
40.885
304.87
3.339E-Ol
2.087E-Ol
1.140E-Ol
8.554E-02
t . 7.8E -01
2.0000
27.212
87.1107
182.58
1.3113E-Ol
1.3111E-Ol
3.314E-02
4.458E-02
7.771E-02
8.0000
81.835
122.330
101.35
5.0341-02
7.044E-02
7.71131-03
2.288E-02
3.0881-02
12.0000
183.271
203.1188
80.79
2.053E-02
3.828E-02
2.180E-03
1.127E-02
1.3431-02
14.0000
1.0.483
231.178
53.83
l.l!I451-02
3.2l!1l1l-02
1.5721-03
11.3151-03
1.08.1 -02
18.0000
244.90l!l
285.l!IOl
43.41
1. 1211 -02
2. 48l!1E -02
Il.1531-04
l!I.l!I57E-03
7.573E-03
TE XV 1
120
10· 2.0211E+00 (RYD)
N•• 11.254l!1
MU'
.7454
E CAYO)
E (IV)
E PHOT
(EV)
LAMBDA
(A)
(L/A/L-l)
(L/R/L+ 1 )
SIGMA 1.-1
SlaMA 1.+1
SIQMA
(MBI
.0000
.000
27.4.8
450.88
4.94111-01
2.37IE-Ol
l.l!III3E-Ol
5.8481-02
2.278E-Ol
2.0000
27.212
54.710
22l!1.82
1.5331-01
1. 2117E-Ol
3.2311-02
3.471E-02
Il.7021-02
l!I.OOOO
81.l!I35
10•. 134
113.81
4.8431-02
IL 1331-02
5.11131-03
1 . 548E -02
2.13.1-02
10.0000
13l!1.0l!l9
Il!13. !l1l8
75.81
2.284E-02
3.710E-02
2.145E-03
8.85I1E-03
1.100E-02
Il!1.0000
217.895
245. 1113
!l0.57
1.1151-02
2.274E-02
7.l!Il!IOE-04
4.7791-03
5. 545E -03
TE XV 1
180
EO.
1 .01l1l7l+0il
1RYD)
N•• 15.2574
MU'
. 742l!1
E (RYOI
1
(IV)
E PHOT
(EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+I)
SIGMA 1.-1
SIGl....
1.+1
SIGMA
(MBI
.0000
.000
14.11113
828.84
Il.002E-Ol
2.878E-Ol
3.0481-01
4.l!Il!IIIE-02
3.514E-Ol
·2.0000
27.212
42.174
2a3.98
1.547E-Ol
1.1114E-Ol
2.538E-02
2.1171-02
4.l!III4E-02
4.0000
54.424
811.388
178.l!I9
8.5811-02
8.724E-02
7.508E-03
1.183E-02
1 .•331 -02
8.0000
81.835
IIl!1.!l1l8
128.35
3.l!I8U-02
4.598E-02
3.308E-03
7.81111E-03
1.10lE-02
12.0000
Il!13.271
178.234
811.58
1.257E-02
2.183E-02
7.081 E -04
3.20U-03
3 .• 1 lE -03
TE XVI
200
EO'
8 .• 022E-Ol
(RYD)
N·· 111.258l!1
MU'
.7414
E (RYD)
1
(EV)
1
PHOT
(IV)
LAMBDA
(A)
(L/R/L-l)
CL/R/L+I)
SIGMA 1.-1
SIGMA 1.+1
SIGMA
(Mill
.0000
.000
9.3111
1320.25
1.412E+00
3.228E-Ol
4.705E-Ol
3.l!I90E-02
5.0741-01
2.0000
27.212
3l!1.&03
338.73
1.404E-OI
Il.815E-02
1.814E-02
1. 330E -02
3.1441-02
4.0000
54.424
l!I3.815
184.2.
5.388E-02
5.318E-02
4.858E-03
l!I.8051-03
1.148E-02
10.0000
138.0Slil
145.450
85.24
1.277E-02
1.11118E-02
5.9511E-04
2.185E-03
2.7811-03
18.0000
244 . • 0&
254.2.8
48.78
4.7281-03
•. 758E-03
1.42.1!.-04
Il. l2I1E -04
1.05111 -03
8st
TE XVI
4F
EO'
1.11751E+Ol
(RYD)
N·· 3.8002
MU'
.311118
E (RYDI
E (EV)
E PHOT
(EV)
LAMBDA (A)
(L/R/L-l)
(L/R/L+l)
SIGMA L- 1
SIGMA L+ 1
SIGMA 1MB)
.0000
.000
288.725
48. 14
2.421E-02
1. 514E-0 1
4.243E-03
2.211E-Ol
2.253E-Ol
2.0000
27.212
2115.837
41.110
2.02I1E-02
1.251 E-Ol
3.282E-03
1. 884E -0 1
1 . 8117E-0 1
8.0000
81 . 835
350.380
35.311
1 .481 E-02
8.1114E-02
2.08I1E-03
Il.1I117E-02
1.020E-Ol
14.0000
1110.483
4511.208
27.00
8.783E-03
5.10lE-02
Il.541E-04
4. 211 lE -02
4.387E-02
TE
XVI
5F
EO'
1.11122E+Ol
(RYD)
N·· 4.83311
MU'
.3881
E
IRYD)
E (EV)
E PHOT lEV)
LAMBDA (A)
(L/R/L-l1
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MBi
.0000
.000
182.207
711.44
5.01l0E-02
2.199E-Ol
1. l111E-02
2.817E-Ol
2.1128E-Ol
2.0000
27.212
1811.4111
115.411
3.818E-02
1.III1I1E-OI
7.43I1E-03
1.IIa.E-Ol
2.03I1E-Ol
8.0000
108.847
271.058
45.74
1.1I110E-02
9.0118E-02
2.804E-03
8.004E-02
8.288E-02
18.0000
244.11011
407.114
30.48
8.8113E-03
4.227E-02
8.1172E-04
2.1112E-02
2.III1I1E-02
TE
XVI
IIF
EO'
8.0514E+00 (RYD)
N·· 5.11388
MU'
.31112
E IRYD)
E (EV)
E PHOT (EV)
LAMIIDA lA)
IL/R/L-l)
IL/R/L+l)
SIGMA L- 1
SIGMA L+'
SIGMA (Mil)
.0000
.000
1011.547
113.18
8.537E-02
2.88!lE-Ol
2.150E-02
3.274E-Ol
3.48I1E-Ol
2.0000
27.212
1311.7811
110.1111
5.724E-02
2.05I1E-Ol
1.207E-02
2.078E-Ol
2.1'7E-Ol
4.0000
54.424
1113.1170
75.112
4.108E-02
1.540E-Ol
7.451E-03
1.31171-01
1.471i-Ol
Il.0000
8 1 . 1135
1111.182
114,85
3.01l0E-02
1.II1I1E-Ol
4.1117E-03
9.823E-02
1. 03lE-Ol
12.0000
1113.271
272.818
48.45
1.574E-02
Il.480E-02
1.820E-03
4.113E-02
4.2115E-02
18.0000
244. 1l01l
354.453
34.118
9.430E-03
4.027E-02
8.48eE-04
2.08~E-02
2.14eE-02
TE XVI
8F
EO'
4.38B3E+00 (RYD)
N·· 7.8404
MU'
.35118
E (RYD)
E (IV)
E PHOT (EV)
LAMIIDA (A)
(L/R/L- 1 )
IL/R/L+l)
SIGMA L- 1
SI GIIIA L+l
SIGMA (Mil)
.0000
.000
511.11117
207.80
1.779E-Ol
4.305i-Ol
5.085E-02
3.1171E-Ol
4.480E-Ol
2.0000
27.212
811.878
142.71
9.135E-02
2.52I1E-Ol
1.1153E-02
1.1181E-Ol
2.188E-Ol
4.0000
54.424
114.0eO
108.117
5.581E-02
I.1I80E-Ol
Il.572E-03
r , 157E-Ol
1.2521-01
Il.0000
81.1135
141.302
87.75
3.7117E-02
1.205E-Ol
5.400E-03
7.38~E-02
7 .1I0~E-02
14.0000
1110.483
250.1411
411.511
1.27I1E-02
4.1180E-02
1.0117E-03
1.1187E-02
2.077E-02
111.0000
217.11115
277.381
44.70
1.043E-02
3.908E-02
8.130E-04
1.521E-02
1.802E-02
20.0000
272.118
331 .785
37.37
7.320E-03
2.83I1E-02
4.787E-04
Il.800i-03
1.008E-02
TE
XVI
lOF
EO'
2.7543E+00 (RYD)
N·· '11.11408
MU'
.35112
E (RYD)
E (EV)
E PHOT (EV)
LAMIIDA (A)
IL/R/L-l)
IL/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
37.475
330.85
2.98I1E-Ol
5.81I1E-Ol
8.III1I1E-02
4.553E-Ol
5.452E-Ol
2.0000
27.212
114.1187
191 .117
1.14I1E-Ol
2,7321-01
2.287E-02
1.733E-Ol
1.11112E-Ol
4.0000
54.424
111.8119
134.112
Il.10lE-02
1,1I34E-Ol
Il.213E-03
8.810E-02
Il.731E-02
8.0000
108.847
1411.323
84.73
2.5112E-02
7.1185E-02
2.1147E-03
3.334E-02
3,5118E-02
14.0000
190.483
227.1158
54.311
1. 115E-02
3.838E-02
7,1I2I1E-04
1.2081-02
1.282E-02
111.0000
217.8115
255. 170
48.511
8.1150E-03
3. 1113E-02
5.505E-04
Il.18I1E-03
Il.7I!iIE-03
TE XVI
12F
EO'
1.88112E+00 (RYD)
-
N·· 11.1I401l
MU'
.35111
E (RYD)
E (EV)
E PHOT
(EV)
LAMBDA (A)
(L/R/L-l1
(L/R/L+ 1)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
25.704
482.311
4.45I1E-Ol
7.42'E-Ol
1.375E-Ol
5.0114E-Ol
Il.488E-Ol
2.0000
27.212
52.11111
234.31
1.2117E-Ol
2.7!l!lE-Ol
2. 287E -02
1.442E-Ol
1.117lE-Ol
4.0000
54.424
80.128
154.74
Il.037E-02
1.50IlE-Ol
7.8115E-03
Il.551E-02
7.337E-02
8.0000
108.847
134.551
112.15
2.332E-02
Il.828E+02
1 .1171 E- 03
2.2521-02
2.450E-02
12.0000
1113.271
188.975
115.111
I.227E-02
3.1143E-02
7. 118llE -04
1.0SSI-02
1.132E-02
14.0000
1110.483
2111.187
57.35
9.475E-03
3. 151 E-02
5.227i-04
7.708E-03
8.228E-03
TE
XVI
1IIF
EO'
1.04114E+00 (RYD)
N.· 15.1140.
MU'
.35111
E IRYD)
E IIV)
1 PHOT
(EV)
LAMBDA (Al
(L/R/L-l)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA (MB)
.0000
.000
14.238
870.82
8.13111-01
1.018E+00
2.540E-Ol
Il. 145E-Ol
8.1185E-Ol
2.0000
27.212
41.450
21111.13
1.288E-Ol
2.52U-Ol
1.847E+02
Il.4112E-02
1 . 134E -0 1
4.0000
54.424
118.11111
180.58
5.24I1E-02
1.218E-Ol
5.088E-03
3.1I111E-02
4.170E-02
10.0000
1311.0511
150.2117
82.4.
1.240E-02
3.8I1lE-02
Il.228E-04
7.2341-03
7.858E-03
18.0000
244.11011
2511, 144
47.84
4.34lE-03
1.471E-02
1.315E-04
2.0351-03
2. l1111E -03
20.0000
272.118
2811.358
43.30
3.583E-03
1.243E-02
Il.788E-05
1.58eE-03
1.118I1E-03
TE
XVI
20F
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1.11I1E+00
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342.12
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1 .342E-02
Il.213E-02
7.5SSE-02
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Il.738E-02
3.225E-03
2.181E-02
2.483E-02
8.0000
108.847
117.8711
105.18
1.402E-02
3.815E-02
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Il.1111E-03
Il.785E-03
111.0000
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XVII
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27.212
278.444
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108.847
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3.28se-02
4.149E-02
XVII
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1. 11S1I0E+0 1 (AYD)
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2. 113E-02
4.1140E-02
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3.720E-02
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30.72
2.0331-02
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XVII
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80.379
154.215
1.890E-Ol
1.414E-Ol
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2.0000
27.212
107.591
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, .004E-Ol
3.044E-02
4.541E-02
7.585E-02
8.0000
108.847
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85.52
4.507E-02
4.9721 -02
8.051E-03
1.geOE-02
2.715E-02
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217.895
298.073
41.1S0
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2.780E-02
2.738E-03
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1.225e-02
XVII
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L-l
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48.544
21111.41
3.110E-Ol
1.984E-Ol
8.835E-02
7.843E-02
1.71S8E-Ol
2.0000
27.212
75.751S
'83.87
1. 4 78E -0 1
1. 144E -0 1
3.4114E-02
4.155E-02
7.81IE-02
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81.lS35
130. '80
911.24
5.934E-02
5.7421-02
9.1S02E-03
1.788E-02
2.7511-02
10.0000
138. ou
184.1103
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3. 284E -02
3.838E-02
4. 1 7U -03
1. 024E -02
1.44U-02
12.0000
183.271
211.815
58.54
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3.0341-02
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8.170E-03
1.117E-02
71
XVII
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E (AYDI
E (EV)
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(L/A/L - 1)
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SIGMA L-l
SIGMA L+l
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32.480
381.73
4.804E-Ol
2.585E-Ol
1. 442E-0 1
8.1152E-02
2.338E-Ol
2.0000
27.212
511.8112
207.71
1.882E-Ol
1.203E-Ol
3.452E-02
3.820E-02
7.072E-02
8.0000
81.835
114.115
108.85
5.55I1E-02
5.182E-02
7.388E-03
1.284E-02
2.022E-02
8.0000
108.847
141.327
87.73
3.888E-02
3.1I05E-02
4.425E-03
Il.031E-03
1.348E-02
18.0000
217.8115
250.175
411.58
1. 483E -02
1.821E-02
1. 121 E-03
3.475E-03
4.5118E-03
18.0000
244.1108
277.388
44.70
1.227E-02
1.5UE-02
8.744E-04
2.1117E-03
3.7112 E-03
XV Il
18P
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1.2835E+00
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E (AYO)
E (EV)
E PHOT ( EV)
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(L/A/L-l)
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SIGMA L- 1
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17.483
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8.381E-Ol
3.111 OE- 0 1
2.58I1E-Ol
1.11SE-Ol
3.887E-Ol
1.0000
13.808
31.0811
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3. 1118E- 0 1
1.877E-Ol
6.848E-02
4.583E-02
1.123E-Ol
4.0000
54.424
71.887
172.47
7.754E-02
6'.203E-02
Il.053E-03
1.15I1E-02
2.084E-02
8.0000
81.835
1111.01111
125.11
4.4114E-02
4.038E-02
4.1113E-03
6.782E-03
1.0115E-02
12.0000
183.271
180.734
88.80
1.813E-02
1 . 7115E-02
Il.853E-04
2.440E-03
3.428E-03
18.0000
244.1108
282.370
47.28
8. 534E -03
1 . 083E - 02
4.003E-04
1.28I1E-03
1.8110E-03
XV Il
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SIGMA L- 1
SIQIIIA L+l
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10.885
11311.08
1.318E+00
5.432E-Ol
3 .1I51E -0 1
1.348E-Ol
5.2117E-Ol
1.0000
13.808
24.481
508.28
3.385E-Ol
1.882E-Ol
5.87I1E-02
3.832E-02
Il.51 1E-02
4.0000
54.424
85.308
1811.85
8.448E-02
5.042E-02
5.88SE-03
8.1154E-03
1.284E-02
10.0000
138.0511
148.1144
84.38
1.81I1E-02
1.880E-02
8.088E-04
1.737E-03
2.544E-03
18.0000
217.8115
228.5711
54.24
7.805E-03
Il.20IlE-03
2. 7811E-04
8.121E-04
1.08I1E-03
XV Il
50
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1.8070E+Ol
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E (AYD)
E (EV)
E PHOT (EV)
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SIGMA L- 1
SIQIIIA L+l
SIGMA
(MB)
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218.845
58.71
5. 827E -02
1.05I1E-Ol
1.740E-02
Il. 2311E-02
1.0118E-Ol
2.0000
27.212
2415.857
50.43
4.805E-02
Il.427E-02
1 .311 E- 02
8.238E-02
Il.54I1E-02
8.0000
81.838
300.280
41.211
3.288E-02
7.584E-02
8.0501-03
8.512E-02
7.317E-02
18.0000
244.1108
483.551
28.75
1 .531 E - 02
4.413E-02
2.732E-03
3.403E-02
3.878E-02
XV Il
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1.0433E+Ol
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N·· 5.2832
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SIGMA L - 1
SIQIIIA L+l
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141.1147
87.35
Il.038E-02
1.270E-Ol
2.1114E-02
8.828E-02
1. 154E-0 1
2.0000
27.212
1811.1511
73.30
6.8110E-02
1.074E-Ol
1.1I03E-02
7.352E-02
Il.255E-02
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81.835
223.583
55.45
4. 131 E - 02
·7.1185E-02
Il.5113E-03
5.348E-02
8.307E-02
12,0000
183.271
305.218
40.82
2.311I1E-02
5.411I1E-02
4.418E-03
3.47I1E-02
3.1121E-02
XVII
80
EO' 5.4548E+00
(AYD)
N·· 7.27811
MU'
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E (AYD)
E (Ev)
E PHOT (EV)
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SIGMA L - 1
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(MB)
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74.215
187.011
1.80IlE-Ol
1. 885E-0 1
8.083E-02
7.141E-02
1.402E-Ol
2.0000
27.212
101.427
122.24
1.057E-Ol
1.254E-Ol
2.8!50E-02
8.012E-02
8.882E-02
Il.0000
81.835
155.850
711.55
5.025E-02
7.877E-02
Il.8II0E-03
3.848E-02
4.835E-02
10.0000
138.0811
210.274
58.118
2.1174E-02
5.523E-02
4.874E-03
2.418E-02
2.888E-02
XVII
100
EO' 3.3524E+00
(AYD)
N·· Il.2848
MU'
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E (AYD)
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/A/L-l)
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SIGMA L - 1
SIGMA L+ 1
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(Mil)
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45.1112
271. 83
2.1183E-Ol
2 ..07I1E-Ol
1. 020E-0 1
7.438E-02
1.784E-Ol
2.0000
27.212
72.824
170.25
1.34lE-Ol
1.332E-Ol
3.2I1lE-02
4.88I1E-02
8.15I1E-02
8.0000
81.835
127.248
117.44
5. 101 E -02
7.1114E-02
8.322E-03
2.483E-02
3.315E-02
12.0000
183.271
208.883
511.38
2.134E-02
3.1141E-02
2.3112E-03
1.223E-02
1.482E-02
111.0000
217.11115
283.307
47.011
1.41!IE-02
2.1127E-02
1.324E-03
8.508E-03
Il.830E-03
20.0000
272.118
317.730
311.02
1.011E-02
2.281E-02
8.182E-04
8.238E-03
7.05lE-03
XVII
120
EO' 2.2882E+00
(AYD)
N.' 11.2877
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SIGMA L- 1
SIGMA L+l
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30.881
401.75
4.42lE-Ol
2.453E-Ol
1. 518E -01
7.004E-02
2.217E-Ol
2.0000
27.212
58.073
213.50
1. 504E -01
1 . 335E - 0 1
3.302E-02
3.1I0lE-02
7.203E-02
8.0000
81.835
112.4117
110.21
4.788E-02
6.357E-02
8.482E-03
1.714E-02
2.382E-02
10.0000
138.0511
188.1121
74.28
2. 311eE -02
3.1140E-02
2.407E-03
Il. 7811E-03
1.218E-02
18.0000
217.8115
248.588
411.88
1.182E-02
2.38I1E-02
8.722E-04
5.281E-03
8.133E-03
XVII
180
EO'
1.2381E+00
(AYDI
N·· 115.21103
MU'
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E (AYD)
E (EV)
E PHOT ( EV)
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SIGMA L-l
SIQIIIA L+l
SIGMA (M8)
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18.8111
737.20
8.043E-Ol
3.142E-Ol
2.735E-Ol
8.25I1E-02
3.381E-Ol
2.0000
27.212
44.030
281.511
1.588E-Ol
1.222E-Ol
2.712E-02
2.481E-02
5.1113E-02
4.0000
54.424
71. 242
174.03
il. 8211E -02
7.10IlE-02
8.351E-03
1.357E-02
2.1112E-02
8.0000
81.835
118.454
125.113
3.8110E-02
4.854E-02
3.744E-03
8.748E-03
1 . 2411E-02
12.0000
183.271
180.0110
88.85
1.344E-02
2.211I1E-02
8.175E-04
3.58I1E-03
4.407E-03
18.0000
244.1108
281.725
47.37
8.811I1E-03
1.412E-02
3.131E-04
1.1187E-03
2.280E-03
XVII
200
EO' 7.7854E-Ol
(AYD)
N·· 111.21115
MU'
.7085
E (AYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/A/L-l)
(L/A/L+l)
SIGMA L - 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
10.588
1173.411
1.282E+00
3.754E-Ol
4.228E-0;
5.813E-02
':.78I1E-Ol
2.0000
27.212
37.777
328.20
1.451 E -0 1
1. 08 lE -0 1
1.III1I1E-02
1. 802E -02
3.801E-02
4.0000
54.424
84.11811
1110.78
5.8118E-02
5.8118E-02
5.211I1E-03
7.1158E-03
1.325E-02
10.0000
138.0511
148.825
84.58
1.372E-02
2.11I1E-02
6.1138E-04
2.481E-03
3.175E-03
18.0000
244.1108
255.472
48.53
5.107E-03
1.031E-02
1.875E-04
1.025E-03
1.1112E-03
72
XV Il
4F
EO· 2. 199&E+0 1 (AYD)
N.· 3.11248
MU'
.37152
E (AYDI
E lEV)
E PHOT (EV)
L.AMBDA
(A)
(L./R/L.-Il
(L./R/L.+')
SIGMA L. - 1
SIGMA L.-l
SIGMA
(MB)
.0000
.000
2ee.271
41.43
2.139E-02
1 . 330E - 0 1
3.11UE-03
1.901E-Ol
1.937E-Ol
2.0000
27.212
328.483
37.98
1.82IE-02
1.11U-O'
2.915E-03
1.411810-01
1.498E-Ol
Il.0000
81.1135
380.907
32.55
1.3112E-02
8.205E-02
1 .90310 -03
9.2081-02
9. 39SE -02
14.0000
190.483
489.754
215. 32
8.3511E-03
4.885E-02
9.210E-04
4.1111110-02
4.288E-02
XVII
5F
EO'
1.3351E+Ol
(RYD)
N.· 4.115211
MU'
.3474
E (RYD 1
E (EV)
E PHOT (EV 1
L.AMBDA
( A)
{L./R/L.-ll
(L./R/L.-II
SIGMA L. - 1
SIGMA
L-l
SICMA
(Mal
.0000
.000
181.1147
118.211
4.511 E - 02
1 . 950E- 0 1
9.9!14E-03
2.481E-01
2.580E-Ol
2.0000
27.212
208.859
59.311
3.493E-02
1.544E-01
Il.882E-03
1.787E-01
1.851lE-Ol
8.0000
108.847
290.494
42.118
1.882E-02
8.1148E-02
2.770E-03
7.801E-02
8.078E-02
1'.0000
244.9011
4211.554
29.07
8.889E-03
4.214E-02
9.07SE-04
2.720E-02
2.81 lE-02
XVII
llF
EO' 8.0331E-00
(AYD)
N·· 5.115113
MU'
.3437
E (AYD)
E (EV)
E PHOT (EV)
L.AMBDA
(A)
(L/RIL-ll
(L./R/L.-ll
SIGMA L. - 1
SIGMA L-l
SlaMA
(MB)
.0000
.000
122.904
100.88
7.1138E-02
2.571E-Ol
1.93lE-02
2.9I1SE-Ol
3.IOU-Ol
2.0000
27.212
150.115
82.59
5.314(-02
1.890E-Ol
1.142E-02
1 .925~-01
2.039E-01
4.0000
54.424
177.327
119.92
3.912E-02
1.448E-Ol
7.307E-03
1.335E-Ol
1.409E-01
Il.0000
81.1135
204.539
110.112
2.998E-02
r . 145E-0 1
4.9111E-03
9.1527E-02
1.012E-01
12.0000
1113.271
2811.175
43.33
1.581 E-02
Il.4211E-02
1.9211E-03
4.244E-02
4.4311E-02
18.0000
244.8011
3117.810
33.71
9.115U-03
4. 082E -02
9.241E-04
2.201E-02
2.294E-02
XV Il
8F
EO. 4.'288E+00 (RYDI
N.· 7.11572
"'U·
.3428
E (RYDt
E ( EV)
E PHOT IEVI
L. ...MBDA
(A)
(L./R/L.-l )
(L/RIL- 1 )
SIGMA L.- 1
SIGMA L.- 1
SIGMA
(liB)
.0000
.000
117.083
184.88
1.597E-OI
3.858E-Ol
4.1107E-02
3.514E-OI
4.045E-Ol
2.0000
27.212
94.274
131.52
8.707E-02
2.371E-01
1.925E-02
1.904E-Ol
2.0911E-Ol
4.0000
54.424
121.4811
102.08
5. 4911E -02
1.1122E-Ol
9.883E-03
1.147E-Ol
1.2411E-Ol
Il.0000
81.835
148.11.8
83.31
3.788E-02
r , 185E-0 1
5.74H-03
7.483E-02
8.0117E-02
14.0000
"0.483
257.545
48.14
1.334E-02
4.7921 -02
1.235E-03
2.123E-02
2. 247E -02
111.0000
217.&85
284.757
43.54
1.091lE-02
4.0211E-02
9.219E-04
1 .1l58E -02
, .750E-02
XV!!
lOF
EO. 3.0987E+00
(RYD)
N.· Il.11573
MU'
.3427
E (AYD)
E (EV)
E PHOT' (EV)
L.AMaDA
( Al
(L./R/L. - 11
(L./R/L.-I)
SICMA L.-l
SJGMA L.+'
SIGMA
(Mil
.0000
.000
42.1111
294.08
2.1187E-Ol
5.233E-Ol
8. lUE -02
4.14!l1-01
4.9115E-0'
2.0000
27.212
119.373
178.72
1. 118E-01
2.1114E-Ol
2.3311E-02
1.702E-Ol
1.1I311E-Ol
4.0000
54.424
911.585
128.37
Il.11111E-02
1.111 OE-O 1
9.888E-03
8."5E-02
9. 97l5E-02
8.0000
108.847
151.008
82.11
2.705E-02
8.01111E-02
2.9711E-03
3.5411E-02
3.843E-02
14.0000
190.483
232.1144
53.29
1.188E-02
3.9811E-02
8.838E-04
1.327E-02
1 . 411lE -02
18.0000
244.9011
287.0118
43.19
7.872E-03
2.780E-02
4.7110E-04
7.9115E-03
8.444E-03
XV Il
12F
EO-
2.12117E+00
(AYDI
H.· 11.11573
MU'
.3427
E (RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
IL./R/L.-n
(L/R/L-l)
SIGMA L.-1
SICMA
L.-l
SICMA
(MB)
.0000
.000
28.935
428.48
4.0111E-Ol
Il.704E-Ol
1.257E-Ol
4.1170E-Ol
5.127E-Ol
2.0000
27.212
511.147
220.82
1.21121-01
2.UU-Ol
2.407E-02
1.44.E-Ol
1.8110E-Ol
4.0000
54.424
83.35.
148.74
Il.222E-02
1.510E-Ol
8.1190E-03
Il.827E-02
7.1198E-02
8.0000
108.8.7
137.783
19.99
2.472E-02
7.017E-02
2.211IE-03
2.431!1E-02
2.11I3E-02
12.0000
U13.271
192.2011
114 .51
1.3181-02
4.11lE-02
8.989E-04
l.l118E-02
1.25&E-02
14.0000
190.483
219.418
511.51
1. 021 E-02
3.30lE-02
Il.1114E-0.
8.5UE-03
9.200E-03
XVII
18F
EO.
1.1789E-00 (RTD)
H·· 15.11573
MU·
.3427
E ( RYD)
E (EV)
E PHOT (IV)
L.AMBDA '(A)
(L./R/L.-ll
IL./A/L.-l)
SICMA
L-l
SlaMA L.+l
SIGMA
(Me)
.0000
.000
111.040
773.00
7.352E-01
Il.940E-Ol
2.335E-01
5.a.1E-Ol
8.028E-Ol
2.0000
27.212
43.251
2811.88
1.321E-OI
2.522E-Ol
2.034E-02
9.87IE-02
1.,9lE-Ol
4.0000
54.424
70.483
175.98
5.547[-02
1. 241SE-01
5. 83SE -03
3.928E-02
4.510E-02
10.0000
138.059
152.089
81.52
1. 348E -02
3.140E-02
7.420E-04
8.0153E-03
8. 795E -03
18.0000
217.895
233.734
53.05
5.904E-03
i . 89U -02
2. 194E-04
3.028E-03
3.245E-03
XVII
20F
EO-
7.4792E-Ol
(RYD)
H·· 19.8572
MU'
.3428
E (RYD)
E lEV)
E PHOT (EV)
LAM8DA
(A)
(L./R/L-l )
(L./A/L+l)
SlaMA L.-l
SIGMA L.+l
SIGMA
(MB)
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10.178
1218.41
1.155E+00
1.358E+00
3. 85:IE -0 1
8.720t-Ol
1.037t-00
2.0000
27.212
37.388
331.82
1.230E-01
2.221E-Ol
1.523E-02
8.823E-02
8. 140E-02
4.0000
54.424
84.800
191.93
4.B1l3E-02
1.00SE-Ol
3.782E-03
2.358E-02
2.735E-02
8.0000
108.847
119.023
104.17
1.528E-02
4.009E-02
7.4841-04
8.8118t-03
7.817E-03
14.0000
"0.483
200.859
81.79
5.1187(-03
1.738E-02
1.74SE-04
2.17&E-03
2.351E-03
18.0000
244.908
255.083
48.81
3. 584E -03
1.IIIU-02
8.724E-05
1.238E-03
, .324E-03
20.0000
272. 118
282.284
43.92
2.911SE-Oa
9.781E-03
8.4871-05
9.1I89E-04
1. 03 lE -03
73
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2.1871E+Ol
(AYD)
H"
3.848S1
MU'
1. 1511
E (AYD)
E (EV)
E PHOT (EV)
LAMBDA
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SIGMA L-l
SIGMA L+ 1
SIGMA (MB)
.0000
.000
2117.580
41.88
.000
5.755E-02
.000
8.1Sl3E-02
8.IUE-02
2.0000
27.212
324.7112
38.17
.000
5. 112 E- 02
.000
5.33I5E-02
5.335E-02
20.0000
272.118
5811.8118
21.78
.000
2.353E-02
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I.Sl82E-02
I.Sl82E-02
lIE lIVIII
8S
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1.3874E+Ol
(AYD)
H"
4.8878
MU'
1 . 1322
E (AYD)
E (EV)
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LAMBDA
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SIGMA L- 1
SIGMA L+I
SIGMA (MB)
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188.044
88.84
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8.33IE-02
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8. 115( -02
8.115E-02
2.0000
27.212
213.2115
158.14
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8.885E-02
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8.3152E-02
II. 352 E-02
20.0000
272. 118
458.182
27.08
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2.320E-02
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1.550(-02
1.550E-02
XE
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(AYD)
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8.8805
MU'
1.11S15
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SIGMA L- 1
SIGMA L+l
SIGMA (MB)
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113.118
133.15
.000
1.475E-Ol
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1.274E-Ol
1.274E-Ol
2.0000
27.212
120.32S1
103.04
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I.OI7E-Ol
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7.8251-02
7.825E-02
10.0000
138.05S1
2211.177
54.10
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3.114S1E-02
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2.248E-02
2.248E-02
20.0000
272. 118
3815.238
33.Sl5
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I.Sl88E-02
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SI.0152E-03
SI.052E-03
lIE
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8.88151
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1.114S1
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SIGMA L- 1
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515.841
222.04
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2.272(-01
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1.811 E -0 1
I.81IE-Ol
2.0000
27.212
83.053
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1.282E-Ol
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8.311E-02
8.31IE-02
8.0000
81.835
137.478
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5.U7E-02
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3.048E-02
3.048E-02
14.0000
ISlO.483
248.324
50.33
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2.475E-02
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SI.488E-03
SI.488E-03
XE XVIII
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10.8873
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37.1S11
333.38
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3.212E-Ol
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2.41li-01
2.41IE-OI
2.0000
27.212
lU .403
1_2.52
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1.408E-01
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8.023E-02
8.023E-02
8.0000
81.835
118.828
104.34
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5.588E-02
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2.3141-02
2.314E-02
12.0000
183.271
200.482
81.85
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2.520E-02
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7.Sl07E-03
7.SlSl7E-03
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1.1107
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1S1.8815
823.52
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5.501E-OI
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3.78IE-Ol
3.781E-OI
2.0000
27.212
47.0Sl7
283.28
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1.472E-OI
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8.40SlE-02
8. 40SlE -02
8.0000
81.835
101.521
122.13
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4.51S1E-02
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1.303E-02
1.303E-02
8.0000
108.847
128.732
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3.13S1E-02
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7.Sl72E-03
7.Sl72E-03
14.0000
ISlO.483
210.388
58.Sl4
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1.482E-02
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2.Sl04E-03
2.Sl04E-03
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18.8S101
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12.354
1003.82
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8.308E-Ol
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5.315S1E-OI
5.35S1E-Ol
2.0000
27.212
311.588
313.37
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4.88S1E-02
8.0000
81.835
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3.5S18E-02
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7.838E-03
7.838E-03
12.0000
183.271
175.825
70.80
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1.374E-02
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2.084E-03
XE XVIII
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277.583
44.87
5.437E-02
8.578E-02
1.71S1E-02
!l.032&-02
8.7!lIE-02
2.0000
27.212
304.7S15
40.88
4.870E-02
5.823E-02
1.3S12E-02
4.47S1E-02
!l.871E-02
8.0000
81.835
311S1.21S1
34.52
3.571E-02
4.8_U-02
SI.5S18E-03
3.808E-02
4.58I1E-02
18.0000
244.Sl08
522.4S10
23.73
1.1131E-02
3.003E-02
4.07S1E-03
2.0Sl4E-02
2.501E-02
XE XVIII
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.0000
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17!l.80!l
70.52
8.1584E-02
8.848&-02
2.7141-02
5.S0IlE-02
8.21S11-02
2.0000
27.212
203.017
81.01
8.7701-02
7.327E-02
1 . Sl4Sil -02
4.5881-02
8.518E-02
8.0000
108.847
284.852
43.18
3.888E-02
4.878&-02
8.Sl21E-03
2.838E-02
3.730E-02
18.0000
244.Sl08
420.712
2S1.47
2.018E-02
2.Sl77E-02
3.5S10E-03
1 . 582E -02
I.U1E-02
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7.0232
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SIGMA L+ 1
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.0000
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8S1.373
138.73
1.8S11E-Ol
1.3331-01
!l.31521-02
8.8114E-02
1.201E-Ol
2.0000
27.212
118.1185
108.35
1.088E-Ol
SI.884E-02
2. 87SIE -02
4.5.8E-02
7.48S1E-02
8.0000
108.847
1S18.220
82.!l5
4.4158E-02
4.11721-02
8.2!lOE-03
2.053E-02
2.878E-02
18.0000
217.8S1!l
307.088
40.38
2.131E-02
2. 801n -02
2. S120E -03
1.0115E-02
1. 307E -02
18.0000
244.Sl08
334.280
37.0Sl
1.848E-02
2.1511E-02
2.388E-03
8.827E-03
1.121E-02
XE XV 1 II
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(RYD)
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SI.028_
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22S1.28
2.77S1E-Ol
1.881E-Ol
8.74S1E-02
7.8I50E-02
1.880E-Ol
2.0000
27.212
81.287
1152.53
1.408E-Ol
1. 125E-Ol
3.388E-02
4.307E-02
7.873E-02
8.0000
81.83!l
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Sll.38
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!l.814E-02
SI. SlSI5E-03
I.U2E-02
2.121 E-02
10.0000
138.051
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8!l.21
3.3150E-02
3.72S11-02
4.470E-03
1.10U-02
1.!l!lIlE-02
12.0000
183.271
217.348
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2.870E-02
3.121E-02
3.2481-03
8.871E-03
1.2.12E-02
XE
XVIII
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2.8823E+00 (AYDI
N.· 11.0317
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7.280E-02
8.0000
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117.8118
1011.20
5.851E-02
5.328E-02
7.88"E-03
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2.1110E-02
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8.302E·03
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1. 858E -02
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2.273E-02
Il.0000
81. B311
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21.212
311.378
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5.328E-02
Il.2113E-03
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2.950E-02
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113.53
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131.01511
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2.7112E-02
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7.018E-Ol
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5.442
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1.370E-02
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2.837E-02
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10.885
23.11315
1524.58
1.311 1E-Ol
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1.150E-02
Il.825E-04
1.248E-02
1.0000
13.11011
211.351
470.42
1.218E-Ol
3.087E-02
Il.82I1E-03
Il.4721-04
1.077E-02
2.0000
2.7.212
311.11112
310.211
7.258E-02
1.314E-Ol
5.288E-03
2.11021-02
3. 130E-02
4.0000
54.424
117.174
184.57
3.704E-02
1.225E-Ol
2.317E-03
3.80lE-02
4.0331-02
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81 . 1135
114.3811
131.311
2.344E-02
Il.1173E-02
1.3031-03
3.3301-02
3.480E-02
8.0000
108.847
12 1 . 5118
101.1111
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7.1184E-02
8.31I1E-04
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4.373E-Ol
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1.1121E+00
1.1188E+00
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1.3111
8.1105
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3.530E-Ol
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2.104E-02
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13.11011
20.850
5114.85
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7.451E-03
1.3541-03
8.805E-03
2.0000
27.212
34.4511
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Il. 2811E-02
8.827E-02
3.42I1E-03
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1.782E-02
1.1113E-02
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88.880
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Il.833E-02
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1.5114E-02
1.1134E-02
8.0000
108.847
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5.373E-02
4.211I1E-04
1.2114E-02
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3.223E-Ol
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2.28I1E-02
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5.212E-03
3. 1211E-03
8. 311SE -03
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31.8110
388.711
5.233E-02
Il.372E-02
2.1115E-03
4.883E-03
7.078E-03
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Il.574E-02
7.77lE-04
Il.1130E-03
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143.115
1.353E-02
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3.1175E-04
8.450E-03
8'. 847E -03
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108.847
113.5211
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Il.178E-03
3.118I1E-02
2.404E-04
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2.1153E-03
3.01lIlE-03
5.71I1E-03
1.5000
20.4011
22.824
543.22
5.148E-02
1.482E-02
1.520E-03
1.8110E-04
1.70IlE-03
2.0000
27.212
211.827
418.411
3.1151E-02
3.85I1E-02
Il.1I25E-04
1.11113E-03
2.115I1E-03
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40.818
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2.1115E-02
4.550[-02
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511.8311
218.14
1.50IlE-02
4.155E-02
3.251E-04
3.701E-03
4.02IlE-03
5.0000
118.030
70.445
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1.11I1E-02
3.1153E-02
2.21I1E-04
3.544E-03
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3.278E-02
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12.3511
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8.408E-03
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1.448E-03
2.0118E-03
3.54I1E-03
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20.4011
21.881
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3.824E-02
8.051E-03
8.041 E-04
5.347E-05
8.57I1E-04
2.0000
27.212
28.1184
432.211
2.1172E-02
2.848E-02
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7.581 E- 04
1.273E-03
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1.58lE-02
3.188E-02
2.115I1E-04
1.112lE-03
1.887E-03
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54.424
55.8115
221.82
1.077E-02
2.1112E-02
1 . 11211E - 04
i . 787E -03
1 .1I411E -03
5.0000
118.030
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178.311
7.1141E-03
2.558E-02
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1.822E-03
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Il.1I32E-03
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13.11011
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8.5115E-04
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2.245E-03
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20.4011
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2511L 38
-1.25I1E-Ol
5.150E-00
2.08I1E-03
4.1117E-00
4.118I1E-00
.01100
.8111
5.738
21110.112
-1.1I27E-02
3.754E-00
7.414E-04
2.1I04E-00
2.1I05E-00
.1000
1 .311 1
Il.212
11173.71
-4.521E-02
3.104E-00
3. 45eE -04
2.174E-00
2. 174E-00
.2000
2.721
7.1142
11122.33
-1. 053E -02
2.03I1E-00
2.282E-05
1. 14lE+00
1.141E-00
.4000
5.442
10.3114
111111.35
1.2112E-02
1.037E-00
4.448E-05
4.000E-Ol
4.001E-Ol
.11000
8. 1114
13.085
1147.511
1 .1181 E- 02
Il.01lIlE-Ol
Il.1I53E-05
1.72I1E-Ol
1.730E-Ol
.8000
10.885
15.8011
784.42
1.1121 E-02
3.887E-Ol
1.11I1E-04
8.574E-02
8.585E-02
1.0000
13.1I01l
18.527
111111.21
1.445E-02
2.115I1E-Ol
1.042E-04
4.11114E-02
4.705E-02
2.0000
27.212
32.133
381l.85
7.070E-03
Il.882E-02
4.32I1E-05
5.411I1E-03
5.50IlE-03
4.0000
54.424
511.345
208.112
2.302E-03
1.520E-02
8.472E-OII
4. 11211E - 04
5.011E-04
G'" 1 Il
IIF
EO·
2.5 11 liE - 01
(RYOI
N.· 5.118112
MU·
.0138
E ( RYO)
E (EV)
E PHOT (EV)
L. ...MIlD... lA)
(L./R/L.-I)
(L./R/L.-l)
SIClM... L. - 1
SIGM... L.-l
SIGM... (MIS)
.0000
.000
3.417
31128.31
-3.035E-Ol
7.1122E-0(\\
8.47I1E-03
7.128E-O<l
7.137E-00
.01100
.8111
4.234
21128.1111
-1. !l73E-Ol
5.077E·00
2.822E-03
3.918E-00
3.1121E-00
.2000
2.721
Il.138
20111.85
-3. 12!lE-02
2. 428E -00
1 .1115E -04
1.300E-00
1.300E-00
.4000
5.442
8.8110
131111.411
Il.84I1E-03
1.124E-00
2.313E-05
4.021E-Ol
4. 02 lE -0 1
.11000
8. 1114
1 1 .1l8 1
1070.112
1 . 11711E - 02
Il.243E-Ol
8.7117E-05
1.1121E-Ol
1.1122E-Ol
.8000
10.885
14.302
81111.112
1.1148E-02
3.870E-Ol
1.04I1E-04
7.1I111E-02
7.70lE-02
1.0000
13.11011
17.023
728.34
1.41l8E-02
2.584E-Ol
Il. 7411E-05
4.082E-02
4.0112E-02
2.0000
27.212
30.11211
404.80
Il.7113E-03
Il.332E-02
3.807E-05
4.40IlE-03
4.447E-03
4.0000
54.424
57.841
214.311
2.118E-03
1.3!l2E-02
Il.118I1E-OII
3.7115E-04
3.8115E-04
18
GA Il 1
8F
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1.41111E-OI
( AYDt
N·· 7.9841
MU·
.01511
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E lEV 1
E PHOT (EV 1
LAMBDA
(Al
(L/A/L-II
(L/A/L+11
SIGMA L - 1
SIGMA L+l
SIGMA (MBI
.0000
.000
1.1121
8454.41
-1I.253E-Ol
1.313E+Ol
4.~2I1E-02
1.188E+Ol
1.1113E+Ol
.0200
.272
2.1113
5853.54
-8.728E-Ol
i . 048E+() 1
2.874E-02
8.8'3E+00
8.&40E+00
.1000
1.381
3.282
3778.211
-2.288E-Ol
5.115E+00
4.548E-03
3.0B3E+00
3.087E+00
.2000
2.721
~. 842
2870.ee
-8.804E-02
2.875E+00
5.788E-0~
1.1113E+00
1.1113E+00
.4000
5.442
7.383
1883.84
3.257E-03
1.072E+00
2. 104E - 08
3.040E-Ol
3.041E-Ol
.8000
8.184
10.085
12211.47
1 . 388E -02
5.548E-Ol
5. 217E - O~
t , 115E-Ol
1.115E-Ol
.8000
10.885
12.808
1188.21
1.418E-02
3.2117E-Ol
8.1117E-05
4.11119E-02
5.008E-02
, .0000
13.808
15.527
7118.53
1.247E -02
2.141E-Ol
8.500E-05
2.558E-02
2.582E-02
2.0000
27.212
211.133
425.511
5.510E-03
4.1121E-02
2.382E-0~
2.533E-03
2.557E-03
3.0000
40.818
~2.731
210.10
2.814E-03
1.982E-02
9.114E-08
5.1I07E-04
5.1118E-04
4.0000
54.424
58.3.5
220.05
1 . 842E -03
1.0 13E - 02
4.0113E-08
2. 075E -04
2.118E-04
GA Il 1
lOF
EO' Il.0304E-02
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N.· Il.11831
MU-
.01811
E 1RYD)
E (EV 1
E PHOT (EV 1
LAMBDA
1A)
IL/R/L-')
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SIGMA L - 1
SIGMA L+l
SIGMA (M81
.0000
.000
1.2211
100111. 07
-1.1128E+00
1 .1I3I1E+0 1
1.230E-Ol
1. 8511E+Ol
1.871E+Ol
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.272
1.501
8281.311
-1.238E+00
1. 3115E+0 1
8.111I1E-02
1.04I1E+Ol
1.055E+Ol
.0800
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2.045
8082.81
-5.1144E-Ol
8.282E+00
I.U8E-02
5.038E+00
5.058E+00
.1000
1.381
2.5811
4788.47
-3.217E-Ol
5.4118E+00
7. 217E - 03
2.810E+00
2.817E+00
.2000
·2.721
3.1150
31311.01
-8.700E-02
2.582E+00
8.051 E-04
Il.307E-Ol
Il.318E-Ol
.4000
15.442
8.871
1858.58
-8.223E-04
Il.323E-Ol
8.1157E-08
2.082E-Ol
2.082E-Ol
.8000
8.184
1.3112
1320.10
1.08I1E-02
4.823E-Ol
2.1lIl8E-05
7.208E-02
7.21 1E-02
.8000
10.885
12.113
1023.55
1.150E-02
2.883E-Ol
4.317E-05
3.132E-02
3.138E-02
1.0000
13.808
1~.835
835.71
1.012[-02
1.718E-Ol
4.0112E-05
r , 581lE -02
1.573E-02
2.0000
27.212
28.Ul
435.15
4.358E-03
3.817E-02
1.455E-05
1 .•88E-03
1.502E-03
3.0000
40.818
42.048
2114.8B
2.111I1E-03
1.504E-02
5.475E-08
3.415E-04
3.48I1E-04
GA III
12F
EO-
8.2882E-02
(RYD)
N.- 11.11828
MU·
.0174
E fAYDI
E (EV 1
E PHOT (EV 1
LAMBDA
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SIGMA L· 1
SIGMA L+I
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.000
.853
14838.02
-3.328(+00
2.841E+Ol
2.541E-Ol
2.138E-Ol
2.181E+Ol
.0800
.818
1.8811
7427.110
-7.574E-Ol
8.809E+00
2.57I1E-02
4.851E+00
~.877E+00
.1000
1.381
2.213
5801.54
-3.755E-Ol
5.U7E+00
8.405E-03
2.358E+00
2.387E+00
.2000
2.721
3.574
34811.10
-1I.235E-02
2.328E+00
8.210E-04
8.UIE-Ol
8.1149E-Ol
.~OOO
5.442
8.2115
11811.54
-2.450E-03
7.131E-Ol
1 .01 8E -08
'.422E·-Ol
1.422[-01
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8.1&4
1.018
1375.12
8.84llE-03
3.830E-Ol
t . 818E - 05
4. 7411E-02
4.750E-02
.8000
10.885
Il.738
1058.32
Il.388E-03
2.1111 E-O 1
2. 773E -05
2.024!-02
2.027E-02
t.OOOO
13.808
14.4511
857.52
8.250E-03
1.38I1E-Ol
2.850E-05
t , 002E -02
1.008E·-02
2.0000
27.212
28.085
44' .711
3.4118E-03
3.032E-02
Il.240E-08
9.2B2E-04
1.354E-04
3.0000
40.818
41.871
2117.54
1. 748E -03
1.187E-02
3.431E-08
2.107E-04
2.141E-04
4.0000
54.42~
55.277
224.30
1.007E-03
8.084E-03
1. 50llE -06
7.300E-05
7.450E-05
GA III
18F
EO·
3.5235E-02
( RYD)
N.· 15.9821
MU-
.01711
E (RYDI
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l)
SIGMA L-'
SIGMA L+l
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.0000
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25882.42
-7.321E+00
4.289E+Ol
8.91I1E-Ol
3.132E+Ol
3.202E+Ol
.0200
.272
.752
18497.115
-2.972E+00
2.0114E+Ol
1.787E-Ol
I.183E+Ol
1.201E+Ol
.0800
.818
1.2118
11588.80
-1I.122E-OI
8.852E+00
2.904[-02
3.483E+00
3.512E+00
.1000
1.381
1.840
8738.311
-3.1181E-Ol
4.813E+00
7.774E-03
1.530E+00
1.538E+00
.2000
·2.721
3.201
3873.88
-8.515E-02
1.831E+00
8.24I1E-04
3.853E-Ol
3.851ll-01
.4000
5.442
5.1122
2013.74
-3.335E-03
5.785E-Ol
r • 774E -08
7.118E-02
7.118E-02
.8000
8.184
8.843
1434.54
5. 828E -03
2.713E-Ol
7.1I02E-08
2.284E-02
2.288E-02
.8000
10.885
11. 38~
10111.03
8.4112E-03
1.52I1E-Ol
1.2110E-0~
9.538E-03
Il.54I1E-03
1.0000
13.80e
14.085
880.25
5.725E-03
Il.800E-02
1.243E-05
4.881E-03
4.874E-03
1.5000
20.409
20.888
5113.57
3.883E-03
3.1158E-02
7.5~8E-08
1.17~E-03
1 . 181 E-03
2.0000
27.212
27.8111
447.75
2.318E-03
2.055E-02
4.288E-06
4.199E-04
4.241E-0~
GA 111
20F
EO-
2.2541E-02
(RYO)
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MU-
.0182
E (AYOI
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lA)
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40427.17
- 1.2111E+Ol
8.175E+Ol
I.378E+00
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4.337E+OI
.0100
.138
.443
28003.70
-8.371E+00
3.471E+Ol
4.83I1E-Ol
1 .1I18E+0 1
1.1184E+Ol
.O~OO
.544
.851
14570.73
-1.878E+00
1.228E+Ol
8.454E-02
4.5113E-00
4.857E+00
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1.088
1 .3115
8888.88
-5.573E-Ol
5.480E-00
1 . 187E - 02
1.4113E-00
1.505[+00
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1.381
1.887
7438.43
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4.052E+00
5 .1I58E - 03
Il. 832E -01
Il.8111E-OI
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2.721
3.028
40114.83
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1.442E+00
4. 258E -04
2.281E-Ol
2.288E-Ol
.4000
5.~42
5.7411
2158.84
-3.041E-03
4.375E-Ol
1.432E-08
3.1181E-02
3.1151E-02
.8000
8.184
8.470
14B3.711
4.237E-03
2.022E-Ol
4.0118E-08
1.244E-02
1.244E-02
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10.885
1 1. 1111
1107.87
4.780E-03
1.131E-Ol
8.887E-08
5. I~OE-03
5.148E-03
1.0000
13.808
13.1113
8111.18
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7.08I1E-02
8.713E-08
2.4118E-03
2.803E-03
1.5000
20.4011
20.718
518.52
2.850E-03
2.888E-02
3.1118E-08
8.205E-04
8.244E-04
17
GE IV
4S
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2.2374
MU'
1.711211
t
(RYD)
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.0000
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2811.12
.000
2. 38 lIE -01
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1.5117E-Ol
1.51171-01
1.0000
13.8011
57.082
217.17
.000
1.8117E-Ol
.000
1.250E-Ol
1.250E-Ol
2.0000
27.212
70.1188
1711.38
.000
1.488E-Ol
.000
8.832E-02
8.832E-02
8.0000
8 1 . 113!
125.121
88.08
.000
7.575E-02
.000
4.511E-02
4.511E-02
GE IV
55
EO-
1.5028E+00 (RYD)
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3.21128
MU'
1.7372
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LAM8DA
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CL/R/L-l)
IL/R/L-l )
SIGMA L-l
SlaMA L-l
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.0000
.000
20.448
11011.33
.000
4.0!2E-Ol
.000
2.108E-Ol
2.108E-Ol
1.0000
13 .11011
34.0515
3ll4.08
.000
2.387E-Ol
.000
1.220i-Ol
1.220E-Ol
2.0000
27.212
47.1180
280.1!
.000
1.585E-Ol
.000
7.81I1E-02
7.1I1I1E-02
8.0000
81.53!
102.084
121.411
· 000
5.8117E-02
.000
2.284E-02
2.284E-02
12.0000
1113.271
183.720
87.48
.000
2.748E-02
. 000
8.718E-03
8.718E-03 .
GE IV
liS
EO' 8.7708E-Ol
(RYD)
N.·
4.2711
MU'
1.7288
E (RYD)
E lEV 1
E PHOT (EV)
LAM8DA
(A)
IL/R/L-l )
(L/R/L-l)
SIGMA L- 1
SIGMA L-l
SIGMA (M8)
.0000
.000
11.834
1038.8·7
.000
5.832E-Ol
.000
2.838E-Ol
2.838E-Ol
1.0000
13.8011
25.538
485.47
.000
2.548E-Ol
.000
1.042i-Ol
1. 042E-Ol
2.0000
27.212
38.145
3111.73
.000
1.481E-Ol
.000
5.382E-02
5.382E-02
8.0000
108.847
120.781
102.8!
.000
3.287E-02
.000
8. 08U-03
8.088E-03
18.0000
217.118!
228.1128
53.'8
.000
1.383E-02
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2.758E-03
2.758E-03
GE IV
es
EO- 4.01l08E-Ol
(RYD)
N.·
Il.2771
MU'
1.7228
E (RYD)
E (EV)
E PHOT (EV)
LAM8DA
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(L/R/L-l)
(L/R/L-l)
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.0000
.000
5.525
2244.08
· 000
1.0281-00
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3.852E-Ol
3.8!2E-Ol
1. 0000
13.1108
18.131
848.08
.000
2.313E-Ol
.000
Il.428E-02
8.428E-02
4.0000
!4.424
58.848
2011.82
· 000
4.808E-02
.000
8.078E-03
8.078E-03
8.0000
108.847
114.372
108.41
.000
2.011 E-02
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2.80U-03
2.808E-03
aE
IV
105
EO' 2.3342E-Ol
(RYDI
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8.2782
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1.7208
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(L/R/L-l)
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SIOMA L- 1
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SIGMA (MS)
.0000
.000
3.1711
3803.83
.000
1.527E-00
.000
4.11521-01
4.1152E-Ol
.5000
Il.803
Il.'78
1242.48
.000
3.802E-Ol
.000
'.053E-02
SI.083E-02
1. 0000
13.11011
18.782
738.81
.000
I.Sl05E-Ol
.000
3.82111-02
3.82I1E-02
4.0000
54.424
57.800
21!.28
.000
3.474E-02
.000
4.388E-03
4.3118E-03
GE IV
12S
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1.5140E-Ol
(RYD'
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10.2802
MU'
1.7188
E (RYD)
E (EV)
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LAM.OA (A)
(L/R/L-1)
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SIGMA L- 1
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.0000
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2.0ao
11018.07
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2.002E-00
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5. 1184E -0 1
5.884E-Ol
.4000
5.442
7.502
11152.115
.000
4.178E-Ol
.000
8.235E-02
8.235E-02
1.0000
13.11011
15.1188
781.4!
.000
1.548E-Ol
.000
2.358E-02
2.358E-02
2.0000
27.212
28.272
.23.!7
.000
8.523E-02
.000
7.82I1E-03
7.82I1E-03
4.0000
54.424
58.48-4
218.51
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2. 5S18E-02
.000
2. 3911E-03
2.388E-03
GE IV
1115
EO'
7.8451E-02
(RYDI
N.· 14.2811
MU'
1.7188
E (RYD)
E (EV)
E PHOT (IV)
LAM8DA
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(L/R/L-l)
(L/R/L-1)
SIGMA L-l
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SIGMA (M15 )
.0000
.000
1.0117
111115.78
.000
3 .• 01E-00
.000
7.7110E-Ol
7.7110E-Ol
.2000
2.721
3.788
3272.84
.000
Il.725E-Ol
.000
1.077E-Ol
i . 077E-Ol
.4000
5.442
Il.510
1804.112
.000
3.234E-Ol
.000
•. 278E-02
4.278E-02
1.0000
13.808
14.1173
844.88
.000
1 .057 E- 01
.000
1 . 030E -02
1. 030E -02
2.0000
27.212
28.27'
438.44
.000
4.22I1E-02
.000
3.178E-03
3.178E-03
GE IV
20S
EO' 4.78741-02
(RYD)
N".
18.2815
MU'
1 . 7185
E (RYD)
E 1 EV1
E PHOT (EV)
LAM8DA
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IL/R/L-l1
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S l'CMA L- 1
SIGMA L-I
SIGMA (M8)
.0000
.000
. 1151
18034.78
.000
4.Sl38E-00
.000
8.Sl71E-01
SI.871E-Ol
.1000
1.381
2. 012
111112.47
.000
1.13I1E+00
.000
1.1132E-Ol
l.e32E-Ol
.2000
2.721
3.373
3e7e.34
.000
5.e28E-Ol
.000
Il.712E-02
e.712E-02
.eooo
8.1e4
8.815
140e.5!
.000
1.487E-Ol
.000
1.24H-02
1.2.'E-02
.8000
10.885
1'.53e
1074.77
.000
1.0301-01
.000
7. e8eE-03
?888E-03
1.0000
13.eoe
14.257
U8 . ll4
.000
7.88S1E-02
.000
5.288E-03
5.2118E-03
GE IV
4P
10' 2.5183E-00 ( RYD)
Na.
2.521e
MU'
1.4784
E (RYD,
E (EV)
E PHOT (IVI
LAM8DA
(Al
(L/R/L-l)
(L/R/L-l )
SI G111A L- 1
SIGMA L-l
SIGMA (M81
.0000
.000
34.238
3e2.15
4.eOOE-Cl
-1.e23E-Ol
1.517E-Ol
3.778E-02
1.885E-Ol
.4000
5.4042
38.e78
312.48
3.e2!E-Ol
-e.5110E-02
1.0112E-Ol
7.1541-03
1.le3E-Ol
.eooo
8.184
.2.400
282.42
3.257E-Ol
-3.428E-02
SI.4181-02
2.0eeE-03
SI.e28E-02
.8000
10.885
4!. 121
274.78
2.8451-01
- 1 . 0321-02
8.200E-02
2.012E-04
8.220E-02
1. 0000
13.eOe
47.842
2!18.18
2.1180E-Ol
8.1801-03
7.1S17E-02
1.341 E-04
7.210E-02
1.2000
18.327
50.5e3
245.21
2.4511-01
2.254E-02
e.3831-02
i . 078E -03
Il.471E-02
1.4000
18.048
53.284
232.88
2.252E-Ol
3.374E-02
5.8e2E-02
2.541E-03
5.81ee-02
2.0000
27.212
el.448
201.77
1.780E-Ol
5.487E-02
4.123E-02
7.eSl3E-03
4.882E-02
3.0000
40.818
75.054
18!.20
1.2871-01
e.7551-02
2. e43E -02
1.435E-02
4.078E-02
5.0000
e8.030
102.288
121.24
7.888E-02
8.710E-02
1.332E-02
1.828E-02
3.2111E-02
8.0000
81.835
115.872
107.00
8.45!E-02
8.348E-02
1.011E-02
I.U7E-02
2.88U-02
7.0000
05.241
12 •. 478
.!.78
5.408E-02
5.8!3li-02
7.825E-0~
1 .• 22E-02
2.714';-02
18
GE IV
!5P
10'
1.21173E+00 (RYD)
N'·
3.5532
MU'
1.44118
E (RYD)
1
lEV)
~ PHOT (EV)
L"'MBD'"
1...1
(L/R/L-l)
(L/R/L+11
SIGM... L· 1
SIGM... L+l
SIGM... (MB)
.0000
.000
17.243
7111.05
Il.215E-Ol
-4.1185E-Ol
3.0117E-Ol
1.7115E-Ol
4.8112E-Ol
.2000
2.721
111.11114
1121.04
7.23I1E-Ol
-3.11I1E-Ol
2. 1111 E-01
8. 1311E-02
3.0015E-Ol
.11000
8.1114
215 .407
488 .01
4.8I1!5E-Ol
-1.200E-Ol
1.25I1E-Ol
1.533E-02
1.413E-Ol
.8000
10.8815
28. 128
440.80
4.113E-Ol
-Il. 8112E-02
Il. Il1111 ! - 02
5.51181-03
1. 0153E-Ol
1.0000
13.11011
30.8411
401.112
3.531E-01
-3.355E-02
8.057E-02
1.455E-03
8.203E-02
1.2000
111.327
33.570
31111.34
3.071E-Ol
-8.57111-03
8.1132E-02
1. 035E-04
Il.1I42E-02
1.4000
111.048
311.2111
341.114
2.700E-Ol
Il.318E-03
5.541E-02
1.320E-04
5.555E-02
1 .11000
21 . 71111
311.012
317.81
2.311I1E-Ol
2.228E-02
4.11111 E- 02
8.110E-04
4. 772E -02
1.8000
24.4111
41.734
287.011
2.143E-Ol
3. 171E -02
4.0151-02
1.758E-03
4.1111E-02
3.0000
40.818
58.0111
213.55
1.242E-Ol
5.272E-02
1.87I1E-02
8.7111E-03
2.5152E-02
4.0000
154.424
71. 11117
173.00
8.775E-02
5.332E-02
1.115I1E-02
8.153I1E-03
2.010E-02
15.0000
118.030
85.273
1415 .40
Il.5112E-02
5.030E-02
7.7111E-03
Il.037E-03
1.1180E-02
Il.0000
81 .1135
118.878
1215.311
5.111I1E-02
4. 1144E-02
5.535E-03
8.1135E-03
1.447E-02
GE IV
IIP
EO'
7. 117117E-Ol
(RYDI
N··
4.51144
MU·
1 .43158
E (RYD)
E (EV 1
E PHOT (EV)
L"'MBD'"
( ... )
(L/R/L-l)
(L/R/L+11
SIGM... L- 1
SIGM... L+ 1
SIGM... (Mil
.0000
.000
10.4411
11811.1511
1.518E+00
-1I.15112E-Ol
5.04I1E-Ol
4.003E-Ol
Il.049E-Ol
.15000
Il.803
17.2152
718.118
8.1I0IlE-Ol
-2.304E-Ol
1.578E-Ol
3.83I1E-02
1.1182E-Ol
1.0000
13.11011
24.0515
!l15.43
3.801E-Ol
-5. 455E -02
7.281E-02
2.III1I1E-03
7.581E-02
1.2000
18.327
211.778
4113.05
3.180E-Ol
-2.34I1E-02
5.870E-02
8.1112E-04
5.732E-02
1.4000
111.048
211.4117
420.33
2.708E-Ol
-2.5117E-03
4.523E-02
8. 144E-OII
4.524E-02
1 .11000
21 .71111
32.218
384.83
2.335E-Ol
1.180E-02
3.881E-02
1.87I1E-04
3.700E-02
1.8000
24.4111
34.840
354.811
2.040E-Ol
2.178E-02
3.045E-02
Il.1142E -04
3. 115E-02
2.0000
27.212
37.11$1
3211.22
1.800E-Ol
2.875E-02
2.55I1E-02
1.304E-03
2.118I1E-02
4.0000
54.424
84.873
181.12
7.2118E-02
4.15I1E-02
7.17I1E-03
4.701E-03
1.188E-02
!I.OOOO
118.030
78.4711
157.1111
5.211I1E-02
3.85I1E-02
4.811 E- 03
4.8117E-03
t. 508E -03
Il.0000
81 .1135
112.084
134.114
4.0113E-02
3.515E-02
3.185E-03
4.7115E-03
7.1150E-03
Gi
IV
8P
EO' 3.70341-01
(IIYDl
N'·
Il.5730
MU'
1.4270
E 1IIYO)
E 1EV)
E PHOT 1EV)
l. ...MBD ... ( ... )
(L/R/L-l)
IL/R/L+l)
SIGM... L- 1
SI01Il... L+ 1
SIGM... (MB 1
.0000
.000
5.0311
24110.114
3.0115E+00
-2.212E+00
1.011 E-00
1 . 033E +00
2.044E+00
.5000
Il.803
11.842
1047.03
7.44I1E-Ol
-2.1138E-Ol
1.37eE-Ol
•. 283E-02
1.805E-Ol
1.0000
13.11011
18.11415
'11504 .1111
3.482E-Ol
-1I.2115E-02
•. 735E-02
3.08I1E-03
5.042E-02
1.2000
111.327
21.31111
580.30
2.770E-Ol
-3. 003E -02
3.435E-02
8.072E-04
3.515E-02
1.4000
111.048
24.087
514.74
2.2115E-Ol
-Il. 850E-03
2.588E-02
9.3117E-05
2.588E-02
1.11000
21.7118
211.808
4112.411
1.8112E-Ol
3. 4113E -03
2.010E-02
1.370E-05
2.012E-02
1.8000
24.4111
211.15211
.'11.87
1.808E-Ol
1.215E-02
1 .1I00E -02
1.825E-04
1.1118E-02
3.0000
40.818
45.857
270.38
7.673E-02
2.753E-02
5.1155E-03
1.45I1E-03
7. 1 IlE - 03
4.0000
54.42.
58:4112
208.51
4.1180E-02
2.701E-02
3.0114E-03
1.817E-03
4.881E-03
5.0000
118.030
73.0es
11111 . 1111
3.512E-02
2.4115E-02
1.888E-03
1 . 8511E- 03
3.747E-03
Il.0000
81 .1135
811.1174
143.05
2.641 E-02
2.214E-02
1. 2118E -03
1.780E-03
3.04I1E-03
7.0000
115.241
100.280
123.114
2.072E-02
1.1188E-02
Il.015E-04
1 .11111 E- 03
2.5113E-03
GE IV
10P
EO'
2 . 1754 E- 01 . 1RYD )
N"
8.5781
MU'
1.42311
E IRYD)
E (EV)
E PHOT CEV)
L"'MBD'"
( ... )
(L/R/L-l)
(l./R/L+l)
SIGM... L- 1
SIGM... L~1
SIGM... (MBI
.0000
.000
2.1180
4188.1111
5.157E+00
-3.8113E+00
r , 11411E -00
1.880E-00
3.52I1E-00
.2000
2.721
5.1181
2182.47
1.73I1E-00
-1.022E+00
3.511I1E-Ol
2.487E-Ol
Il.08I1E-Ol
.4000
5.442
8.402
1475.114
9.037E-Ol
-4.1113E-Ol
1.437E-Ol
8.188E-02
2. 058E -0 1
.8000
10.885
13.845
8815.58
3.1I08E-Ol
-1.0114E-Ol
4.430E-02
8.571E-03
5.0B7E-02
1.0000
13.11011
111.51111
748.45
2.8110E-Ol
-5.575E-02
2.811I1E-02
2.157E-03
3.114E-02
1.4000
111.048
22.008
5113.37
1.7111 E-01
-II. 7711E-03
1.47I1E-02
8.817E-05
1.488E-02
1.8000
21 . 71111
2•. 728
501.37
1.472E-Ol
Il.'74E-04
1.122E-02
1.031 E-08
1.122E-02
1.8000
24.4111
27.450
451.117
1.234E-Ol
7.1I07E-03
8.758E-03
7.1110E-05
8.830E-03
2.0000
27.212
30.172
410.114
1.052E-Ol
1.240E-02
8.1188E-03
1.1145E-04
7.1112E-03
3.0000
40.818
43.778
283.22
!5.817E-02
1 .1I5!1E -02
2.8113E-03
7.011E-04
3.5114E-03
4.0000
5 •. 424
57.383
2111.07
3 .5111 E- 02
1 .1I02E -02
1 .5241-03
8.11114E-04
2.3113E-03
5.0000
B8.030
70.11811
174.115
2.490E-02
1. 722E -02
Il.222E-04
8.814E-04
1.8041-03
Il.0000
81 .1135
U.5115
1411.511
1.857E-02
1.538E-02
8.10IlE-04
8.382E-04
1.44I1E-03
GE IV
12P
EO'
1.4300E-Ol
IRYD)
N·· 10.5777
MU'
t.4223
E (IIYD)
E 1 EV)
E PHOT (EV)
L"'MBD'"
( ... )
(L/A/L-l)
IL/II/L+I)
SIG"'''' L- 1
SIQ/lI... l.+1
SIGM... (MB)
.0000
.000
1.1148
11372.44
7.883E+00
-5.1178E+00
2.40IlE+00
2.1113E-00
5.318E+00
.1000
1.381
3.308
3750.05
3.174E+00
-2.14111+00
6.'78E-Ol
8.3118E-Ol
1.338E+00
.4000
5.442
7.388
11178.21
8.2115E-Ol
-3.'00E-01
1.057E-Ol
•. 70IlE-02
1.528E-Ol
.11000
8.184
10.109
12211.47
4.881E-Ol
- 1. 7118E-0 1
5.045E-02
1. 31111E - 02
8.4141-02
.8000
10.885
12.830
111111.35
3.211I1E-Ol
-1I.108E-02
2.871E-02
4.45I1E-03
3.317E-02
1.0000
13. 110 Il
15.552
717.211
2.3114E-Ol
-4.702E-02
1.820E-02
1. 440E - 03
1.1184E-02
1.4000
".048
20.11114
590.58
1.425E-Ol
-8. 5UE -03
8.1130E-03
Il.4I2E-05
8.11115E-03
1.11000
21 . 71111
23.715
522.82
r , 1110E -0 1
1.435E-04
Il.1I84E-03
2.047E-08
Il.1I84E-03
1.8000
24.4111
211.4311
4811.00
Il. 85SE -02
5.11113E-03
5.183E-03
3.552E-05
5.1118E-03
2.0000
27.212
211. 157
425.23
8. 183E-02
Il. 205E -03
4.01l0E-03
1.035E-04
4. Ill3E -03
4.0000
54.424
511.31111
2111.115
2.1I'IIE-02
1. 423E -02
8.538E-04
4.782E-04
1.332E-03
5.0000
88.030
1111.1175
177. III
1.811I1E-02
1. 283E -02
5.118E-04
•. 828E-04
Il. 114 liE -04
Il.0000
8 1 . 1135
83.581
148.34
1 .3871 -02
1. 143E-02
3.38I1E-0.
4.572E-04
7.1141 E-04
GE IV
ll1P
EO'
7.5277E-02
(RYD)
If·· 14.57110
MU'
1.4210
E (AYD)
E (EV)
E PHOt
(EV)
l. ...MBD ... ( ... )
(LiR/L-1I
IL/R/L+l)
SIQ/lI... L- 1
SIQ/lI... L-1
SIGM... (Mil)
.0000
. 000
1.02.
12105.55
1.408E+Ol
-1.130E+Ol
4.242E+00
5.475E+00
Il.717E+00
.1000
1.381
2.385
511111.02
3.432E-00
-2.3115E+00
5.884E-Ol
5.588E-Ol
1.147E+00
.4000
5.442
Il.4117
11117.34
Il.44I1E-Ol
-3.08I1E-Ol
5.1133E-02
2.57I1E-02
8.213E-02
.11000
8.18.
Il.188
13411.47
3.572E-Ol
-1.33I1E-Ol
2. 4511E -02
8.873E-03
3. 143E -02
1.0000
13.11011
14.1130
847.47
1 .1I30E -0 1
-3.328E-02
8. 1411E-03
6.787E-04
8.825E-03
1.4000
111.048
20.072
817.1111
Il.5!1I1E-02
-1I.231E-03
3.83I1E-03
3.2115E-05
3.872E-03
1 .11000
21.71111
22.7114
!l43.115
7.708E-02
-2.833E-04
2.837E-03
7.11112E-08
2.837E-03
1.8000
24.4111
25.515
485.'4
Il.311I1E-02
3.425E-03
2.1118E-03
1. 254E -05
2. 181 E-03
3.0000
40.818
41.842
21111.32
2. 75llE -02
Il.332E-03
6.1171E-04
1.528E-04
8.1118E-04
•. 0000
54.424
55.448
223.111
1.715E-02
8.11115E-03
3.41I1E-04
1. 880E -04
5.2115E-04
5.0000
118.030
1111.054
1711 . 55
1 . 185E -02
8.082E-03
2.030E-04
1.888E-04
3.1120E-04
8.0000
81.1135
82.1180
150.00
8.780E-03
7. 177E -03
1.32I1E-04
1.783E-04
3.112E-04
lia
GE IV
20P
EO' 4.8350E-02
IRYD)
N.· 18.5788
MU'
1.4204
E IAYD)
E lEV)
E PHOT (EV 1
LAMBDA
(A)
(L/A/L-O
(L/A/L-l )
SIGMA L-l
SIGMA L-l
SICMA 1MB)
.0000
.000
.831
18880.77
2.213E-Ol
-1.808E-Ol
Il.471E+00
8.1133E-00
I.510E-Ol
.1000
1 .3111
1.181
8228.115
3.247E-00
-2.252E-00
4. 38eE-0 1
4.230E-Ol
8.1128E-Ol
.2000
2.721
3.352
3888.08
1.357E-00
-8.283E-Ol
1.283E-Ol
8.1135E-02
2.25H-Ol
.4000
!5.442
1.073
2041 .80
!5.003E-Ol
-2.407E-Ol
3.18!5E-02
1.473E-02
4 .8!58E -02
.8000
8. 184
8.784
1408.87
2.882E-Ol
-1.010E-Ol
1.3281;-02
3.7!58E-03
1.701E-02
.8000
10.185
1 1 . !51!5
1078.70
1.703E-Ol
-4. 873E -02
8.883E-03
1.148E-03
8.138E-03
1.0000
13.808
14.237
870.80
1.180E-Ol
-2.4!55E-02
4.225E-03
3.585E-04
4.!584E-03
1.4000
18.048
18.879
830.0!5
Il.88I1E-02
-4. 1I40E - 03
1 . 854E -03
1.775E-05
1. 872E -03
1 .8000
21.788
22.400
!5!53.51
5.533E-02
-3. 185E-04
1 . 4311E-03
8.403E-08
r , 438E -03
1.8000
24.481
2!5. 121
483.!5!5
4.555E-02
2.3111E-03
1.0821-03
5.885E-08
1.088E-03
2.0000
27.212
27.842
44!5.31
3.828E-02
4.041E-03
8.548E-04
1 .804 E-05
8.738E-04
3.0000
40.818
41.448
288.13
1.854E-02
Il.!5112E-03
3.318E-04
7.478E-05
4.063E-04
4.0000
!54.424
55.0!54
225.21
I.208E-02
8.318E-03
1.883E-04
.8.208E-05
2.804E-04
5.0000
88.030
88.880
180.!58
8.3331-03
5. 884E -03
8.88eE-05
8.227E-05
1.821 E-04
8.0000
81.1135
82.288
150.71
Il.147E-03
5.028E-03
Il.511 E-05
8.708E-05
1.522E-04
GE IV
4D
EO'
1. !5837E-00 (AYD)
N.· 3. 1885
MU'
.8315
E ( AYD)
E (EV)
E PHOT (EV 1
LAMIDA 110)
(L/A/L-l)
(L/A/L+I)
SIGMA L- 1
SIGMA L-l
SIGMA (MBI
.0000
.000
21.883
571. 10
3.272E-Ol
-3.288E-Ol
5.838E-02
8.734E-02
1.4!57E-Ol
.2000
2.721
24.405
!508.04
2.733E-Ol
-1.557E-Ol
4.583E-02
2.23lE-02
8.815E-02
.4000
!5.442
27.128
457.08
2.328E-Ol
-4.833E-02
3.888E-02
2. 18U -03
3.818E-02
.!5000
0.803
28.488
435.25
2.183E-Ol
-8. 788E -03
3.3!lOE-02
4.8150E-05
3.3515E-02
.8000
8. 184
28.847
411S.41
2.0181-01
2.538E-02
3.04U-02
7.21581-04
3.122E-02
.7000
8.!524
31.208
387.30
1.88!5E-Ol
5. 188E-02
2.787E-02
3.1421-03
3. 101 E- 02
.8000
12.245
33.828
3815.43
1.1582E-Ol
8.08!5E-02
2.3!58E-02
1 . 01S8E- 02
3.411E-02
1.0000
13.8015
3!5.288
351. 34
1.588E-Ol
1 . 0!53E -0 1
2.178E-02
1.4771-02
3.1553E-02
3.0000
40.818
82.!501
188.37
Il.1I20E-02
1. !58.E-0 1
Il.885E-03
!l.8015E-02
8.483E-02
4.0000
!54.424
711.107
112.8\\
4.814E-02
I.433E-0\\
4.81U-03
!5.183E-02
Il.354E-02
!5.0000
88.030
88.713
138.20
3.8281-02
1 . 288E -0 1
3.304E-03
!I. 588E - 02
!5.828E-02
CI
IV
50
EO' 8.132U-Ol
IAYD)
N.· 4.18515
MU'
.8144
E (AYD)
E (EV)
E PHOT 1 EV1
LAMBDA
lA 1
(L/A/L-l)
(L/A/L-l)
SIGMA L- 1
SIGMA L-l
SIGMA IMBI
.0000
.000
12.428
887.78
!l.7301-01
-1.021E-00
1. 028E-0 1
4.180E-Ol
5.80I5E-Ol
.2000
2.721
15.147
818.54
4.2121-01
-!l.:I821-Ol
B.7581-02
1.15150E-Ol
2.3381-01
.4000
5.442
17.888
813.88
3.283E-Ol
-2.7821-01
4.784E-02
5.2531-02
1.004E-Ol
.7000
8.524
21.850
!l84.85
2.377E-Ol
-7.738E-02
3.118E-02
4.853E-03
3.814E-02
.8000
10.885
23.311
531.88
2.1871-01
-3.700E-02
2.7!l21-02
1.203E-03
2.872E-02
.8000
12.245
24.871
502.55
1. 888E-0 1
-4.873E-03
2. 4481 -02
·2.30lE-0!l
2.448E-02
1.0000
13.808
28.032
478.28
1.8281-01
2.058E-02
2.188E-02
4.157E-04
2.230E-02
2.0000
27.212
38.838
312.80
8.583E-02
1.12U-Ol
8. 11 II- 03
1.80!lE-02
2.818E-02
3.0000
40.818
!l3.244
232.87
15.0531-02
1.1815E-Ol
4.804E-03
2.722E-02
3.213E-02
4.0000
54.424
88.850
185.47
4.248E-02
1.081E-Ol
3.032E-03
2.838E-02
3.140E-02
!l.0000
88.030
80.458
154\\.11
3. 18lE-02
8.4UE-02
2.0471-03
2. 887E -02
2.801E-02
8.0000
108.847
121. :::73
102.24
1.873E-02
8.838E-02
8.530E-04
2.0151-02
2.100E-02
GE IV
8D
10' 5.8351E-Ol
(AYD)
H·· !l.11121
MU'
.8078
E ( AYD)
1
(EV)
E PHOT (EV)
LAMBDA
(A)
(L/A/L-l)
(L/A/L-l )
SIGMA L- 1
SIGMA L-l
SIOMA (MBI
.0000
.000
8.075
1!l35.38
8.804E-Ol
-1.885E-00
1.503E-Ol
1.0581-00
1 . 208E -00
.2000
2.721
10.7811
1148.40
5.483E-Ol
-8.8041-01
8.088E-02
3. 155E -0 1
3.885E-OI
.5000
8.803
14.878
833.34
3.321E-Ol
-3.1!l21-Ol
4.124E-02
5.!573E-02
8.887E-02
.8000
10.885
18.880
8!l3.84
2.2811-01
-8.711E-02
2.480E-02
8.741E-03
3.154E-02
.9000
12.245
20.321
1I10.1!l
2.048E-Ol
-!l.803E-02
2.144E-02
2.40!l1-03
2.385E-02
1.0000
13.11011
21.881
571.81
1.8!l3E-Ol
-2.4141-02
1.871E-02
4.782E-04
1.819E-02
:.0000
27.212
35.287
351.311
8.882E-02
8.411E-02
8.888E-03
8.4131-03
1.810E-02
3.0000
40.818
41.883
253.!l8
!l.208E-02
8.U21-02
3.333E-03
1.4801-02
I.824E-02
4.0000
54.424
82.488
188.38
3.538E-02
8.1731-02
1.8811-03
1.!l14I-02
1.771E-02
!l.0000
88.030
78. 105
182.82
2.!582E-02
7.218E-02
1.2851-03
1.4851-02
1.8241-02
Il.0000
81.83!l
88.711
138.21
1. U8i-02
Il.3511-02
8.0001-04
1.388E-02
1.458E-02
8.0000
122.4153
130.528
84.88
1.102E-02
4.4751-02
3.882E-04
8.858E-03
1.025E-02
GE IV
80
EO' 3. 0887E-0 1 (AYDI
N.· 7.1874
MU'
.8028
E (AYD)
E (EV)
E PHOT (EV 1
LAM8DA
(A)
(L/A/L-I)
(L/A/L-O
SIGMA L- 1
SIGMA L-l
SIGMA (MB)
.0000
.000
4.202
2850.34
1 . 540E -00
-3.8821-00
2.5081-01
2.512E-00
2.7831-00
.2000
2.721
Il.824
1780.77
7.041E-Ol
-1.3801+00
8.827E-02
4.825E-Ol
5.888E-Ol
.8000
8. 184
12.368
1002.84
2.858E-Ol
-2.854E-Ol
2.542E-02
3.787E-02
8.338E-02
1.0000
13.808
17.808
898.23
1.821E-Ol
-5.4401-02
1.178E-02
1.8871-03
1.375E-02
1.2000
18.327
20.530
1103.84
1.288E-Ol
-8.288E-03
8.88U-03
5.317E-05
8.752E-03
1.4000
18.048
23.251
!l33.211
1.088E-Ol
1.82lE-02
Il.873E-03
3.234E-04
8.888E-03
1 . 8000
21 . 788
25.872
477.38
8.882E-02
3.5118E-02
5.287E-03
1.288E-03
8.538E-03
3.0000
40.818
45.020
275.40
3.7881i:02
!l.872E-02
1.807E-03
5.8521-03
7.480E-03
4.0000
54.424
58.828
211.411
2.4781-02
!l.32lE-02
Il.0381-04
8.258E-03
7.18lE-03
5.0000
88.030
72.232
171.85
1.775E-02
4.888E-02
5.7181-04
5.834E-03
8.508E-03
GE IV
100
EO'
1.88081-01
(RYD)
H.· 8.1884
MU'
.8008
E ( RYC)
1
(IV)
E PHOT (EV)
LAMBDA
(A)
(L/A/L-O
(L/A/L-l )
SIGMA L- 1
SIGMA L-l
SIGMA 1MB)
.0000
.000
2.572
4818.88
2.34lE-00
-1I.838E-00
3.544E-Ol
4.27!lE+00
4.830E+00
.2000
2.721
5.284
2342.23
7.558E-Ol
-1.577E-00
7.800E-02
4.8871-01
5.727E-Ol
.8000
8.184
10.738
11!l4.88
2.523E-Ol
-2.788E-Ol
1.718E-02
3.10lE-02
4.819E-02
.8000
10.885
13.457
1121.35
1.775E-Ol
-1.300E-Ol
1.01l1lE-02
8.580E-03
1.8241-02
1.0000
13.808
111.178
7lll1.38
1.3321-01
-5.!l811-02
7.215E-03
1.800E-03
8. 11 5E - 03
1.2000
18.327
18.888
1158.03
1.0441-01
-1.48U-02
5.1821-03
1.800E-04
5.342E-03
t.4000
18.048
21 .821
573.48
8.4157E-02
8.1584E-03
3.887E-03
8.147E-05
3.84\\8E-03
1.15000
21 . 788
24.342
508.38
7.018E-02
2.2UE-02
3.014E-03
4.78U-04
3.483E-03
2.0000
27.212
28.784
418.28
5.1041-02
3.8811-02
1 .851 E-03
1.5051-03
3.455E-03
3.0000
40.818
43.380
285.75
2.8081-02
4.1821-02
8.804E-04
2.882E-03
3.722E-03
4.0000
54.424
58.988
217.54
1. 8:17E -02
3.783E-02
4.728E-04
3. 07lSE -03
3.548E-03
!l.0000
88.030
70.802
175.151
1.288E-02
3.308E-02
2.848E-04
2.814E-03
3.208E-03
20
GE IV
120
EO'
1.2754E-Ol
(AYD>
N.· 11.2004
MU'
.7111UI
E (AYDI
1
(EVI
E PHOT (EV)
lAMIDA
(A)
(l/A/l-l)
(l/A/l-l)
SIGMA l-l
SIGMA l-1
SIGMA
(MIS)
.0000
.000
1.735
7144.811
3.248E+00
-1I.80IlE+00
4.803E-Ol
8.2115E+00
8.75I1E+00
.2000
2.721
4.4511
2782.15
7.427E-Ol
-1.818E-00
8.178E-02
4.40lE-Ol
5.01U-Ol
.4000
5.442
7.178
1727.311
3.550E-Ol
-5.1174E-Ol
2.274E-02
8.7131-02
1. OIlIlE-O 1
.8000
8.184
Il.81111
1252.53
2.157E-Ol
-2,477E-Ol
·1.157E-02
2.2110E-02
3.447E-02
.8000
10.885
12.820
1182.48
1.478E-Ol
-1.1501-01
8.1131E-03
8.2111 E- 03
1.322E-02
1.0000
13.1108
15.341
808. III
1.01l0E-Ol
-5.025E-02
4.580E-03
1.481E-03
8.040E-03
1.2000
18.327
18.0112
1188.43
8.43I1E-02
- 1. 5411E -02
3.233E-03
1 . 835E -04
3.3117E-03
1,4000
111.048
20.784
5118.511
8. ?tIIlE-02
4. 3311E -03
2. 3114E -03
1.475E-05
2.40IlE-03
1.8000
2 1 . 71111
23.5015
527.411
5.577E-02
1 . 804E -02
1.837E-03
2.280E-04
2.0118E-03
2.0000
27.212
28.1147
428.32
4.012E-02
2.731E-02
1 . 171 E -03
8.1401-04
1.1185E-03
3.0000
40.818
42.553
291.37
2.17d-02
3.181E-02
5.055E-04
1.804E-03
2.10IlE-03
".0000
54.424
58. 1511
220.78
, .3115E-02
2.857E-02
2. 748E -0"
1.72I1E-03
2.003E-03
5.0000
88.030
811. 715
177.72
Il.842E-03
2.4114E-02
1 . 81111E -04
1.837E-03
1.807E-.03
7.0000
1115.241
118.1177
127.815
15. 788E-03
1.1I05E-02
8. 188E-05
1.327E-03
1. 40llE -~3
GE IV
t8D
EO-
8.1123111-02
( A.YDI
N··
15.2014
MU'
.71186
E (AYDI
E (EV 1
E PHOT 1IV)
lAMIDA
(A 1
(l/A/l-l )
(l/A/l-l)
SIGMA
l-1
SIGMA l+l
SIGMA
(MI)
.0000
.000
.1142
13181.11
5.348E+00
-1.781E+Ol
8.7881-01
1. 101 E+O 1
1.18I1E+Ol
.1000
1.381
2.303
5384.411
1.317E+00
-3.581E-00
1.004E-Ol
1.101 E-OO
1.201E+00
.2000
2.721
3.883
3384.80
8."23E-Ol
-1.484E+00
3.7118E-02
2.1I110E-Ol
3.33I1E-Ol
.4000
5.442
8.384
11142.01
2.72d-Ol
-4.523E-Ol
1.1111E-02
4.1125E-02
8.115E-02
.8000
8.184
Il. 108
13111.85
1.5721-01
-1.882E-Ol
5.853E-03
1 .2181 -02
1.78lE-02
.8000
10.885
11.827
1048.35
1.048E-Ol
-8.588E-02
3.255E-03
3.28111-03
8.543E-03
1.0000
13.808
14.548
8152.28
7.573E-02
-3.7111E-02
2.0117E-03
7.885E-04
2.888E-03
1.2000
111.327
17.2811
717.118
5.788E-02
- 1 .280E-02
1.454E-03
1. 01l8E -04
1 .1511 1E- 03
1.4000
111.0411
111.11110
&20.23
4.5118E-02
1.283E-03
1 . 082E -03
1.240E-08
1.0113E-03
1.8000
21.7811
22.712
545.112
3.780E-02
Il ... 711E- 03
8. 0811E -04
7.1114E-05
8.83I1E-04
2.0000
27.212
21.154
440.311
2.87,IlE-02
1,730E-02
5.0117E-04
3.178E-04
1.243E-04
3.0000
40.818
"'.780
2118.110
1 . 428E-02
2.02U-02
2.140E-04
8. 485E -04
8.824E-04
4.0000
5".42"
55.3118
223.114
Il.084E-03
1.832E-02
1.148E-04
7.00IlE-04
1.158E-04
5.0000
118.030
88.1172
1711.78
8.37I1E-03
1.5117E-02
7.054E-05
1.831E-04
7.337E-04
GE IV
200
EO· 4.331115E-02 {AYD)
N·· 111.2018
MU'
.71182
E (AYD)
E (EV)
PHOT leV)
lAMIDA
(A)
( l/A/l-O
1l/A/l+ 1 )
SIGMA
l - 1
SlaMA
l+1
SIGMA
(MI)
.0000
.000
.5110
20111111.58
7. 7815E+00
-2.7211E+Ol
8.111115E-Ol
1.15155E+Ol
1,745E+Ol
.0500
.880
1. 271
11757,18
2.332E+00
-7.224E+00
1.738E-Ol
2.500E+00
2.874E+00
.1000
1.381
1 .1I5!
835... 117
1.200E+00
-3.347E+00
7.080E-02
8.242E-Ol
8.1148E-Ol
.2000
2.721
3.312
3743.1111
5.308E-Ol
- 1 .238E+00
2. 3"5E - 02
1.1I0IlE-Ol
2.143E-Ol
.4000
5.442
8.033
2055.21
2.105E-Ol
-3.557E-Ol
Il.718E-03
2.877E-02
3.54I1E-02
.1000
8.184
8.754
''''8.34
1.183E-Ol
-1.4"3E-Ol
3.07I1E-03
8.870E-03
Il.114I1E-03
.8000
10.885
Il.4·75
1080.48
7.788E-02
-8.51I1E-02
1 . 7"0E -03
1.83llE-03
3.578E-03
i"- C' 0000
13.808
14,1118
873.37
5.570E-02
- 2. U5E -02
1.107E-03
4.458E-04
1 . 553E - 03
1.0000
13.1108
14. 11111
873.37
5.515I1E-02
-2.888E-02
1,107E-03
".4117E-04
1.5153E-03
1.2000
18.327
18.1118
732.811
4.230E-02
-1.005E-02
7. 808E -04
8.447E-05
8.253E-0"
1 .4000
111.048
19.1139
831.34
3.345E-02
".152E-04
5.524E-04
1.278E-07
5.525E-0"
1.8000
21 .7811
22.380
55".50
2.728E-02
8."54E-03
4.181E-0"
3.512E-05
4.533E-0"
2.0000
27.212
27.802
445.118
1 .1131 E-02
1.218E-02
2. 805E -0"
1.558E-0"
".182E-0"
3.0000
40.818
.. 1. "08
21111.42
1 . 02d -02
1. "38E-02
1 . 0111 E-04
3.227E-0"
4.318E-04
4.0000
54.424
55.014
225.37
8.48151-03
1 . 2QIII -02
5.815E-05
3.501E-04
".0831-04
5.0000
88.030
88.820
110.811
".54I5E-03
1.1311-02
3. 5114E -015
3.3081-04
3.8841-0"
GE IV
4F
ID'
1.004I1E+00 {AYD)
N··
3.111102
MU'
.00118
E (RYDI
E lEV 1
E PHOT «EV 1
lAfIItlDA lA)
(l/A/l-l )
Il/R/l-l)
SIGMA L - 1
SIGMA L-l
SIGMA
1Mtll
.0000
.000
13.873
1I01l.82
Il.514E-02
1 .812E+00
3.333E-03
1.278E-00
1.27I1E+00
1.0000
13.1108
27.279
4154.52
3.534E-02
3. 030E-0 1
Il.175E-0''
8.11112E-02
Il.084E-02
2.0000
27.212
40.88"
303.28
1.758E-02
t . 01l7E-0 1
3."03E-04
t . ?tlllE-02
1.800E-02
3.0000
40.818
54.4110
227.5 ..
1 .0121 -02
5.211I1E-02
1. 503E -04
5."1I4E-03
5 . 11451 - 03
",0000
15".424
88. 011 li
182.08
8.380E-03
3.020E-02
7.485E-05
2.231E-03
2.305E-03
GE IV
5F
EO'
8.4371E-Ol
(AYD)
N'"
".11858
MU'
. 01 ....
E IAYD>
E (EV l
E PHOT (EV)
LAMIDA (A)
(l/A/l-l)
(UA/l-l)
SIGMA
l - \\
SI GlllA l+1
SIGMA
(MB)
.0000
.000
8.758
1415.88
1.713E-Ol
2.1125E+OO
8.1122E-03
2.8110E+00
2.8117E+00
.4000
5."42
14.201
873.11
Il.2941-02
1.05I1E+00
3.303E-03
5.713E-Ol
5.747E-01
1.0000
13.808
22.384
5114 .40
4.77I1E-02
3.81111-01
1 . 375E -03
1.17lE-Ol
1. 185E-0 1
2.0000
27.212
35.1170
344.1111
2.140E-02
1.244E-Ol
4.434E-04
1.IIIIIE-02
2.043E-02
3.0000
40.818
411.578
250.01l
1.11115E-02
5.714E-02
1.813E-0"
5.812E-03
5.11114E-03
4.0000
154.42"
83.182
11111.2"
7.102E-03
3.1112E-02
8 . 582 E- 05
2.288E-03
2.354E-03
GE IV
IF
EO' 4.411117E-Ol
(AYD>
N'"
5.11830
MU'
.0170
E UYD)
E (EV)
E PHOT (EV)
lAMIDA
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2.0000
27.2t2
41l.240
21l8.14
i , 118E-0 1
1.320E-Ol
1.453E-02
3.03IlE-02
4.4ll0E-02
3.0000
40.818
5ll.841l
207. 18
7. 31l4E - 02
1.318E-Ol
8.157E-03
3.ll17E-02
4.733E-02
4.0000
54.424
73.4152
11l8.80
5.277E-02
1.202E-Ol
5. 142E-03
4.001E-02
4.51I1E-02
Il.0000
118.030
87.058
142.42
3.lIllllE-02
1.073E-Ol
3. 4llllE -03
3.180E-02
4.130E-02
AS V
110
EO- Il.1214E-Ol
(RYO)
N'"
5.2353
MU'
.71l47
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L·I)
SIGMA L- 1
SIGMA L+ 1
SIGMA (Mil)
.0000
.000
12.411
lllll.04
7.17llE-Ol
-8.3llIlE-OI
1.1l0BE-Ol
3.2ll8E-Ol
4.ll0IlE-Ol
.4000
5.442
17.853
11ll4.4ll
3.ll8IlE-Ol
-2.2ll2E-Ol
7. 12llE-02
3.537E-02
1.01l7E-Ol
.1l000
8. 1114
20.514
1l02.1l3
3.1IlllE-Ol
- 1 .031 E-01
5.1.4E-02
8.247E-03
Il.01llE-02
.7000
Il.524
21 .ll35
51l1l.25
2.8158E-Ol
-5.llUE-02
4.502E-02
2 .•IlH -03
4.7•• E-02
.8000
10.885
23.2llll
1132.24
2.5ll3E-Ol
-2.571E-02
3 . 113 liE -02
5. 80H -04
3 .1l114E -02
.llOOO
12.245
24. IlIlIl
502.87
2.3UE-Ol
1.513E-03
3. 41l7E -02
2.128E-01l
3.41l7E-02
1.0000
13.1l01l
21l.011l
471l.57
2. 11l8E - 01
2.332E-02
3.075E-02
5.333E-04
3.128E-02
2.0000
21.212
311.1l22
312.ll2
\\ . OllllE - 01
1.028E-Ol
1.lll5E-02
1.57llE-02
2. 774E -02
3.0000
40.818
53.228
232.ll3
Il.71l1E-02
1.05I1E-Ol
Il.11I1E-03
2.233E-02
2.844E·02
4.0000
54.424
1l1l.834
185.51
4.1l51E-02
Il.570E-02
3.1l3I1E-03
2.308E-02
2.1112E-02
5.0000
1l8.030
80.440
154.13
3.42IlE-02
8.41l7E-02
2.374E-03
2.174E-02
2.412E-02
8.0000
108.847
121.258
102.211
1.735E-02
5.87llE-02
Il,177E-04
1.580E-02
1.1l72E-02
AS V
80
EO'
4.7880E-Ol
(RYO)
N··
7.2411
MU'
.75811
E (RYOI
E (EV)
E PHOT (EV)
LAMBDA
tAI
(L/R/L-l)
( L/R/L+I')
SIGMA L- 1
SIGMA L+l
S ICMA
(Mill
.0000
.000
Il.487
1ll1'.22
1.334E+00
-2.007E+00
2.903E-Ol
Il.8117E-Ol
1.271lE+00
.2000
2.721
Il.208
1341l.44
7.558E-OI
-8.U1E-Ol
1.322E-Ol
2.lIll8E-Ol
3,ll21E-Ol
.4000
5.442
11.1130
10311.31
4.ll11E-Ol
-4.11l8E-Ol
7.40IlE-02
7.815E-02
1.522E-Ol
.1l000
8. 184
14.851
848.27
3.1I1l4E-Ol
-2.03IlE-Ol
4.1l7llE-02
2.2110E-02
Il.llIl8E-02
.8000
10.885
17.372
713.71
2.704 E-0 1
-lI.boIlE-02
3.1ll4E-02
5.312E-03
3. 72!5E -02
.1000
12.245
18.733
1l1l1 .87
2.3ll3E-Ol
-1I.33lE-02
2.IlIlIlE-02
2.001E-03
2.8ll7E-02
1.0000
13.1l01l
20.0ll3
1I17.01l
2.135E-Ol
-2.513E-02
2.303E-02
4. 7815E-04
2.351E-02
2.0000
27.212
33.llllll
31l7.ll2
Il. 183E -02
Il.745E-02
7.144E-03
5.781E-03
1 .,2112E - 02
3.0000
40.818
47.305
21l2. 10
5.255E-02
1. 173E-02
3.28.. E-03
Il.17IlE-03
1.24IlE-02
4.0000
54.424
110 .lll 1
203.1111
3. 457E -02
Il.41l0E-02
1.830&-03
Il.1I811&-03
1.142E-02
5.0000
1l8.030
74.1517
11l1l.3ll
2.412E-02
Il.1l5I1E-02
1.14I1E-03
8.118IlE-03
1.013E-02
Il.0000
81.11311
88.123
140.10
1.8118E-02
4.ll41E-02
1.731E-04
8.112E-03
8.8815E-03
AS V
100
EO'
2.ll2110E-Ol
(RYDI
N.·
Il.2433
MU'
.1111l7
E CRYO)
E lEV)
E PHOT (EV)
LAMllOA
(A)
(l./R/L-l )
(L/R/L-ll
SIGMA L- 1
SIGMA L+ 1
SIGMA (MB1
.0000
.000
3.ll81
3114.33
2.08llE+00
-3.1I02E+00
4.3IlllE-Ol
1.841E+00
2.278E+00
.2000
2.721
Il.702
184ll.ll0
8.ll75E-Ol
- 1 . 141lE+00
1.3117E-Ol
3.321E-Ol
4.1118E-Ol
.4000
5.442
Il.424
1315.71
Il.173E-Ol
-4.ll24E-Ol
Il.3311&-02
8.1l13E-02
1.411I5E-Ol
.11000
8. 1114
12.1411
1020.ll1
3.432E-Ol
-2.312E-Ol
3 .lIlll5E -02
2.447E-02
Il.042E-02
.8000
10.885
14.81l11
834.03
2.473E-Ol
- 1 . 0111 E- 0 1
2. 281lE-02
Il.305E-03
2.ll15E-02
1.0000
13.801l
17 .587
704.llll
1.882E-Ol
-3.1141E-02
1.58IlE-02
1.030E-03
1.1l1l8E-02
1.2000
111.327
20.308
1l10.52
1. 48llE -0 1
-1.44.E-03
1.131E-02
1 .807E -Oll
1.131E-02
1.4000
Ill.048
23.0211
153'.38
1.212E-Ol
2.107E-02
8.1510E-03
3.8113E-04
8.8llIlE-03
1.1l000
21.711ll
211.751
481 .4ll
1.010E-Ol
3.474E-02
Il.1l03E-03
1.172E-03
7.7715E-03
3.0000
40.818
44.7llll
271l.71l
4.057E-02
5.2UE-02
1.8114E-03
4.15ll3E-03
Il. 44111-03
4.0000
154.424
58.4015
212.2ll
2.1l1lE-02
4.1l77E-02
1.001 E-03
4.817E-03
5.818E-03
5.0000
1l8.030
72.011
172. "
1.840E-02
4.072E-02
Il.127E-04
4.502E-03
5.115E-03
AS V
120
EO-
l.ll772E~01 (RYD)
N·· 11.2445
MU'
.7555
E (RYDI
E (EV)
E PHOT (EV)
LAMBDA
(A 1
(L/R/L-l1
(L/R/L+I)
SIGMA L-l
SIGMA L+l
SIGMA (MB)
.0000
.000
2.llll0
41l08.77
2.ll72E+00
-15.30IlE+00
5.1172E-Ol
2.85IlE+00
3.453E+00
.2000
2.721
Il.411
22ll1.20
Il.157lE-Ol
- 1. 293E+00
1.248E-Ol
3.412E-Ol
4.1l58E-Ol
.4000
!l.442
8.133
1524.1511
4.llS1E-Ol
-5.013E-Ol
5.022E-02
7.70IlE-02
1.273E-Ol
.1l000
8. 1114
10.1154
1142.33
3.108E-Ol
-2.257E-Ol
2.1l35E-02
2.0815E-02
4.721E-02
.8000
10.885
13.575
ll13.35
2.11l3E-Ol
-1.033E-Ol
1. 5llllE -02
5.41l3E-03
2.142E-02
1.0000
13.1l01l
18.2llll
71l0.83
1 .1l07E-0 1
-4.111E-02
1.0158E-02
1.03IE-03
1.11l2E-02
1.2000
11l.327
Ill. 017
1l51.ll7
1.250E-Ol
-8.81IlE-03
7.411IlE-03
3.331E-05
1.1I00E-03
1.4000
111.048
21.73ll
570.315
1.004 E-0 1
·1.307E-02
5.1513E-03
1.400E-04
5.1l113E-03
:2 .0000
27.212
2ll.ll02
414.84
5.ll53E-02
3.1130E-02
2.1l1l41-03
1.4815E-03
4.14llE-03
3.0000
40.818
43.508
284 .ll7
3.203E-02
3.1I8H-02
1.122&-03
2.1l08E-03
3.730E-03
4.0000
54.424
57.114
217.0ll
2.037&-02
3.51l8E-02
S-.ll5I1E-04
2.74lE-03
3.331l&-03
5.0000
1l8.030
70.720
175.32
1. 4215E-02
3.097E-02
3.1I09E-04
2.557E-03
2.ll1IE-03
25
AS V
USD
EO.
t , 0158E-OI
(RYD)
N·· 15.2455
MU·
.7545
E (RYD)
E (EV)
E PHOT <EV)
LAMBDA
(A)
(L/R/L-I)
(L/RIL+I)
SICMA L-I
SICMA L+ 1
SIGMA (MIS)
.0000
.000
1.483
8412.12
5.090E+00
-8.195E+00
8.531E-OI
5.284E+00
8.247E+00
.1000
1.381
2.824
43l10.31
I.752E+00
-2.8110E+00
2.17I1E-OI
8.885E-OI
I.I07E+00
.2000
2.121
4.185
21182.88
8.288E-Ol
-1.328E+00
8.075E-02
2.715E-Ol
3.883E-OI
.4000
5.442
8.1I01S
1191.311
4.14IE-Ol
-4.428E-OI
2.871E-02
5.I07E-02
8.084 E -02
.8000
10.885
12.348
1004.08
1.811E-Ol
-8.411E-02
8.11I1E-03
3.341 E-03
1. 148E -02
1.0000
13.808
15.0811
822.77
1.170E-OI
-3.5021-02
5.188E-03
8.1I10E-04
5.883E-03
1.2000
18.327
11.1111
8l18.112
8.1121E-02
-8.815E-03
3.584E-03
4.1I1I1E-05
3.813E-03
1.4000
111.048
20.512
804.47
7.014E-02
8.304E-03
2.580E-03
3.074E-05
2.811E-03
1.8000
21.188
23.233
533.87
5.788E-02
1.504E-02
1.843E-03
1.8821-04
2.14IE-03
3.0000
40.818
42.281
2113.24
2.147E-02
2.5110E-02
4.8117E-04
1.070E-03
I.558E-03
4.0000
54.424
51.8.7
221.85
1.34I1E-02
2.312E-02
2.555E-04
1.128E-03
1 .381 E -03
5.0000
88.030
811.4l13
118.42
8.358E-03
2.000E-02
1.52I1E-04
1. 0411E -03
1.201E-03
8.0000
81.8311
83.0llll
1411.20
8.1127E-03
1.73IE-02
1.002E-04
8.388E-04
I.03I1E-03
AS V
20D
EO· 8. 14113E-02
IRYD)
N·· 18.2480
MU·
.7540
E ( RYD)
E (EV)
E PHOT (EV)
LAMBDA
lA)
IL/R/L-l)
(L/RIL+I)
SIGMA L- 1
SIGMA L+ 1
SIGMA
(MISI
.0000
.000
.818
13.1501.87
7.848E+00
-1.540E+OI
1.3150E+00
8.214E+00
Il.584E+00
.1000
1.381
2.2111
5440.83
1.152E+00
-2.1181E+00
1.758E-Ol
7.838E-Ol
Il.387E-Ol
.2000
2.721
3.8311
'3408.10
8.242E-Ol
-1.208E+00
8.214E-02
2.002E-Ol
·2.823E-Ol
.4000
5.442
8.381
111411.27
3.353E-Ol
-3.875E-Ol
1.7117E-02
3.23I1E-02
5.038E-02
.8000
8.184
Il.082
1385.21
I.888E-Ol
-1.507E-Ol
8.12IE-03
7.772E-03
1.588i-02
.8000
10.885
Il.803
1050.48
1.234E-Ol
-8.710E-02
4.518E-03
2.003E-03
8.518E-03
1.0000
13.808
14.524
853.85
8.801E-02
-2.802E-02
2.832E-03
4.2I1l1l-04
3.282E-03
1.2000
18.327
11.245
118.115
8.8·58E-02
-7.853E-03
1 .1121 E-03
3.80n-05
1 . IIII1E -03
1.4000
18.048
111.887
820.117
5.242E-02
3.728E-03
1.37I1E-03
1.0451-05
1.3110E-03
1.8000
21.1811
22.888
548.411
4.24I1E-02
I.033E-02
1.030E-03
Il. 125E-05
1 . 121 E -03
2.0000
27.212
28.130
440.18
2.1183E-02
1.85IE-02
8.2110&-04
2. 8UE -04
Il.183E-04
3.0000
40.818
41.738
2117.07
1.551E-02
1.847E-02
2.524E-04
5. 311E -04
7.8114E-04
4.0000
54.424
55.342
224.04
8.8115E-03
1.847E-02
1.307E-04
5. 8511E -04
8.1188E-04
5.0000
88.030
88.'48
1111.83
8.70 1E-03
1.423E-02
7.783E-05
5.2831-04
8.041E-04
AS V
4F
10.
I.5182E+00 (RYD)
N·· 3.11825
MU·
.0175
E (RYD)
E (EV)
1 PHOT (EV)
L....O.
(A)
(L/R/L-l)
(L/II/L+l)
SIGM. L - 1
SI GIIlA
L- 1
SIGMA (M8)
.0000
.000
2J.44e
518.12
1.031E-Ol
r , 05.E +00
8.20llE-03
8.840E-OI
8.702E-Ol
1.0000
13.808
35.052
353.12
4.824(-02
3.324E-Ol
2.018E-03
t .3110E-Ol
1.41IE-01
2.0000
27.212
48.858
254.81
2.5811-02
1.503E-Ol
8.838E-04
3.1141E-02
4.0341-02
4.0000
54.424
15.870
183.42
1.010E-02
• 5.085E-02
2.338E-04
7.044E-03
7.278E-03
8.0000
81.835
103.082
120.28
5.520E-03
2.4231 -02
8.45I1E-05
2.113E-03
2.257E-03
AS V
5F
EO·
1.0102E+00 (RYD)
N·· 4.11148
MU·
.0252
E (RYD)
E (EV)
1 PHOT (EV)
LAMISDA
lA)
(L/R/L-I)
IL/R/L+II
SICMA L- 1
SIGMA L+l
SIGMA (M8)
.0000
.000
13.744
1102.10
2.081E-Ol
1.1111 E+OO
1.803E-02
1.803E+00
1.81I1E+00
.5000
8.803
20.541
803.42
1.111E-Ol
8.348E-Ol
8.82I1E-03
5.1421-01
5. 210E -01
1.0000
13.80e
21.350
453.33
8.1148E-02
4.5031-01
3.554E-03
1 .1I1I2E-0 1
2.027E-Ol
2.0000
27.212
40.1158
302.13
3.4201-02
1.82IE-Ol
1.2l10E-03
4.878E-02
5. 007E -02
3.0000
40.818
54.582
227.24
1 .1I110E-02
Il.401 E-02
5.822E-04
1.731E-02
I.7110E-02
4.0000
54.424
88.188
181.88
1 ..218E-02
5.5113E-02
2.88I1E-04
7.8511-03
1. 1158E - 03
AS V
8F
EO. 7.0130E-Ol
( RYDI
N·· 5.11708
MU·
.. 02114
E (RYD)
(EV)
E PHOT (EV)
LAM8DA
(A 1
(L/R/L-I)
IL/R/L+l)
SIGMA L - 1
SIGMA L+ 1
SIGMA (M8)
.0000
.000
Il.542
1211t.311
3.225E-Ol
2. 80SE +00
2.8131-02
:1.702E+00
2. 7211E+00
.5000
8.803
18.345
158.57
1.418E-Ol
1.0051 +00
8.854E-03
5.828E-OI
8.014E-Ol
1.0000
13.808
23.148
535.83
8.08111-02
4.11451-01
4.07I1E-03
2.033E-Ol
2.073E-Ol
2.0000
27.212
38.154
337.34
3.8331-02
1.833E-OI
1.308E-03
4.434E-02
4.584&-02
3.0000
40.818
50.380
248.20
2.011E-02
Il.072E-02
5.520E-04
1.488E-02
1.5441-02
4.0000
54.424
83.11118
1113.83
1.251E-02
5.2881-02
2.721E-04
8.38I1E-03
8.84IE-03
AS V
8F
10. 3.113112E-Ol
(RYD)
N·· 7.11884
MU·
.0338
E (RYD)
E (EV)
E PHOT (IV)
LAM8DA
lA)
(L/R/L-l)
(L/R/L+l)
SICMA L- 1
SICMA L + 1
SlalllA
(M8)
.0000
.000
5.380
2313.31
5.853E-OI
4.782E+00
4.812E-02
4.402E+00
4.448E+00
.5000
8.803
12.183
10111.40
1.884E-Ol
1.127E+00
Il.284E-03
5.54I1E-Ol
5.842E-Ol
1.0000
13.801S
18.1188
853.14
8.3441-02
4.802E-Ol
3.558E-03
1.571 E -0 1
1.8081-01
2.0000
27.212
32.512
380.88
3.3181-02
1.582E-Ol
Il.8401 -04
2.1128E-02
3.0241 - 02
3.0000
40.818
48.171
288.50
1.13l1l-02
7.440E-02
3.1821-04
Il.1781-03
Il.5541-03
4.0000
54.424
511.783
207.3l1
1.0481-02
4.1118E-02
1.770E-04
3.780E-03
3.1157E-03
5.0000
88.030
73.3811
188.114
8.88IE-03
2.8481-02
Il.351E-05
1 .84111 -03
1 .1I42E -03
AS V
lOF
EO· 2.5178E-Ol
(RYDI
N·· Il.11845
IIIU·
.0355
1
(RYD)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(LIR/L-l)
(L/R/L+I)
SICIIIA L - 1
SIGMA L+ 1
SIGMA (MIS)
.0000
.000
3.428
38111.24
8.111 E-O 1
7.014E+00
8.010E-02
8.052E+00
8.113E+00
.5000
8.803
10.2211
1212.14
1.813E-Ol
1.0114E+00
7.712E-03
4.311I1E-Ol
4.478E-Ol
1.0000
13.808
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211.588
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1.083E-Ol
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1. 201 E -02
1 .244 E-02
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3.58"E-02
3.118I1E-Ol
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Il.281E-02
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10.885
15.102
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4.551E-03
5.7118E-02
1.310E-05
5.711I1E-02
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3.1151E-02
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1.111I1E-02
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8.211IlE-03
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2.8118E-02
2.283E-03
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2.888E+00
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2.Sl7.88
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10.885
13.127
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1.825E-08
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1.3811
81127 .• 5
1.038E+Ol
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3. 135E+00
1.113E-00
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2.721
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3.358E-02
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10.885
12.274
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2.1583E-OI
-3. 138E-03
1.851 E-02
5.057E-08
1.851E-02
1.0000
13.808
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Il .• '21-03
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5.585E-05
1.I54E-02
2.0000
27.212
28.801
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1.8.2E-02
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2.855E-03
3.0000
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287 .• 3
2.0.n-Ol
1.1110E-Ol
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7.380E-02
1.0000
13.808
511.1187
2015.715
1.3"IIE-Ol
1.80SE-Ol
2.7.2E-02
7.372E-02
1.011E-Ol
2.0000
27.212
73.573
1158.52
SI.678E-02
1. 85"E-0 1
1.732E-02
SI.5331-02
1. 1215E-0 1
3.0000
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1.181E-02
1 .001 E-01
1.120E-Ol
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100.785
123.02
5.711. E-02
1.511I1E-Ol
8.5015E-03
SI.71.E-02
1.0515E-Ol
8.0000
108.8.7
155.2011
7S1.88
2.850E-02
1.08.E-Ol
3.16I1E-03
15.8715E-02
7.1113E-02
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1.11742E+00 (RYD)
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4.2703
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28.8111
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3.731E-Ol
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Il.397E-02
4.7117E-03
IL874E-02
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1.3111
28.221
4311.34
3.440E-Ol
-2.8110E-02
8.3112E-02
8.887E-04
8.481E-02
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2.721
211.582
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3.183E-Ol
3.787E-03
7.53IlE-02
1. 1I00E - 05
7.53I1E-02
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5 :442
32.303
383.82
2.755E-Ol
5.31I1E-02
Il. 1111 E-02
3.442E-03
Il.505E-02
.11000
8. 184
35.024
354.00
2.411E-Ol
8.715E-02
5.11I1F-02
1. 003E -02
Il.122E-02
1.0000
13.11011
40.41111
3011.311
1.1101 E-O 1
1.2117E-Ol
3.117I1E-02
2.44I1E-02
Il. 1211E-02
2.0000
27.212
54.072
2211.30
1.178E-Ol
1.523E-Ol
1.88I1E-02
4.727E-02
Il.1I13E-02
3.0000
40.818
117.1178
183.20
8.117E-02
1.41l1E-Ol
1 . 121E -02
5.370E-02
Il.4111E-02
4.0000
54.424
81.284
152.53
5.1180E-02
1.312E-Ol
7.307E-03
5.27I1E-02
Il.010E-02
8.0000
108.847
135.708
111.311
2.52I1E-02
8.377E-02
2.177E-03
3.5111E-02
3.808E-02
SE VI
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1.21124E+00 (RYD)
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5.7114E-01
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1.484E-Ol
Il.534E-02
2. 13.7E -01
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4.082
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1l72.27
4.107E-Ol
-1I.343E-02
Il.184E-02
7.131E-03
Il.8117E-02
.4000
5.442
23.0211
538.411
3.714E-Ol
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7.118IlE-02
2.085E-03
8.1113E-02
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Il.803
24.387
50'.42
3.37I1E-Ol
-1.3111E-02
Il.11117E-02
1.703E-04
7.014E-02
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8.1114
25.747
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3.08I1E-Ol
1 .4 711E - 02
Il. 175E-02
2. 1 14E -04
Il.1117E-02.
1.0000
13.11011
31.1'0
3117.52
2.250E-Ol
8.310E-02
3.III1I1E-02
8. 12 lE -03
4.7I1E-02
2.0000
27.212
44.71111
2711.78
1.234E-Ol
1.257E-Ol
1.714E-02
2.III1I1E-02
4.382E-02
3.0000
40.818
58.402
212.30
7.1I1I1E-02
1.20IlE-Ol
Il.205E-03
3.220E-02
4.140E-02
4.0000
54.424
72.007
172. 111
5.5118E-02
1.083E-Ol
5.1112f -03
3.182E-02
3.743E-02
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Il.232
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1.01l5E+00
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2.784E-Ol
3.2118E-Ol
Il.052E~01
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2.721
11.IIB3
1037.211
7. 154E - 01
-4.5118E-Ol
1.538E-Ol
Il.403E-02
2.478E-Ol
.4000
5.442
14.874
844.111
5.101E-Ol
-2.152E-Ol
Il.5117E-02
2.5112E-02
1.21I1E-Ol
.8000
8. 184
17.3'11
712.75
3.852E-Ol
-8.755E-02
Il.488E-02
5.027E-03
Il.11111 E-02
.8000
10.881l
20.117
11111.33
3.02I1E-Ol
-1.513E-02
4.1140E-02
1 . 738E -04
4.1157E-02
1.0000
13.1108
22.838
542.110
2.45IlE-Ol
2.7851-02
3.4110E-02
Il.1I78E-04
3.8281-02
2.0000
27.212
311.4."
340.21
1.127E-Ol
8.81581-02
1.184E-02
1.078E-02
2.241E-02
3.0000
40.818
50.0eO
247.73
8.815E-02
8.11281-02
5.5041-03
1 . 40llE -02
1 .III1I5E -02
4.0000
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7.11131-02
3.103E-03
1 .3111 E-02
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SE VI
10D
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1.738E+00
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7.17GI-Ol
1.148E+00
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2.721
8.401
1475.83
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1.337E-Ol
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13.843
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5.1577E-02
Il. &!lSlE - 03
Il.15831-02
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10.885
111.15815
748.1l0
2.117I1E-Ol
-4.754E-02
3.1187E-02
1.412E-03
3.828E-02
1.0000
13.11011
111.28e
1142. &li
2.313E-Ol
1.827E-03
2.5113E-02
2.427E-OII
2.15114E-02
2.0000
27.212
32.8112
378.115
Il.411111-02
Il.55I1E-02
7.415I1E-03
5.331E-03
1 . 2711i -02
3.0000
40.8111
411.4118
21111.85
5.304E-02
Il.434E-02
3.288E-03
7.258E-03
1.055E-02
4.0000
54.424
110.104
208.2.
3.432E-02
Il.112I1E-02
1.77I1E-03
7. 180E-03
8.115I1E-03
5.0000
111.030
73.7011
1118.21
2.423E-02
4.8481-02
1.087E-03
Il.531 E-03
7.1I1I1E-03
Il.0000
81.835
87.315
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1.812E-02 .
4. 1811E - 02
7.207E-04
8.778E-03
8.411I1E-03
SE VI
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SIGMA L+I
SIGMA (M8)
.0000
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3.844
3225.08
2.411I1E+00
-2.8851+00
Il.034E-Ol
1 . 207E +00
1.810E+00
.2000
2.7:1
Il.588
1888.42
1.035E+00
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1.78I1E-Ol
1.1148E-Ol
3.7115E-OI
.4000
5.442
Il.287
1335.08
5.852E-Ol
-3.588E-Ol
7.11114E-02
4.50IlE-02
1.210E-Ol
.8000
10.885
14.7211
841.77
2.733E-Ol
-5.11031-02
2.711I1E-02
1.1135E-03
2.11801-02
1.0000
13.8011
17.450
710.51
2.0&4E-Ol
-1I.41lIlE-03
1.8I1l1!-02
5.882E-05
1 . 875E -02
2.0000
27.212
31. ose
31111.23
7.8113E-02
5.0117E-02
4.8113E-03
3.00IlE-03
7.811I1E-03
3.0000
40.818
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277.111
4.280E-02
4.91141-02
2.05I1E-03
4 . 11111 E- 03
Il. 25.5E -03
4.0000
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58.2118
212.711
2.724E-02
4.3"111-02
1. 087E -03
4. 1411E-03
5.23eE-03
5.0000
118.030
71.174
172.51
1.1I03E-02
3.725E-02
Il.5''IIE-04
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4.41 5E -03
SE
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15.28811
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2.0'11
51118.73
4.31l2E+00
-5.550E+00
Il.1I78E-Ol
2.433E+00
3.431E+00
.1000
1.3111
3.458
31l87.45
1.1I11E+00
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3.171E-Ol
5.1I"8E-0 1
8.8181-01
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5.4"2
7.538
111"4.84
5.307E-Ol
-3.51151-01
5.338E-02
3.1173E-02
Il.00IlE-02
.8000
8.184
10.21511
1208.55
3. 1114E-0 1
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2.83IE-02
8.388E-03
3. 488E -02
.8000
10.885
12.1180
Il.55. III
2.18I1E-Ol
-5.82I1E-02
1.530E-02
1.1183E-03
1.11117E-02
1.0000
13.11011
15.701
78'.115
1.580E-Gl
-1.523E-02
Il.8!l71-03
1.37"E-04
Il.1I114E-03
2.0000
27.212
211.307
423.08
5.57I1E-02
3.3281-02
2.2113E-03
1.2241 -03
3. 517E -03
3.0000
40.818
42.1113
288.112
2.1133E-02
3.2'''E-02
Il. 2711E-04
1 . 758E -03
2.88"E-03
4.0000
54.424
511.5111
2111.37
1.8311E-02
2.851E-02
4.7111E-04
1.733E-03
2.212E-03
5.0000
118. 030
70.125
1711.81
1.271 E- 02
2.432E-02
2.848E-04
1.583E-03
1.8"8E-03
SE VI
20D
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1.3111
11418.23
Il.822E+00
-8.1117E+00
1.451E+00
3.1I"7E+00
Il.3117E+00
.1000
1.3111
2.1177
41131.47
2.082E+00
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2.880E-Ol
5.547E-Ol
8.407E-Ol
.4000
5.4"2
Il.71511
1834.44
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3.455E-02
2. 587E -02
8.042E-02
.11000
8.1114
Il.480
1307.87
2.584E-Ol
-1.255E-Ol
1. 5111 E-02
5.831E-03
2. 154 E -02
.8000
10.885
12.201
10111.18
1.703E-Ol
-4.1182E-02
8. 8lI8E -03
1.142E-03
1. 004E -02
1.0000
13.8011
14.1122
830.88
1.220E-Ol
-1.44I1E-02
5.587E-03
1.18lE-0"
5.705E-03
2.0000
27.212
28.528
434.111
4.1"OE-02
2.387E-02
1.22I1E-03
Il. 127E-04
1. 8.. 2E -03
3.0000
40.818
42.134
211... 27
2.144E-02
2.388E-02
4.8118E-04
8.1I0IlE-04
1.377E-03
4.0000
54.424
51l.740
222.44
1.331E-02
2.0"3E-02
2.481E-04
8.772E-04
1 . U5E -03
5.0000
118.030
1111.348
178.711
Il. 183E -03
1. 7311E - 02
1.48.. E-04
7.1I0IlE-04
Il.370E-04
Il.0000
81.831l
82.11152
1411.47
Il. 734E-03
1. "88E-02
Il.45I1E-05
Il.1127E-04
7.872E-04
30
SE VI
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3.11742
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31.013
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277.88
s , 231 E-02
3.258E-OI
3.288E-03
1.1l11!-01
1.732E-Ol
2.0000
27.212
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212.1!l
3.11IE-02
1.740E-Ol
1 .804 E-03
8.330E-02
8.4110E-02
4.0000
54.424
8!l.438
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1 . 500E -02
8.1117E-02
5.17!lE-04
1 . !l02E -02
1.554E-02
8.0000
81.83!l
112.6"8
110.07
8.340E-03
3.833E-02
2.110E-04
5.338E-03
!l.54IE-03
8.0000
108.147
1311.880
88.85
!l.135E-03
2.188E-02
9.1133E-05
2.311ll-03
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111.882
123.1l0
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1.354E+OO
2.2110E-02
1.301E+OO
1 . 332E +00
1.0000
13.808
33.488
370.24
8.523E-02
4.858E-Ol
8.!l52E-03
2.807E-Ol
2.1l72E-Ol
2.0000
27.212
47.014
21l3.27
4.810E-02
2.231E-Ol
2.IlIIIlE-03
8.420E-02
8.8110E-02
4.0000
54.424
74.308
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7.2114E-04
1.737E-02
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7.741l
11l00.71
Il.278E-Ol
3.344E-00
8.221 E-02
3.110E+OO
3.1112E+OO
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2.277E-Ol
1.130E+OO
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8.888E-02
8.81lIlE-04
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5.174E-02
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4.714E-Ol
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7.21l8E-02
4.457E-04
8.3I1SE-03
8.83U-03
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173.50
7.585E-03
2.880E-02
l.l07E-04
1.843E-03
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Il.315E-01
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3.1153E-03
4.170E-03
4.0000
54.424
58.350
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8.094 E-03
2.884E-02
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1.883E-03
1.782E-03
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3.11152
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8.471E-Ol
8.780E-Ol
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Il.8110E-02
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112.321
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872.57
1.112E+00
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3.1181E-Ol
1.1187E-03
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1140.38
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3.372E-Ol
7.305i-04
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1.887E-02
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5.485E-02
1.72I1E-Ol
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8.771E-Ol
.0200
.272
7.573
1837.15
1 .1I77E +00
-5.305E-02
6.201E-Ol
8.1128E-04
8.210E-Ol
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.50404
7.8045
1580.38
1.884E+00
-3.33I1E-02
5.710E-Ol
3.884E-04
5.714E-Ol
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8.118
1527.311
1.781E+00
-1.827E-02
5.273E-Ol
8.119U-05
5.274E-OI
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1.088
8.3S10
1477.85
1 . 887E +00
-1.315E-03
4.882E-Ol
8.078E-07
4.8'2E-Ol
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1 .381
8. ll82
10431.042
1.580E+00
1.177E-02
4.531E-Ol
5.023E-05
4.531E-Ol
.2000
2.721
10.022
1237.10
1.238E-00
5. 880E -02
3.220E-Ol
1.355E-03
3. 233E -0 1
.5000
8.1804
15.0488
801.74
5.1185E-Ol
1.014E-Ol
1.180E-Ol
8.882E-03
1.227E-Ol
.8000
10.885
18. 188
881.77
4.558E-Ol
1.002E-Ol
7.Sl08E-02
7.857E-03
8.873E-02
1.0000
13.808
20.1107
5S13.03
3.802E-Ol
Il.574E-02
5.882E-02
8.02I1E-03
8.48I1E-02
2.0000
27.212
304.513
35S1.25
1.543E-Ol
8.1148E-02
1.720E-02
Il.Sl80E-03
2.418E-02
3.0000
040.818
048.1111
2117.87
8.78I1E-02
5.1118E-02
7.750E-03
5.448E-03
1.320E-02
KR VIII
18P
EO· 2.874lE-Ol
(RYD)
N••
104 .112204
MU'
1 . 0778
E (RYD)
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3.aI4E+00
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1 . 1111 E + 00
2.442E-02
1.218E+00
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1.088
04.111111
2480.28
2.532E+00
-1.311I1E-Ol
8.71 lE-Ol
4.01lIlE-03
8.752E-Ol
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1.381
5.271
2352.21
2.317E-00
-1.043E-Ol
5.Sl28E-Ol
2.400E-03
5.1152E-Ol
.2000
2.721
8.832
1881.82
1.578E-00
1.87I1E-03
3.45I1E-Ol
Il.805E-07
3.459E-Ol
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4.082
7.1IS12
111111.33
1.1S4E+00
04 . 740E -02
2.230E-Ol
7.524E-04
2.238E-Ol
.04000
5.04042
Il.353
1325.88
8.885E-Ol
8.7115E-02
1.540E-Ol
1.80IlE-03
1.5118E-Ol
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10.885
14.7118
838.02
4.0118E-Ol
7.889E-02
5 . 11111 E - 02
3.858E-03
5.584E-02
1.0000
13.808
17.518
707.83
3.080E-Ol
7.413E-02
3.480E-02
4.033E-03
3.883E-02
2.0000
27.212
31.122
398.38
t , 183E -0 1
5.0121-02
8.811 E-03
3.27I5E-03
1.20SlE-02
3.0000
040.818
0404.728
277.20
8.28I1E-02
3.811 E-02
3.883E-03
2.443E-03
8.128E-03
KR V1 I l
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1.7873e-Ol
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5.1178E+00
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1.820E+00
7.051E-02
1.8111E+00
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1.088
3.520
3!522.10
3.224E+00
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7.885E-Ol
1. 0811E -02
7.7721-01
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1 .381
3.7112
32811.37
2.847E+00
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8.438E-Ol
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8. 504E- 01
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2.721
5.153
2408.12
1.704E+00
-3.435E-02
3.133E-Ol
2.548E-04
3.138E-Ol
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04.082
Il.514
11103.52
1.150E+00
2.533E-02
1. 804E -01
1.8111E-04
1.808E-Ol
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5.4042
7.874
1574.80
8.381E-Ol
5.053E-02
1. 153E-0 1
8.423E-04
1.181 E-O 1
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10.885
13.318
1131.07
3.44I1E-Ol
8.228E-02
3.317E-02
2. 1804E - 03
3.534E-02
1.0000
13.808
111. 038
773.011
2.51I1E-Ol
5.787E-02
2. 131 E- 02
2.250E-03
2.3118E-02
2.0000
27.212
211.80404
0418.28
8.883E-02
3.755E-02
4.1I00E-03
1.751E-03
8.85lE-03
3.0000
40.818
43.2S0
288.88
4.887E-02
2.854E-02
1.1173E-03
1.278E-03
3.24I1E-03
KR VIII
040
EO' 5.82381+00
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3.3150
MU'
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1.322E-Ol
1.1183E-Ol
3.483E-02
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1.4S1I1E-Ol
1.0000
13.1l08
112.844
133.54
1.01I1E-Ol
1 .1I38E -0 1
2.403E-02
1.313E-Ol
1.553E-Ol
2.0000
27.212
108.450
118.047
8. 08U - 02
1.824E-Ol
1.7421-02
1.335E-Ol
1.50IlE-Ol
3.0000
040.818
120.058
103.27
8.511IE-02
1.888E-Ol
1 .311 E -02
1.287E-Ol
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287.72
2.440E-Ol
1 .5.1 E -0 1
6.1133E-02
4.418E-02
1. 135E-0 1
1.0000
13.808
511.• ,8
208.Sl3
1 .581 E-0 1
1.804E-Ol
3.783E-02
7.352E-02
1.1121-01
2.0000
27.212
73.524
188.83
1. 117E-0 1
1.711E-Ol
2.307E-02
8.180E-02
1.04I1E-Ol
3.0000
40.818
87.130
1042.30
8.385E-02
1.583E-Ol
1.532E-02
8.028E-02
•. 581E-02
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EO' 2.240IlE·00
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3.1147E-02
9.404E-02
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281.18
2.057E-Ol
1.828E-Ol
4.888E-02
4.394E-02
9.0821-02
2.0000
27.212
57.701
2104.88
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1.577E-Ol
2.480E-02
5.413E-02
7.873E-02
3.0000
040.818
71.307
173.88
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1.473E-02
5.38llE-02
8.8042E-02
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504.04204
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8.711E-02
1.24111-01
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4.115I1E-02
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N·. 7.3508
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8.1178e-03
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2.832E-Ol
1.255E-Ol
5. 178E - 02
1.785E-02
8.1142E-02
2.0000
27.212
043.328
288.16
1.387E-Ol
1.284E-Ol
2.0118E-02
2.8114E-02
4.7110E-02
3.0000
040.818
58.11304
217.77
8.887E-02
1.120E-Ol
1.080E-02
2.8111E-02
3.770E-02
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13.11015
23.5150
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0.558E-02
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3.753E-Ol
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8.223E-02
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7 .• 82E-0(1
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4. 8.8E -02
1. SSiE -0 1
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2. 730E "00
1.831E-Ol
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15.01 tE-Ol
1.080E-02
2.01.E-Ol
3.112E-Ol
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315.0153
3.3.81
7.832E-02
2.S15E-Ol
5.iSn-03
8.85n-02
0 .• 53E-02
3.0000
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4.355E-02
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4.002(-02
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715.881:'
115 1 .27
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7.3S8E-04
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3.228E+00
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5.1153E-Ol
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2.2S5E-Ol
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27.212
33.3.3
371.85
7.040E-02
2.280E-Ol
4 .• 5tE-03
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7.5lS7E-02
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1.2.5E-02
1.33.E-02
5.0000
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1157.18
1 . 5711E- 02
5.113E-02
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7 .• 57E-03
38
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2.192E+00
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04.589E+00
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8.803
10.2041
1210.71
3.807E-Ol
1.01l8E+00
3.58BE-02
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04.5040E-Ol
1.0000
13.808
17.0.04
727 .• 11
1.522E-Ol
•. 859E-Ol
1.083E-02
1.32tE-Ol
1 .• 351-01
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27.212
30.850
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5 .• 50E -02
1.710E-Ol
2 .• 52E-03
3.219E-02
3 .• 8.E-02
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8.831E-02
9.313E-0"
1.239E-02
1.333E-02
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57.882
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5.358E-02
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3.307E+00
8.283E+00
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8. 031E +00
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2.721
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8.831E-Ol
2.0408E+00
1.033E-Ol
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1.212E+00
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8.718E-02
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27.212
174.374
71.10
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8,7114E-02
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27.212
105.212
117.84
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1113.77
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8.437E-02
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88.030
173.8112
71.40
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Il.811I1E-02
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5.14I1E-02
5.14I1E-02
10.0000
1311.0511
241.11112
51.30
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4.2711E-02
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2.7771-02
2.777E-02
MO XIV
85
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2211.80
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2.407E-OI
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1.1I114E-Ol
I.1I54E-Ol
4.0000
54.424
108.3711
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8.7114E-02
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5.23tE-02
5.231E-02
8.0000
108.847
1112.802
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4.814E-02
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2.371E-02
2.371E-02
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1MB)
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32.1188
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3 . 1111 TE- 0 1
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2.753E-Ol
2.753E-OI
4.0000
54.424
87.1011
142.33
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8.1I10E-02
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4.058E-02
4.0581-02
8.0000
108.847
141.5:13
81.110
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4.1117E-02
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1.545E-02
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1110 XIV
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21.1105
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5.134E-Ol
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3.1128 E - 0 1
3.1128E-Ol
4.0000
54.424
111.328
1112.44
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1.1132E-02
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3.01 8E - 02
3.018E-02
8.0000
108.847
130.752
114.83
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3.522E-02
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1.01I1E.02
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1110 XIV
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11.191
1050.1115
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8.100E-Ol
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5.512E-Ol
5.512E-Ol
3.0000
40.BI8
52.1515
235.155
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8.95I1E-02
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2.558E-02
2. 55aE -02
Il.0000
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93.433
132.70
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3.738E-02
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8.195E-03
8.195E-03
MO XIV
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I.308E-00
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1.881E-Ol
2.0000
27.212
34.512
358.84
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I.214E-Ol
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3.200E-02
3.200E-02
4.0000
54.424
81.183
200.88
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4.1115E-02
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9.80IlE-03
MO XIV
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2811.204
48.08
5.443E-02
1.58H-02
I.511E-02
8.458E-02
8
1211E-02
2.0000
21.212
298.418
41.83
4.551E-02
8.848E-02
1 . 343E - 02
5.8241-02
7, 187E -02
4.0000
54.424
323.828
38.31
4.028E-02
Il.228E-02
I.IOOE-02
5.258E-02
8.358E-02
MO XIV
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80.112
Il.800E-02
i . 033E-0 1
3.083E-02
8.8521-02
Il.1I35E-02
3.0000
40.al8
1114.042
83.90
8.81I1E-02
8.030E-02
I.181E-02
5.242E-02
1.023E-02
8.0000
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234.8511
52.111
4.8121-02
8.457E-02
1.13I1E-02
4,I02E-02
5.24 tE-02
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2.1801-02
4.8110E-02
1.010E-02
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5.8051-02
8. 1511E-02
1.1111 E-02
3.483E-02
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240.32
2.1184E-OI
1.1184E-Ol
Il.41111E-02
8.340E-02
1.184E-OI
3.0000
40.818
112.410
134. t1
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I.Ol2E-OI
2.407E-02
3.1I117E-02
Il.37<4E-02
Il.0000
81.835
133.221
113.08
5.119I1E-02.
Il.487E-02
1 . 004E - 02
2.334E-02
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MO XIV
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1MB)
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3112.110
4.8111E-OI
2.1151E-Ol
I.533E-Ol
Il.2114E-02
2.4112E-OI
2.0000
21.212
58.1811
210.111
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3.541E-02
4.103E-02
7. 850E -02
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8.1115E-02
1.078E-02
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2.350E-02
3.181E-02
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S82.82
7.088E-Ol
3.388E-Ol
2.228E-Ol
1.022E-Ol
3.250E-Ol
2.0000
27.212
48.483
2511.88
1.774E-Ol
1.273E-0·1
3. 188E-02
3.284E-02
8.482E-02
4.0000
54.424
75.704
183.78
8.338E-02
7.288E-02
1.103E-02
1.878E-02
2.778E-02
MO XIV
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1.273E+00
4,881E-OI
3.823E-OI
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5.128E-OI
2.0000
27.212
38.781
318.88
1.885E-Ol
1.124E-Ol
2.252E-02
2.0S0E-02
4.302E-02
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8.748E-02
5,857E-02
8.283E-03
8.848E-03
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1713.31
1 .888E+00
8.7154E-Ol
5.'83E-Ol
1.387E-01
7.380E-OI
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8.803
14.040
883.12
8.5152E-Ol
2."'E-0'
1.288E-Ol
5.283E-02
l,782E-01
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20.843
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3.375E-Ol
1 .808E-Ol
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2.857E-02
7.832E-02
MO XIV
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4.872E-02
1.358E-Ol
1.32IE-02
l,548E-Ol
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5.0000
88,030
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42.87
3.058E-02
8.823E-02
8.821E-03
1.078E-Ol
1.1471-01
10.0000
138.0'.
358.812
34.57
2.105E-02
7.484E-02
3,8113E-03
7.5841-02
7.883E-02
MO XIV
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132.757
83.38
8,058E-02
1,8'2E-Ol
2.738E-02
1.433E-Ol
1.7071-01
5.0000
88.030
200.787
81.75
4.388E-02
1. 080E-OI
8,723E-03
8.822E-02
8,784E-02
10.0000
138.058
288.818
48.12
2.1508E-02
7,448E-02
4 . 511eE- 03
5.820E-02
8.080E-02
MO XIV
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88.4.1
140.11
I.435E-Ol
2.020E-Ol
4.580E-02
l,381E-Ol
1.81U-Ol
5.0000
88.030
158.521
7 •. 21
5.304E-02
1.105E-Ol
1,1071-02
7,210E-02
8.317E-02
10.0000
138.058
224.550
55.22
2,785E-02
7.025E-02
4,378E-03
4.178E-02
4.818E-02
MO XIV
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3,4883E+00 (RYD)
N.'
7,4858
MU'
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SIGMA L-l
SIGMA L+I
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47.482
28 l. 24
2,804E-Ol
2.ll48E-Ol
8,377E-02
1 . 253E - 01
2,181E-Ol
5,0000
88.030
115.481
107.38
5.885E-02
1.043E-Ol
l,043E-02
4.735E-02
5,77IE-02
10,0000
138,058
183.521
87.58
2.828E-02
5.832E-02
3. 181 E-03
2,353E-02
2.15711-02
MO XIV
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2. 1725E+00 (AYD)
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SIGMA L-l
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28.558
418.48
4.584E-Ol
3.238E-Ol
l,548E-Ol
1. 18IE-0 1
2.718E-Ol
5.0000
88.030
87.588
127,05
5.788E-02
8.208E-02
8.248E-03
3.120E-02
3.845E-02
10.0000
138.058
185,818
74.88
2.280E-02
4.7271-02
2. 127E -03
1.385E-02
1 . 808E -02
MO XIV
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1.4821E+00 IRYD)
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20,188
814,83
8.888E-Ol
3.789E-Ol
2.275E-OI
1,088E-Ol
3,372E-Ol
5,0000
88,030
88.185
140.58
5,2 72E -02
7.854E-02
8.1153E-03
2.104E-02
2,720E-02
10.0000
138.058
1515.225
78,38
1.808E-02
3.8515E-02
1.428E-03
8.758E-03
1. 018E-02
MO XIV
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11,088
1117, 12
1. 204E +00
4.838E-Ol
4.044E-Ol
8, 788E -02
5.024E-Ol
4,0000
54,424
85,522
188.23
5.755E-02
7,43IE-02
5,454E-03
1,3871-02
1.812E-02
8.0000
108,847
118.848
103.37
1.878E-02
3.507E-02
1 , 178E -03
5.582E-03
8,741 E -03
MO XIV
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E (AYD)
E (EV)
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SIGMA L-l
SIGMA L+l
SIGMA (Mil)
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7.012
1788.15
1.875E+00
5,773E-Ol
15,1I15E-Ol
8.811E-02
7.077E-Ol
2.0000
27,212
34.224
382.28
1.288E-Ol
1.148E-Ol
1 . 383E -02
l,702E-02
3.084E-02
4.0000
54.424
81 .4315
201,81
4,585E-02
5,78IE-02
3.280E-03
7.708E-03
1.087E-02
MO XIV
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1.2783E+Ol
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3.8143
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E (EV)
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LAMBDA (A)
( L/R/L-\\)
(L/A/L+l )
SIGMA L-l
SIGMA L+l
SIGMA (Mil)
.0000
.000
174.054
71.23
3.208E-02
1.588E-Ol
4.825E-03
1.578E-Ol
1.827E-Ol
4,0000
54.424
228.477
54.27
1 . U8E -02
8.833E-02
2.125E-03
8.4011-02
8.813E-02
8.0000
108.847
282.801
43.83
l,188E-02
5.53!5E-02
1.0771-03
3.113E-02
3.220E-02
MO XIV
5F
EO. 8. 1883 E+00
(A YD)
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4.8831
MU'
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E (AYD)
E (EV)
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LAMIIDA
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(L/A/L-l)
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SIGMA L-'
SIGMA L+l
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111.382
111. 32
7,082E-02
2.711E-Ol
1.504E-02
2.838E-Ol
3.080E-Ol
4.0000
54.424
185,808
74,78
3.281E-02
1.288E-Ol
4.8371-03
8.583E-02
1. 008E -01
8.0000
108.847
220.22'
515.30
1.857E-02
7.218E-02
2, 04 SE -03
4,1171-02
4.322E-02
MO XIV
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5.8828E+00 (RYD)
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5.8832
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E (EV)
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(L/A/L-l)
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77.047
180.82
1.1.8E-Ol
3.832E-Ol
2 .•15E-02
4,082E-Ol
4.380E-Ol
4.0000
54.424
131.471
84.31
4.3815E-02
1.485E-Ol
15.843E-03
1.0411-0f
1.110E-Ol
8.0000
108.847
185.885
88.70
2.218E-02
7.728E-02
2.482E-03
3.888E-02
4.233E-02
MO XIV
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(RYD)
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7.8744
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E (EV)
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(L/R/L-l)
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SIGMA L+l
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43.00'
288.211
2.477E-Ol
5.207E-Ol
7. 104E -02
5.11150E-Ol
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4.0000
54.424
117.432
127.2!5
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1.812E-Ol
8.110E-03
Il.01l0E-02
Il.1I0lE-02
8.0000
10'.847
1!51 .855
81.155
2.357E-02
7.2112E-02
2. 272E-03
2.811I1E-02
3.125E-02
MO XIV
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9.8705
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27.371
452.118
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1.25.E-0.
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151.!58
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1. !537E-0 1
7.277E-03
5.1137E-02
7.555E-02
8.0000
108.8.7
135.2111
111.02
2.155E-02
5.310E-02
1.719E-03
1 .1I.8E -02
2.120E-02
MO XIV
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1.3111.E+00 (AYD)
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5.138E-Ol
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5.584E-02
8.872 E-02
1.457E-Ol
1.0000
13.808
15.5117
788.48
2.423E-Ol
-1.48IlE-Ol
1.814E-02
1. 400E -02
3.313E-02
2.0000
27.212
28.173
.25.01
7.1I1IlE-02
-1.288E-02
3.543E-03
2.058E-04
3.748E-03
3.0000
.0.818
42.778
288.83
3.858E-02
4.402E-04
1.334 E-03
3.473E-07
1. 335E -03
•. 0000
54.424
58.3$4
218.88
2.1l12E-02
3.002E-03
7.454E-0.
2.128E-05
7.B87l!-04
8.0000
81.835
83.588
148.32
1 . 41l4E -07
Il.223E-03
3.703E-04
Il.5UE-01l
4.858E-04
8.0000
108.847
110.808
11 1 .88
8.71I1E-03
Il.833E-03
2.182E-04
1.578E-04
3.772E-0.
CD 1 1
10P
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7. 555d -02
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N·· 7.2782
MU'
2.7238
E (RYO)
E (EV)
E PHOT (EV.
LAMBDA
(A)
(L/R/L-l)
IL/R/L+I)
SIGMA L - 1
SIQMA L+ 1
SIQIllA
(MB)
.0000 •
.000
1.028
12081.22
1.414E+Ol
-2.07I1E+Ol
4.307E+00
1.85I1E+Ol
2.287E+Ol
.1000
1.381
2.388
5180.83
3.1l27E+00
- •. 8811E+00
Il.225E-Ol
2.372E+00
2.885E+00
.2000
2.721
3.748
3307.04
1.1182E+00
-2. 148E+00
2.222E-Ol
7.248E-Ol
8 .• 70E-Ol
. 8000
8.18•
Il.182
1348.82
3.782E-Ol
-3.422E-Ol
2.7118E-02
4.508E-02
7.278E-02
1.0000
13.8011
14.1134
847.21l
1.1182E-Ol
-1.030E-Ol
8.772E-03
Il.508E-03
1 . 528E -02
2.0000
27.212
28.240
438.01l
5. 034E -02
-8.021E-03
1.488E-03
7.1112E-05
1 . 1l75E -03
3.0000
40.818
.1.848
2811.28
2.475E-02
7.10eE-04
5. 3118E - 04
8.857E-07
5. 378E -04
4.0000
54.424
55.452
223.58
1. 584E -02
2.074E-03
2.81IlE-04
8.U8E-OII
3. 015E J04
Il.0000
81.1135
82.11113
148.88
8.085E-03
3.252E-03
1.428E-04
3.1I111E-05
1.78I1E-04
8.0000
108.847
108.87!:>
112.84
Il.01l4E-03
3.1115E-03
8.4113E-05
Il.017E-01l
1 . 4.8E -04
CD 1 1
12P
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(RYO)
N.· Il.2783
MU-
2.7207
E (RYD)
E (EV)
PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L-l )
SIOMA L-l
SIQIllA L+l
SI QIllA
(Mil)
.0000
.000
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1911111.23
2.224&+01
-3.204E+Ol
Il.551E+00
2.718E+Ol
3.374E+Ol
.1000
1.3111
1.883
11222.18
3.337E+00
-4.578E+00
4.847E-Ol
1.751E+00
2.215E+00
.2000
2.721
3.353
3887.51
1.417E+00
-1.80111+00
1.410E-Ol
4.580E-Ol
5 .. 880E -0 1
.8000
8.1114
8.788
1408 ....
2.858E-Ol
-2.5871-01
1.505E-02
2.411I1E-02
3.870E-02
1.0000
13.11011
14.238
870.81
1.241E-Ol
-7.588E-02
4.58I1E-03
3.435E-03
8. 03 lE -03
2.0000
27.212
27.84.
4415.28
3.1I05E-02
-15. 587E-03
7.581 E-04
3.115IlE-05
7. 8.8E -04
3.0000
40.818
41.450
288. 12
1.750E-02
Il.283E-04
2. 115SE-04
Il.855E-07
2. 1185E -04
4.0000
54.424
51l.0511
225.20
1.112E-02
1. 512E-03
1 .• 25E -O.
5.271E-08
1.478E-04
Il.0000
81. 113Il
82.2118
150.71
Il. 348E-03
2. 2ll1lE -03
8.845E-05
1.77.E-05
8.718E-01l
CD Il
ll1P
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(RYO)
N·· 13.2818
MU'
2.7182
E (RYD.
E (IV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-n
(L/R/L+l )
SIOMA L - 1
SIQIllA L+l
SlaMA
(MB)
.0000
.000
.308
.0188.28
4.3251+01
-1I.01lIlE+Ol
1.2081+01
•. 757E+Ol
5.885E+Ol
.0200
.272
.1l81
21353.118
1.513E+Ol
-2.138E+Ol
2.78111+00
1. 111E+Ol
1.31101+01
.0800
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1.125
11022.30
Il.080E+00
-7.058E+00
Il.034E-Ol
2.348E+00
2.851E+00
.1000
1.381
1 . 11118
7428.31
2.838E+00
-3.58.E+00
2.428E-Ol
8.034E-Ol
1.14111+00
.2000
2.721
3.030
4082.37
8.858E-Ol
-1.253E+00
Il.11191-02
1.8841-01
2.1I1lE-Ol
.11000
8.1'"
8.472
14113.47
1.788E-Ol
-1.1123&-01
5.1178E-03
8.3521-03
1 . 50U -02
1.0000
13.11011
13.814
881.011
7.1183E-02
-4. 8511E-02
1.1180E-03
1.2"'E-03
2.8441 -03
2.0000
27.212
27.1l20
dO.53
2.1111E-02
-3.283E-03
2.1181E-04
1.250E-05
2.81I1E-04
3.0000
40.818
41.1211
301.48
1. 038E -02
•. 38151-0.
8.27d-05
3.2I1H-07
8.307E-05
4.0000
54.424
54.732
2211.53
Il.5IllE-03
8.1"&-04
4.818E-05
1.828E-OII
5. 112E - 011
8.0000
108.847
108. 1Sil
113.118
2.484E-03
1.473E-03
1. 411 E -es
8.8171-011
2.4021-05
10.0000
1311.058
1311.3118
80.82
1.77I1E-03
1. 4011E -03
8.008E-OII
1.1331-011
2.0341-01l
•
CD 11
20P
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1. 33.2E -02 1RYD)
N"· 17.2828
MU'
2.7172
E (RYD)
E (EV)
E PHOT IIV)
LAM5DA (A)
(L/R/L-I)
(L/R/L+I)
SlaMA L-l
SlaMA L+l
SlaMA
(M5 )
.0000
.000
.182
1180.. 7.150
7.03"1+01
- •. 11.51+01
1.8881+01
7.1751+01
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.0100
. 1311
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3881511 .•8
2.7821+01
-3.882E+Ol
5.11101+00
2.0101+01
2.52111+01
.0200
.272
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272.0.30
1.15"01+01
-2.1581+01
2.21581+00
8.81101+00
1.1121+01
.01100
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•. 1721+00
-!l.7.31+00
3.11401-01
1. "O.E+OO
1 . 71181+00
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, . 3111
1 . 5.3
80311. "II
2.0311+00
-2.71111+00
1.3331-01
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Il.21101 -0 1
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2.721
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7. '''.1-0'
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3.10.1-02
1.0021-01
1.3131-01
.11000
8. 1114
8.3.11
1••5.112
1.23.1-01
-1.12l1E·Ol
2.118H-03
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7.1131'03
1.0000
13.11011
13.788
•••. 23
S.2151-02
-3.2081'02
7.853E-0.
5 ....51-0.
1.3801-03
2.0000
27.212
27.3."
4112.110
1."1I111-02
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1.2371-0"
5.50.1-011
1 . 2.3E -0"
3.0000
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"1.000
302 .• '
7.0.IIE-03
3.02llE-0.
".211.1-05
1.573E-07
".2801-05
".0000
5..... 2..
5".11011
227.011
•. .. 2"E-03
8.15.E·0•
2.23.1-05
8.117.1-07
2.32111-05
Il.0000
81 .1135
81.818
151 .5"
2.5201-03
8.820E-0.
1.08.E-05
2.811111-011
1.355E-05
8.0000
108.8.7
10•. 030
113.72
1 .11821 -03
1. 012E-03
Il.''IIIE-OII
•. 11111-011
1.".1-05
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(RYD)
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3.0827
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1..,73
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1 (EV)
1 PHOT (EV)
LAMIDA (AI
IL/R/L-l)
IL/R/L+I)
SlaMA L-l
SIGMA L+ 1
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.0000
.000
5.727
2115.00
3. 85.E -02
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2.25IE-0.
1.82H-Ol
1.82I1E-Ol
.0200
.272
5 .•88
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8.188E-Ol
3.052E-0.
8.11112E-02
8.8I3E-02
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Il.271
'.77.11
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3.III1"E-Ol
3.855E-0"
3.227E-02
3.211I1E-02
.01100
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181 •. 23
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5.37l1E·0"
3.7.3E-05
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7.0'7
17.9.38
5.8371-02
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Il.0701-0.
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7.233E·03
.1500
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7.7118
115.8. 17
Il.2271'02
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7.5711-0"
5.323E-02
5.38.E-02
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2.721
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8.74.E·0.
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13.890
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1.18eE-03
3.31131-01
3.3751-01
1.0000
13.11011
18.333
1141.33
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-8.258E-Ol
1.288E-03
2 .•5111-01
2.811.1-01
2.0000
27.212
32.838
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1.112IE-03
1. .. ,5E·Ol
1 ... 31 E·Ol
3.0000
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3.7871-02
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1 .11781-03
8.284E-02
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110.151
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3. 111 E-02
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8.0000
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12.0000
1113.271
1118 .••8
73.31
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3.0721-04
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3.073E-0"
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1.88.0
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3.8".E+00
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".037
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1. 1171 E+00
1.0115E-03
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27011.115
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8.8351-01
2.833E-0.
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1.35IE-Ol
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5.2111
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- •. 3751-03
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1.1112E-05
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1.50.E-02
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2.721
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20811.• 2
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1.0000
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8.0000
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3.337E-03
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111.0000
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220 .• ,5
511. 12
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Il. 12117
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1.8733
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LAMIDA (AI
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1.138E+Ol
8 .•32E-02
7.077E+00
7. 111111 +00
. 01100
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15.71.011
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3.8.5E+00
1.112111-02
1.28I1E+00
1.313E"00
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1 . 3111
2 .810
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3.11101-01
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3.1127& -02
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2.77IE-02
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10.8815
12.335
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1.11131-0"
S. 8112E - 02
5.8.1 E-02
1.0000
13.11011
15.058
823.51
2.181E-02
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1.801 E·O.
5.3.. 111-02
5.3I1AE-02
3.0000
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"2.2118
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8.0000
81.1135
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1.21131-0.
2."31E-03
2. 55.E -03
8.0000
108.8"7
110.287
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10.0000
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137.508
110. 17
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5."7.1-015
8.8231-05
1 ... 30E -0"
12.0000
1113.271
111•. 721
75.27
3.08.1-03
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3.8113E-01I
1.27111-07
3.87I1E-05
1•. 0000
180 .•83
'.'.'.13
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1.81.I-OS
2.8881-0S
2.381E-05
5.S.01-05
18.0000
2.... 8011
2"11.3511
50.33
1. 7.,1-03
3.188E-03
1.8771-015
8.30SE-05
r , 118E-0"
20.0000
272.118
273.588
.8.32
1 .••31-03
3.302E-03
1.53"1-015
1.12I1E-0.
1.27.E-0.
10
CD Il
100
EO· 8.041131-02
(RYD)
N·· 8.1318
MU'
1.8884
E CRYD)
E (EV)
E PHOT (EV.
LAIIIIDA
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(L/R/L-l )
IL/R/L+1 )
SIQMA L - 1
SI ClllIIA
L+l
SIClMA (M8)
.0000
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.823
11084.00
-3.870E+00
2.108E+Ol
3.0118E-Ol
1.377E+Ol
1.408E+Ol
.0200
.272
1.0U
11321.07
-2. 153E+00
1.1111E+Ol
1.278E-Ol
5.881E+00
5.1188E+00
.0800
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1.8311
7582.82
-8.811I1E-Ol
".1I53E+00
3.11I1E-02
1.518E+00
1.5"81+00
· 1000
1.381
2.184
5877.113
-".218E-Ol
2."25E+00
Il. 758E-03
".841E-Ol
".1I38E-Ol
. 2000
2.721
3.5....
3 .. 118.2 ..
-1I.052E-02
..... 7I1E-Ol
7.300E-0"
2.880E-02
2.753E-02
.2500
3.401
4.225
21:5" . 111
-".0"71-02
1.271E-Ol
1 . 740E -0"
2.573E-03
2.7471-03
.3000
".082
".1105
2527.84
-1.383E-02
-".1I52E-02
2.357E-05
".535E-0"
".771E-0"
... 000
5."42
8.285
11178.110
Il.37''E·03
-2.08"E-Ol
1.38"E-015
1 . 028E-0.2
1.0271-02
.8000
8.1504
8.1187
13711.88
1.85"E-02
-2.878E-Ol
7.788E-05
2."27E-02
2 ... 3 .. E-02
.8000
10.885
11.708
10511.01
1.738E-02
-2.455E-Ol
8.888E-05
2.880E-02
2. 8811E -02
1.0000
13.808
14 . •211
8511.211
1.514E-02
-2.1171-01
8.31"E-05
2."3111-02
2.4"71-02
3.0000
40.818
"1.841
2117.75
8.571E-03
-5.873E-02
7.888E-05
5.0154E-03
5.130E-03
8.0000
108.847
1011.870
113.05
3.583E-03
-8.028E·03
3.500E-05
2.88"E-04
3.013E-0"
10.0000
138.0511
138 .•82
110.58
2.820E-03
-2.722E-03
2.382 E-05
3.825E-05
8.187E-05
12.0000
183.271
18".011"
75.58
2. 0'32E -03
-1.038E-0"
1 . 703E -05
8.888E-OI
1.710E-05
'''.0000
1110.483
1111.308
8... 81
1.8371-03
1. 183E-03
1.288E-05
1.00IE-05
2.2171-05
".0000
2"4.1108
2"5.730
50 ... 8
1 . 143E-03
2.070E-03
8.088E-08
3.118n-05
4.775E-05
CD Il
120
EO· 3 . 81151E -02
(RYD)
N.'. 10.1338
MU'
1.888,2
E (RYD)
E (IV)
E PHOT lEV)
LAMIDA (A)
(L/R/L-l)
(L/R/L+ 1 )
SlaMA L - 1
SICIMA
L+l
SlaMA
(M5)
.0000
.000
.530
23311e.3lI
-7.1"7E+00
3.283E+Ol
8.805E-Ol
2.15.. E+Ol
2.222E+Ol
.0200
.272
.802
15458.12
-3. 185E+00
1. 50"E+0 1
2.020E-Ol
8.8"3E+00
7.0"5E+00
· 0800
.818
1.3"8
112011.31
-1.03I1E+00
5.211E+00
3.85"E-02
1 . 3781+00
1 . "15E+00
· 1000
1.381
1 .•111
'158.21
-".588E-Ol
2.382E+00
1.00lE-02
3.117.E-Ol
4.078E-Ol
.2000
2.721
3.251
3813.12
-1I.215E-02
".252E-Ol
8 .1I311E-04
2.218E-02
2.288E-02
.2500
3."01
3 .•31
3153.71
- ... 248E -02
1.311I1E-Ol
1.782E-04
2.1I02E-03
3.080E-03
.3000
".082
".812
28.8.50
-1.8871-02
·'.278E-02
3.2118E-05
2.131E-015
8. 1211E-05
... 000
9."42
5.1172
2078.01
".8.5E-03
-1. 4811E -0 1
3.5118E-08
".85I1E-03
".883E-03
· 8000
•. 18"
8 .811"
'''28.111
1.358E·02
-1.1171E-Ol
".032E-05
1 . 2731-02
1.2781-02
.8000
10 .••15
1'."'5
10 ••. 20
1.2I1lE-02
-1.812E-Ol
".785E-05
1.414E-02
1."'IE-02
1.0000
13.808
'''.'38
.77.10
r . l111E-02
-1.581E-Ol
..... 53E-05
1 .211111 -02
1.304E-02
3.0000
"0.818
"'.348
21111.88
8. 155E -03
-".115E-02
3.1138E-05
2.8"OE-03
2.880E-03
5.0000
88.030
lS8.580
180.84
..... 85E-03
-1.1I11E-02
3."87E-05
Il ....... E-04
Il.7110E-0''
8.0.000
108.847
1011.377
113.38
2.571E-03
-5.788E·03
1.817E-05
1 . 382E -0"
1. 583E -0"
10.0000
138.0511
138.5811
110.77
1. asilE -03
-1.118"E-03
1.225E-05
1 .1I8IE -05
3.21 o'k -95
12.0000
183.271
183.801
75.811
1."85E-.3
-7.715E-05
8.838E-08
3.878E-08
8.873E-08
'''.0000
1110."83
1111.013
8".111
1. 181 E-03
8.518E·04
8.8112E-08
5.225E-08
r , 1112E-05
18.0000
217.8115
218.225
58.82
Il. 780E-0"
1.2111E-03
5.225E-08
1 . 37lE -05
1.8113E-05
CD Il
180
EO'
2.0018E-02
(RYO)
N·· 1".1358
MU·
1 . 8504..
E (RYDI
E (EV)
E PHOT CEV)
LAMIDA (A)
IL/R/L-l)
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SlaMA L-l
SlaMA L+l
siaMA
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.272
"15521.81
·'.857E+Ol
8.231E+Ol
1.8801+00
3.1187E+Ol
... 175E +0 1
.0100
.138
... 08
30357.02
-7.800E+00
3.04"E+Ol
8.2"8E-Ol
1 ."27E+Ol
1 . "1I0E +0 1
.0200
.272
. 54"
22771.2 ..
- ... "72E+00
1.805E+Ol
2.737E-Ol
8.8110E+00
8.1183E+00
.0800
.818
1.0811
11388.23
-1.082E+00
".708E+00
3.088E-02
Il.01l1E-Ol
Il.''OOE-Ol
.1000
1.381
1.8'33
75112.7"
-4. 15"E-Ol
1 . 11211E +00
7.08"E-03
2.2111E-Ol
2.382E-Ol
.2000
2.721
2.1111"
"''''.78
~7.588E-02
3.288E-Ol
".332E-0"
1 .220E-02
1.283E-02
.2500
3.401
3.87"
337".84
-3.53"E-02
1.170E-Ol
1.153E-0"
1.8117E-03
2.012E-03
.3000
".082
".31"
28"7.55
-1 .508E-02
7.135E-03
2 .... 7E·05
8.3IeE-08
3.323E-05
... 000
5.4"2
5.715
21811.511
1.882E-03
-8.714E-02
".0821-07
1.838E-03
1.837E-03
.8000
8.18..
8.438
1"811.704
1.388E-03
-1.223E-Ol
1. "."E -05
".7571-03
4.771E-03
.8000
10.88S
1 1 . 1S7
1111.28
8.0821-03
-1.127t-Ol
1.8321-05
5.3"2E-03
5.380E-03
1.0000
13.808
13 .• 78
8113.38
7.002E-03
-1I.8,8E-02
1.710E-05
".1I21E-03
... 1I38t-03
3.0000
"0.818
.. , .0110
301.7..
3.732E-03
-2.518E-02
1 ... 311E-05
Il.8281-04
Il.1I70E-0''
5.0000
".030
88.302
181.53
2.740E-03
-1.18"E-02
1.2811E-05
3. "II2E-O"
3.82lE-0"
8.0000
108.8"7
1011.120
113.82
1.187E-03
-3.5"3E-03
8.7381-08
5. 15041-05
5.837E-05
10.0000
138.0511
138.332
110.11"
1.147E-03
- 1.11151-03
".5121-08
7.337E-08
1.1851-05
12.0000
183.271
183.543
75.81
'.1I05E-04
-5.0081-05
3.280E-08
1. '471-08
3.275E-08
14.0000
1110.483
1110.755
85.00
7.1411-04
5.1 .. 5E-0"
2 ..... 5E-08
1.1I04E-08
".3"IIE-08
18.0000
244.1108
2.. 5. 1711
50.57
4.83111-0"
Il.078E-04
1.503E-08
7.815E-08
Il.11I1E-08
CD 1 1
200
EO* 1.2181 E -02
(RYD)
PI·' 18.138"
MU·
1 .8838
E (RYD)
E (IV)
1 PHOT (EV)
LAIII5DA
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SlaMA L-l
SlaMA L+l
SIGIIIA (M5)
.0000
.000
. 185
741135.83
-2.117"1+01
Il.1I33E''01
3.878E+00
8.158E+Ol
8.523E"01
.0100
. 138
.302
.. 1120.114
-11.11301+00
3.517E+01
7."7"1-01
1."07E+Ol
1 ."81E+Ol
.0200
.272
.438
28334.85
-".880E"00
1 .813E+Ol
2.81I1E-Ol
5 ... 2"E+00
5.885E+00
.0800
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.1182
12828.32
-1I.343E-Ol
3.11141"00
2. HS"E -02
5.871E-Ol
5.888E·Ol
.1000
1.381
1.528
812".88
-3."'7E-Ol
1.511E"00
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1.32"E-Ol
1 .38I1E-Ol
.2000
2.721
2.887
042115. 18
-5.11371-02
2.502E-Ol
2.5571-0"
8.813E-03
7.0881-03
.2500
3.401
3.587
3"75.1111
-2.78111-02
Il.1181-02
8.823E-05
1.118E-03
1.188E-03
.3000
4.082
".247
2'111.23
-1.201E-02
Il.7115E-03
1.54lE-05
1.5381 -05
3.077E-05
... 000
5.442
5.808
2210.15
7.2871-04
-5.112"E-02
7."841-08
7 ... 20E-04
7."21E-04
.8000
8.184
8.32.
l .. as.81
5.801E-03
-8.4113E-02
7.0045E-08
2.28IE-03
2.2721-03
.8000
10.885
11.050
1122.03
5.8211-03
-7.8331-02
•. 7114E-08
2.558E-03
2.585E-03
1.0000
13.808
13.771
800.32
".870E-03
-8. 7311E-02
8.211E-08
2.3581-03
2.388E-03
3.0000
.. 0 .• ,8
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302.53
2.55I1E-03
- r , 7040E -02
8.7"4E-08
4.871SE-04
4.7"5E-0"
8.0000
81.835
81.801
151.57
1. 538E -03
-5.598E·03
4.88"1-08
Il.5271 -05
1.00lE-0"
8.0000
108.847
1011.013
113.7"
1.080E-03
-2."27E-03
3.1118E-08
2."22E-05
2.7"21-05
10.0000
138.0511
138.225
111.02
7.1118E-04
-8.284E-04
2.178E-08
3.525E-08
5.704E-08
12.0000
183.271
183.438
75.88
8.1421-04
-2.1185E-05
1.550E-08
5 ....0E-OII
1.555E-08
'''.0000
1110."83
1110.1548
85.03
".1I42E-04
3.545E-04
1.170E-08
Il.035E-07
2.074E-08
18.0000
217.8115
217.880
58.111
4.113E-0"
5. 317E -04
Il.285E-07
2.375E-08
3.30lE-08
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8.877E+00
8.578E-03
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5.810E+00
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2.721
8.220
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1.585E·OO
3.1118E-03
5.812E-Ol
5.155lE-Ol
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8.18"
11 . 882
1083.15
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2.517E-Ol
8.143E-0"
2.1552E-02
2.714E-02
1.0000
13.808
17.105
72".88
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8.1I07E-02
7.028E-05
2.1130E-03
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8.117SE+00
1.737E-02
8.428E+00
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1.381
3.S85
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4.S17E+00
1.18lE-02
2.834E+00
2.84I1E+00
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2.721
4.858
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2.177E+00
7.174E-03
8.433E-Ol
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a.184
10.388
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3.08lE-Ol
1 . oallE -03
3.58U-02
3.87I1E-02
1.0000
13.8015
15.141
7.2.88
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8. 178E-02
r , 1134E-04
3.804E-03
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1.7B7E+Ol
2.418E-02
1.775E+Ol
1.777E+Ol
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8.088E+00
1.770E-02
S.S23E+00
5.541E+00
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2.721
4.288
2804.27
-2.828E-Ol
2.385E+00
7.8381-03
8.573E-Ol
8.552E-Ol
.8000
8.1'"
8.711
1278.70
-8.S21E-02
3.084E-Ol
1.112E-03
3.214E-02
3. 38U -02
1.0000
13.808
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818.18
-2.088E-02
7.83lE-02
1.783E-04
3.423E-03
3.802E-03
CD Il
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7.8248
MU·
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E (AYD)
E (EV)
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14307.80
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3.011E+Ol
1.844E-02
2.a2IE+Ol
2.823E+Ol
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.272
1.138
10888.83
-8.073E-Ol
1.808E+Ol
1 . 888E -02
1 .4881+01
t .480E+Ol
.0800
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I.U3
7357.38
-8.014E-Ol
8.824E+00
1 .15381-02
5.5871+00
S.813E+00
.2000
2.721
3.5S.
3<415.83
-2.570E-Ol
2.232E+00
8.382E-03
8.418E-Ol
5.480E-Ol
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8. 18<4
8.030
1373.03
-S.888E-02
2.S55E-Ol
7.80E-04
2.117E-02
2. 188E -02
1.0000
13.808
14.472
818.70
-1.8'37E-02
8.d3E-02
1.318E-04
2. 1841 -03
2.288E-03
1 . SOOO
20.408
21.275
582.77
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1.8721-02
1.21101 -es
2.872E-04
3.088E-04
2.0000
27.212
28.078
441.S7
-8.7321-04
1. 083E -02
7.1831-07
1.1381-04
1.1481-04
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22431.8S
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4.377E+Ol
8.4S3E-03
3.803E+Ol
3.803E+Ol
.0200
.272
.825
15031.42
-7.588E-Ol
2.3OOE+01
1.272E-02
1.5871+01
1.588E+Ol
.0800
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1.:188
80158. , •
-S.753E-Ol
8.778E+00
1.220E-02
4.701E+00
4.713E+00
.1000
1.381
1.1113
8<480.18
-4.224E-Ol
5.381E+00
8.1121-03
1.88.E+00
1.8118E+00
.2000
2.721
3.274
:1787.10
-2.242E-Ol
1.8181+00
4.431E-03
4.330E-Ol
4.374E-Ol
.11000
8.1'"
8.718
1422.47
-4.837E-02
2.045E-OI
5. 048E -04
1.30IlE-02·
1 . 3511E -02
1.0000
13.11011
14.158
875.118
-'.41i15E-02
S.01l8E-02
8.52I1E-OS
1.3221-03
1.407E-03
1.5000
20.408
20.8112
581.41
-3.833E-03
1.53lE-02
8.731E-08
1.7841-04
1.8SlE-04
2.0000
27.212
27.785
4411.S8
-8.808E-04
8.021E-03
5.831E-07
8.41SE-OS
Il.4UE-OS
CD 1 1
12F
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N·· 11.8218
MU·
.0782
E (AYD)
E (EVI
E PHOT (EV)
LAM8DA
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(L/A/L-l)
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SIGMA L-l
SiaMA L+l
SiaMA
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.0000
.000
.383
32371.40
4.8117E-02
5.882E+Ol
2.S45E-OS
4.7731+01
4.773E+Ol
.0200
.272
.855
181128. 18
-Il. 110E-Ol
2.52I1E+Ol
Il. 58'1E -03
1.50lE+Ol
I.S02E+Ol
.0800
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1 . 1111
10338.48
-5.183E-Ol
8.273E+00
8.810E-03
3.703E+00
3.712E+00
.1000
1.381
1.744
7111.31
-3.727E-Ol
4.811E+00
8.5221 -03
1 .448E+00
1.458E+00
.2000
2.721
3.104
31184.28
-1.805E-Ol
1.818E+00
3.033E-03
2.823E-Ol
2.853E-Ol
.8000
8.184
8.548
1450.73
-3. 780E -02
1.811E-Ol
3. 280E -04
8.370E-03
8.888E-03
1.0000
13.808
13.18'
888.32
-1.218E-02
4.087E-02
1.574E-OS
8.383E-04
8.8501-04
1.1000
20.408
20.712
588.32
-3.248E-03
1.218E-02
5.811E-08
1.105E-04
1.1841-04
2.0000
27.212
27.515
448.31
-7.487E-04
8.277E-03
4. 177E-07
3.804E-05
3.848E-05
CD Il
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15.8207
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4. 135E -02
8.78lE+Ol
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2.8231+01
8.838E-04
1.202E+Ol
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1.031
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7.720E+00
4. 348E -0.3
2.207E+00
2.211E+00
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1.381
1 .575
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3.718E+00
3.372E-03
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7. 847E -01
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2.721
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4223.11
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1.188E+00
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1.442E-Ol
1.4S7E-Ol
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8.184
8.:178
14711.88
-2.828E-02
1.1371-01
I.S80E-04
3.883E-03
4.048E-03
1.0000
13.808
13.821
887.11
-8.484E-03
2.7115E-02
2.88U-05
3.878E-04
4. 148E -04
1.5000
20.408
20.824
801.11
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8.2881-03
2.844E-08
5. 082E -05
S.347E-OS
2.0000
27.212
27.427
4B2.07
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4.1771-03
2.1031-07
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7.785E+00
1.341E+02
2.244E-Ol
8.857E+Ol
8.880E+Ol
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8.'22E-Ol
4.8421+01
7.088E-03
2.114E+Ol
2.115E+Ol
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2.488E+Ol
1.188E-OS
8.838E+00
8.83111+00
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-3.0531-01
8.273E+00
2.384E-03
1.347E+00
1. 350E +00
.1000
1.381
1.488
8278.21
-2.174E-Ol
2.81181+00
1.8081 -03
4.510E-Ol
4.528E-Ol
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2.721
2.888
4337.71
-1.0<43E-Ol
8.7114E-Ol
8.381E-04
7.838E-02
8.022E-02
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8.184
8.301
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8.3181-02
8.4011-05
2.08lE-03
2. 18SE -03
1.0000
13.808
13.743
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-8.222E-03
2.047E-02
1.433E-OS
2.088E-04
2.2111-04
1 .5000
20.4011
20.548
803.48
-1.883E-03
8.022E-03
1.588E-08
2.8751-05
2.832E-05
2.0000
27.212
27.341
4113.35
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3. 0211E-03
1.088E-07
8.012E-08
8.12lE-08
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13.1011
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1.237E-Ol
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3.5721-01
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18,138
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7."38E-02
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IN
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7.20110
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1.8110E+00
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13.11011
111.11115
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IN
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Il.2078
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2.078E·02
2.078E-02
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27.212
28.111111
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5.870E-02
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6. _'7E-03
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".0000
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IN III
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IN
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IN
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8347.83
5.1182'-00
-Il. 1311E+00
1.173E-Ol
2.343E-00
3.340E-00
.1000
1.381
2.021
11101.24
3.370E+00
-3.538E-00
4.82IE-Ol
1.0831-00
1.548E-00
.2000
2.721
3.310
311117.33
1.43BI+00
-1.314E+00
1.4118E-Ol
2.7110E-Ol
4.227E-Ol
.11000
8.184
8.832
1403.78
2.t22E-Ol
-2.0501-01
1.571(-02
1 . 5511E-02
3.138E-02
1.0000
13.1108
14.2711
8118.57
1.217E-01
-8.3011-02
5.0271-03
2.374E-03
7.4011-03
2.0000
27.212
27.881
444.70
3 .1I75E -02
-4.207E-03
1.228E-04
2.0117E-015
1.4315E-04
2.8000
34.011
34.884
357.48
2.888E-02
5.110E-04
5.185E-04
3.114E-07
5.18IE-04
3.0000
40.B18
41.487
218.81
1.823E-02
2.18U-03
3.2121-04
8.3311-08
3. 215E -04
3.5000
47.821
48.210
251.78
1.482E-02
2.7215E-03
2.183E-04
1.1502E-05
2.314E-04
8.0000
81.835
82.304
150.84
8.124E-03
2.5481 -03
8.48I1E-08
2.23IE-05
8.705E-05
IN
III
20P
EO' 2.tl282E-02
CAYO)
N··
17.5314
MU·
2.4888
1
IAYO)
E (EV)
1
PHOT lEV)
LAM'OA CA)
CL/R/L-l)
(L/R/L-l)
SIGMA L- 1
SlaMA L-l
SIGMA (M8)
.0000
.000
.3t18
311111.se
3.4541+01
-3.120E-Ol
Il.154E-00
2.885E+Ol
3.5801+01
.0200
.272
.871
18410.70
1.452E-Ol
- 1 .821 E +0 1
2.1811+00
7.378t+00
1.034E-Ol
.0800
.818
1 .215
10208.57
5.4001+00
-5. 83!5E +00
7.4111-01
1.733E-00
2.475E-00
.1000
1.381
1.751
7048.88
2.118E+00
-3.0841+00
3.1331-01
8. 873E -0 1
1.001E-00
.2000
2.721
3.120
31174.43
1. 121E+00
- 1.0101+00
8.284E-02
1.553E-Ol
2.37t1E-Ol
.8000
8.184
8.582
1441.11
2.Otl4E-01
-1. 473E-Ol
7.183E-03
7.784E-03
1.588E-02
1.0000
13.808
14.004
888.34
1.112E-02
-4.4471-02
2.4351-03
1.1110E-03
3.515E-03
2.0000
27.212
27.110
441.011
2.750E-02
-2.81111-03
4.373E-04
1.855E-08
4.4711-04
2.5000
34.018
34.413
380.21
1.83IE-02
3.7011-04
2.43151-04
1.175E-07
2.4371-04
3.0000
40.818
41.218
300.82
1.322E-02
1.5171 -03
1.5081-04
3.t73E-08
1.548E-04
4.0000
114.424
54.122
221.18
7.157E-03
1.1481-03
7.2711-011
8.718E-08
1.143E-05
1.0000
81.838
82.034
151. 14
4.1721-03
1.7431-03
2.IIU-05
1. 045E -08
4.03I1E-05
IN III
8D
EO· 8.7B83E-Ol
CAYO)
N··
3.2005
MU'
1.7915
1 (RYD)
E (EV)
E PHOT (EV)
LAM80A (A)
(L/R/L-l)
tL/R/L-1 )
SIGMA L-l
SIGMA L+l
SIGMA (M8)
.0000
.000
11.tI''
1037.14
3.40U-Ol
-1.428E+00
3.413E-02
1.185E-Ol
8.5141-01
.1000
1.3111
13.315
131.17
2.1201-01
-1.410E+00
2.884E-02
l.ga7l-01
1.0271+00
.2000
2.721
14.878
844.84
2.844E-Ol
-1.31181+00
2.3871-02
1.018E+00
1.042E+00
.3000
4.082
18.038
773.18
2.2481-01
-1.2851+00
2.0381-02
1.184E-Ol
1.01IE+00
1.0000
13.1108
211.580
488.07
1.2181-01
-7.1801-01
1.54IE-03
8.137E-Ol
8.233E-Ol
4.0000
84.424
88.378
188.71
4.311t1E-02
-1.782E-Ol
3.22IE-03
7.7701-02
8.0131-02
8.0000
81.835
13.510
132.48
2.tl23E-02
-7.1301-02
2.010i-Oa
2.21IE-02
2.4201-02
8.0000
108.847
120.802
102.84
2.074E-02
-3.2871-02
1.308E-03
4.8811-03
8.187E-03
10.0000
138.081
148.014
83.77
1.5581-02
-1.21181-03
1.0081-04
4.7t13E-04
1.3801 -03
Il.0000
141.885
181.820
78.71
1.3711-02
-2. 3.5E -03
7.838E-04
3.351E-05
7.171E-04
12.0000
1.83.271
1711. 228
70.78
1.21U-02
2.187E-03
8.550E-04
4.421E-05
8.1121-04
14.0000
110.483
202.437
Ill. 215
li. B781-03
8.572E-03
4 .1I83E -04
5.808E-04
1.017E-03
18.0000
217.1115
221.8411
53.11
8. lal1E-03
1.14l1E-02
3.8BOE-04
1.143E-03
1.531E-03
14
IN
III
80
EO-
5.0011E-01
(RYOI
N.·
4.2385
MU'
1.7815
E (RYO'
E (EV)
E PHOT (EVI
LAMBDA
(Al
(L/R/L-O
(L/R/L+I)
SIGMA L- 1
SIGMA
L+l
SIGMA
(M8)
.0000
.000
8.118
1818.15
5.080E-Ol
-1.183E+00
4.421E-02
3.514E-Ol
4.038E-OI
.2000
2.721
1.538
1211.18
3.1IIE-Ol
-1.321E+00
2.454 E-02
Il.278E-01
8.521E-Ol
.3000
4.082
10.818
1137.88
2.81l0E-01
-1.258E+00
1.138E-02
Il.488E-Ol
8.880E-Ol
.4000
5.442
12.251
1011. 41
2.258E-Ol
-1. 17lE+00
1.571E-02
Il. 3401 -0 1
8.4117E-Ol
.1000
10.885
17.701
700.44
1.345E-Ol
-8.38IE-Ol
8.048E-03
4.818E-Ol
4.771E-Ol
1.0000
13.808
20.422
807.11
1.100E-Ol
-7.017E-Ol
Il. 21lE -03
3.878E-Ol
3.140E-Ol
8.0000
81 .535
88.452
140.17
2.02IE-02
-5.50lE-02
9.152E-04
1.001E-02
1.10IE-02
10.0000
1311.051
142.878
88.78
1.05IE-02
-8.823E-03
4.028E-04
2. 383E -04
8. 38I1E -04
11.0000
141.185
158.481
71.23
1.275E-03
-1.107E-03
3. 384E - 04
2.148E-05
3.518E-04
12.0000
183.271
170.087
72.10
8.208E-03
1.431E-03
2.880E-04
1.313E-05
3.012E-04
18.0000
217.8115
224.511
55.23
5.443E-03
7.313E-03
1.872E-04
4.8:;I7E-04
8. 211E -04
IN
III
80
EO-
2.2175E-Ol
(RYDI
N.·
Il.2588
MU'
1.7412
E (RYOI
E 1EV)
E PHOT 1EV)
LAMBDA
lA)
IL/RIL-l)
(L/R/L+I)
SIGMA L-I
SIGMA
L+l
SIGMA
(MB)
.0000
.000
3.128
3188.30
7.708E-Ol
-8.113E-02
4.888E-02
1.31131-04
4.780E-02
.0200
.272
3.3118
3841.88
8.147E-Ol
-3.118E-Ol
4.122E-02
2.048E-02
8.188E-02
.0800
.818
3.142
3144.11
5.787E-Ol
-7.77BE-Ol
3.311E-02
8.113E-02
1.231E-Ol
.0800
1.088
4.214
21141.12
5.334E-Ol
-8.100E-Ol
3.014E-02
1.25IE-Ol
1. 580E-Ol
.2000
2.721
5.847
2120.45
3.585E-Ol
-1.100E+00
1.888E-02
2.888E-Ol
2. 8!l1E -0 1
.3000
4.082
7.208
1720.18
2.73IE-Ol
-1.058E+00
1.35IE-02
3.031E-Ol
3.188E-Ol
.4000
5.442
8.588
1447.03
2.18IE-Ol
-1.885E-Ol
1.0321-02
3.030E-Ol
3.134E-Ol
.8000
8.184
11. 210
1ott8. 24
1.510E-Ol
-7.877E-Ol
8.474E-03
2.841E-Ol
2.708E-Ol
1.0000
13.808
18.732
74·1.02
8.851E-02
-5.237E-Ol
3. 147E-03
1.730E-Ol
1. 782E -0 1
2.0000
27.212
30.338
408.81
3.708E-02
.-2.271E-Ol
1.04IE-03
5.142E-02
8.048E-02
8.0000
81. 835
84.7111
148.28
1.188E-02
-3.228E-02
2.IIIE-04
3.328E-03
3.828E-03
10.0000
138.051
131.185
81.08
8.14lE-03
-3.174E-03
1.31I1E-04
8.281E-05
2. 148E-04
11.0000
1411.885
152.7111
81.15
5.357E-03
-1.238E-03
1.1021-04
8.7114E-08
1.1110E-04
12.0000
183.271
188.3117
74.51
4.723E-03
1I.1I411E-04
Il.32I1E-05
3.030E-08
8.832E-05
18.0000
217.8115
220.821
58.15
3.01lIlE-03
4.113E-03
5.32I1E-08
1.408E-04
1.841 E -04
IN III
100
EO-
1.3175E-Ol
(RYO)
N.·
8.2851
MU'
1.73411
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA
lA)
(L/R/L-Il
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA
(M8)
.0000
.000
1 .7113
81118.78
9.042E-Ol
1.854E+00
3.884E-02
1.84I1E-Ol
2.218E-Ol
.0200
.272
2.088
8005.18
7.727E-Ol
7.218E-Ol
3. OIlIlE - 02
4.053E-02
7.1821-92
.0400
.544
2.337
5305.88
Il.74BE-Ol
1.44I1E-Ol
2.875E-02
1 .851 E- 03
2.880E-02
.0500
.880
2.473
5013.12
Il.345E-0~
-5.1142E-02
2.502E-02
3.2111E-04
2.535E-02
.0800
.8111
2.8011
4152.44
5.1185E-Ol
-2.240E-Ol
2.34I1E-02
4.93.04E-03
2.843E-02
.1000
1.3151
3.153
31132. tel
4.885E-Ol
-8.244E-Ol
1.8715E-02
4.15381-02
Il.512E-02
.2000
2.721
4.514
27411.87
3.251E-Ol
-8.8031-01
1.II1I1E-02
1.31I1E-Ol
1.43I1E-Ol
.3000
4.082
5.874
2110.155
2.382E-Ol
-8.508E-Ol
8.380E-03
1.1502E-Ol
I.B815E-Ol
.4000
5.442
7.238
1713.72
1.842E-Ol
-7.88I1E-Ol
8.173E-03
1.'813E-Ol
1.1l74E-Ol
.5000
Il.803
8.51115
1442.415
1.47'7E-Ol
-6.8381-01
4.718E-03
1.515E-Ol
1.583E-Ol
1.0000
13.1508
15.3118
805. 111
II. 808E - 02
-3.880E-Ol
1.8110E-03
8.740E-02
8.1I0IlE-02
2.0000
27.212
211.004
427.47
2.833E-02
-1.1l13E-Ol
5.058E-04
2.841E-02
2.817E-02
15.0000
81. 835
83.428
148.81
7.IISIIE-03
-2. 188E-02
1.32I1E-04
1.47U-03
1 .1511 E -03
10.0000
138.0511
137.852
811.114
4.112E-03
-2.15115E-03
5.880E-05
3.774E-05
Il.1534E-05
11.0000
1411.68a
151. 458
81.88
3.5831-03
-8.587E-04
4.8871-05
4.21lE-01l
5. 308E -05
12.0000
1153.271
188.084
75.11
a.1541-03
4.328E-04
4. 1211E-05
1.18Ie-08
4.245E-05
115.0000
217.1115
2111.487
811.411
2.0151E-03
2.712E-03
2. 343E -05
8.08SE-08
8.42I1E-05
20.0000
272.118
273.1111
45.27
1.474E-03
3. 12lE -03
1.4118E-015
1.008E-04
1.151E-04
IN
III
120
EO-
8.5384E-02
(AYO)
N·· 10.21580
MU-
1.7320
E (RYO)
E ( EV)
E PHOT (EV)
LAM8DA (Al
(L/R/L-l)
(L/R/L+I)
SIGMA L- 1
SIGMA L+l
SIGMA
(M81
.0000
.000
1.181
1015'75.14
9.02U-Ol
3.111141+00
2.3715E-02
15.1188E-Ol
7.224E-Ol
.0400
.S44
1.708
721511.00
8.333E-Ol
8.38IE-Ol
1. 71 liE -02
4.50llE-02
II. 224E-02
.0800
.s ie
1.1178
U88.811
5. S17E -0 1
2.213E-Ol
1.1513E-02
3.852E-03
1.878E-02
.0800
1.088
2.250
5S10.811
4.87111-01
-1.41531-01
1 . 34lSE -02
1.818E-03
1.828E-02
.1000
1.381
2.522
41118. 11
4.38SE-Ol
-3.7301-01
1.20U-02
1.32U-02
2.531E-02
.2000
2.121
3.883
31113.38
2.7111E-Ol
-7.0831-01
7. 1502E -03
7.343E-02
8.1041-02
.3000
4.082
5.243
2384.70
1 .1I110E -0 1
-15.8721-01
5.2I1E-03
Il.338E-02
1. 8!l7E -02
.4000
5.442
15.1504
11577.ll0
l.llI0E-Ol
-8. 14!l1-01
3.788E-03
Il.4011-02
Il. 780E - 02
.5000
8.803
7.11154
Isse. 78
1.II1.04E-Ol
-5.4015E-Ol
2. 8!l41 -03
8.777E-02
Il.0153E-02
1.0000
13.1508
14.787
831.150
5.1401-02
-2.1172E-Ol
Il.808E-04
4.1I1I1E-02
5.017E-02
2.0000
27.212
28.373
438.118
1.I715E-02
- 1 .207E-Ol
2.78BE-04
1. aSilE -02
1.587E-02
15.0000
81.l535
82.7117
141.75
5.7112E-03
-1. 580E-02
8.11811-05
7.7117E-04
8.4118E-04
10.0000
138. OU
137.221
110.38
2.111141-03
- 1.11721 - 03
3.0112E-08
2.012E-0!l
5.104E-05
11.0000
I d . 15155
180.827
82.20
2.1507E-03
-15.3S'7E-04
2.578E-05
2.2I8E-08
2.8015E-05
12.0000
163.271
1154.432
75.40
2.2113E-03
3.037E-04
2. 173E-05
5.720E-07
2.230E-05
18.0000
217.15115
218.n15
515.155
1.4115E-03
1.IISII-03
1. 230E -05
3. 1I8E -05
4.318E-05
20.0000
272.118
273.280
45.37
1.08I1E-03
2.2S15E-03
7.850E-015
5.24SE-05
15.030E-05
HI
IN III
USD
EO· 4.41115E-02
(RYOl
Ne.
14.2704
MU·
1 . 7211lS
E (AYO)
E (IV)
E PHOT (EV)
LAMBDA (A)
(L/R/L-l)
(L/R/L+l)
SlaMA L- 1
SlaMA L+l
SIaMA (MI)
.0000
.000
.lSOI
20lS111.44
4.741E-Ol
1. 037E+0 1
3. 3117E -03
2.438E+00
2.4421+00
.0200
.272
.873
141115.40
4.1151E-Ol
4.01IE+00
1.382E-03
1.415E-Ol
lI. 4lSIIE -0 1
.0lSOO
.81lS
1. 418
8741.83
4.0lS4E-Ol
7.23l!1E-Ol
1.884E-03
2.711I1E-02
3.387E-02
.0700
.1182
1 . 554
71171. Ils
3.83lSE-Ol
4.1lS7E-Ol
5.748E-03
1.017E-02
1.5112E-02
.0800
1.088
l.lSlO
7337.42
3.lS18E-Ol
1.1118E-Ol
1.5lS1E-03
2.345E-03
7.1I05E-03
.01100
1.225
1 .8U
lS7110. lS4
3.418E-Ol
2.438E-02
1.3lS2E-03
4. OIl2E-01
5.403E-03
.1000
1.3lS1
1.112
lS3111.71
3.233E-Ol
-1.018E-Ol
5. 114E -03
7.lS73E-04
5.1122E-03
.2000
2.721
3.322
3731.73
2. 007E-0 1
-4.8171-01
3.3lS3E-03
2.1I07E-02
3.243E-02
.3000
4.082
4.U3
2lS47.14
1.3114E-01
-4.lSI4E-Ol
2.288E-03
3.8110E-02
4.11IE-02
.4000
5.442
8.044
2051.51
1.03I1E-Ol
-4.142E-Ol
1.838E-03
3.1I0IlE-02
4.073E-02
.5000
8.803
7.404
IlS74.53
8.01lIlE-02
-3.51I1E-Ol
1. 221 E-03
3.lS17E-02
3.73IE-02
.lS.OOO
8.1lS4
8.781
1414.58
lS.527E-02
-3.135E-Ol
Il.38lSE-04
3.24I1E-02
3. 342E -02
1.0000
13.lS08
14.207
872.70
3.3lS0l-02
-1.1I1eE-Ol
4.03lE-04
1 .lIlSlSE -02
2. OOlSE -02
2.0000
27.212
27.813
4415.78
1.24I1E-02
-7.80IlE-02
1.011 E-04
8.071E-03
8.180E-03
lS.OOOO
81 .835
82.237
150.77
3.55I1E-03
-1.732E-03
2.81I1E-05
2.1137E-04
3.IIIIE-04
10.0000
138.0811
138.880
00.73
1.84lSE-03
- 1 .2281-03
1.171 E-05
7. 775E-OlS
1.1148E-05
11.0000
1411.lSlS5
150.2lSlS
82.51
1.805E-03
-4.00lE-04
1.725E-08
I.OlS81-07
1.0lSU-OS
12.0000
183.271
IlS3.872
75.lSlS
1.418E-03
1.812E-04
8.284E-08
2.02IE-07
8.487E-OlS
IlS.0000
217.515
218.21lS
lIlS.80
1.154E-04
1.1I4E-03
4.511IE-OlS
1 . 174E -05
l.lS33E-05
IN III
200
EO· 2. l!II511E -02 (RYO)
N··
18.2714
MU·
1.721lS
E (RYO)
E (IV)
E PHOT (IV)
LAHOA CA)
(L/R/L-l)
(L/R/L+ 1 )
SIGMA L- 1
SlaMA L+l
SIGMA (MlS)
.0000
.000
.387
33802.44
-5.332E-Ol
1.8110E+Ol
2.lS21E-03
4 .1I40E +00
4.1143E+00
.0050
.OlS8
.435
28113.17
-2.087E-OI
1.317E+OI
4,782'E-04
2.842E+00
2.842E+00
.0100
.13lS
.103
24lSllS.42
-1.41181-02
Il.5l!12E+00
2.8381-0lS
1.734E+00
1.7341+00
.0200
.272
.lS311
11405.75
1.713E-Ol
5.47IE+00
5. 180E-04
7.231&-01
7.2371-01
.0lSOO
.81lS
1.113
10471.32
2.847E-Ol
8.780E-OI
2.410E-03
3.43l1E-02
3.880E-02
.0700
.lI82
1.3111
113'8.82
2.752E-Ol
5.38lSE-Ol
2.511 1 -03
1.4431-02
l.lSl4l-02
.0800
1.088
1.4l15
8511.81
2.lS3lSE-Ol
3.003E-Ol
2.542E-03
4.lI481-03
7.4I1E-03
.oeoo
1 .2211
1. III 1
7711 .37
2.513E-Ol
1.2110E-Ol
2.5271-03
1.l7l1E -04
3.525E-03
.1000
1.381
1.727
7177.87
2.311E-Ol
3.805E-03
2.482E-03
8.4lS21-07
2.483E-03
.2000
2.721
3. a.8
4011.13
1.4881-01
-3.4,.. E-Ol
1.7111-03
1.422E-02
1 .III4E -02
.3000
4.082
".441
2787.10
1.022E-Ol
-3.412E-Ol
1.leH-03
1.152E-02
2.00E-02
.4000
5 ..... 2
5.10'
2134.32
7.551E-02
-2.118IE-Ol
8.32.1-04
1.157E-02
2.0"OE-02
.5000
lS.803
7.170
172l1.30
5.855E-02
-2.583E-Ol
8.177E-04
1.804E-02
1. 8lS5E -02
1.0000
13.808
13.173
887.35
2.310E-02
-1.353E-Ol
2, 008E -0"
1.15lE-03
1.851E-03
2.0000
27.212
27.5711
"41.57
8.758E-03
-1.324E-02
5.3171-05
2 .1..8E -03
3.00tE-03
lS.OOOO
81.835
82.002
151.20
2 ....llE-03
-lS.752E-03
1 .258l-05
1.410E-0"
1.535E-0"
10.0000
13lS.0111
138 ... 2.
10.88
1. 271 E-03
-8.4"4E-04
5.542E-08
3. 888E -OlS
1. 20llE -08
11.0000
'''1.885
150.032
12.8"
1.100E-03
-2.73lE-0"
".583E-08
4.218E-07
4. 185E -OlS
tN 111
4F
EO· 5.1828E-Ol
(RYO)
N··
3.8785
MU·
. 1211
E (RYOI
E IIV)
E PHOT (IV)
LA.1I0A CA)
(L/R/L-l)
(L/R/L-l )
SIGMA L-1
StGMA L-l
SIGMA (U)
.0000
.000
8.140
1523.14
-5.213E-Ol
3.2821+00
5.1571-02
3.11lE+00
3.1701+00
2.0000
27.212
35.312
350.72
-1.7821-02
1.018E-Ol
2.IS8E-0"
1 .31IE-02
1.345E-02
".0000
5".424
lS2.5."
118.18
-".7131-03
3.5801-02
3.7421-05
2.8801-03
2. lI17E - 03
8.0000
81.835
8l1.778
138.11
-2.4041-03
1.7231-02
1.31171-05
1.5721-04
lI.7121-0"
8.0000
108.147
118.187
105.18
- 1.2131 -03
1.7181-03
... U.E-OlS
3.1851-04
4.011E-04
12.0000
183.271
171 .411
72.33
-2.llI5E-0"
4.4501-03-
4. '''H -07
1 .2111-04
. '1.2231-04
'''.0000
110.483
1I8.lS23
lS2.42
- 1.43111-0"
3.3"51-03
1.10lE-07
7.1821-05
7 .lI13E -05
18.0000
217.lS15
225.838
54.10
-5.8I1E-0!I
2.lS17I-03
2.111E-08
5.55el-05
5.55IE-05
18.0000
24" .Ioe
253.0.. 7
41.00
-1.278E-05
2.101E-03
1.1131-01
4.0311-05
4.03IE-05
20.0000
272.118
280.258
..... 24
1.28IE-OII
1.735E-03
1.25U-01
3.028E-05
3.0281-05
IN t 1 1
IF
EO· 3.11131-01
(RYOI
N··
4.111"
MU·
. 140lS
1 (AYD)
1 IIV)
E PH01' (EV)
LAMeOA (Al
(L/Il/L-l)
IL/R/l+l)
SIGMA L-1
SIGMA L+l
SIGMA (MI)
.0000
.000
Il.11lS
2310. li"
-1.155E+00
5.7Il1l-00
1.8841-01
8.2"'1+00
8.427E+00
.11000
lS.803
11.1181
1034.20
-2.5231-01
1.0221+00
2.0551-02
4.4l171-01
".703E-Ol
1 .0000
13.808
18.712
lS51.80
-1.83"1-02
3.5101-01
... lSl7l-03
8.0111-02
li. 1881-02
2.0000
27.212
32.317
312.70
-2.32111-02
1.0321-01
4.7171-04
1 .23111 -02
1.28eE-02
".0000
54.424
1I1.loe
201.00
-4.5101 -03
3.3lSlIt-02
3.2lS51-08
2.4301-03
2.482E-03
8.0000
81.835
88.821
'''2.11
-2.1131-03
1.8531-02
1.1251-08
8.523&-04
8.83IE-04
8.0000
101 .•47
114.033
108.73
-1.I"lIl-03
1.3111-03
4.05IE-08
3.5501-04
3.511 E-04
12 .0000
183.271
111•. 457
73 .•0
-2 .... 01-04
4.2051-03
3.lSIOI-07
1.0701-0"
1.0731-04
14.0000
110."83
1111.8U
83.37
-1.345E-04
3.1131-03
1.52111-0.
8.118"1-05
8.11131-05
1•. 0000
217.lS15
222.180
55.lS3
-5.503E-05
2.4821-03
1.8181-01
4.81101-05
4.8521-05
18.0000
2.. 4.IOlS
250.0112
41.58
-1.1381-05
1.lI7111-03
8.7211-10
3.5181-05
3.5181-05
20.0000
272.118
277.304
..... 71
1.21131-05
1.8271-03
1.2"81-011
2.8371 -05
2.11371 -05
IN III
8F
la· 2.lS2115E-Ol
IRYO)
N··
5.8l104
MU·
. 14l1lS
E IRYO)
1 IIV)
1 PHOT IIV)
LAMBDA lA)
(L/R/L-l)
IL/R/L+l)
SIGMA L-l
SIGMA L+l
SIGMA
(M5l
.0000
.000
3.578
34lS5.111
-1.lllSl+OO
8.287E+00
3.5381-01
8.7711+00
1.1331·00
.5000
8.803
10.381
1114.40
-2.11131-01
1.0811+00
2.3721-02
4.4141-01
".85tE-Ol
1 .0000
13.808
17.184
721.54
-1.0331-01
3.5411-01
4.1421 -03
7. 75U -02
•. 2471-02
2.0000
27.212
30.788
402.81
-2.3841-02
1.34I1E-02
4.7121-04
1.8541 -03
1.0131-02
4.0000
54.424
5•. 001
213.7.
-4. OOlSl -03
2.8841-02
2.50lSl-05
1.7321-03
1.7571 -03
8.0000
81.835
15.213
145.50
-1.841 E-03
1.4271-02
7.7741-011
lS.22111-0"
lS.307E-04
10.0000
1311.05l1
13l1.lS37
88.711
-4.1741-0"
5.1341 -03
1.3031-07
1.3221-0"
1.33tE-04
12.0000
1113.271
18lS.841
74.31
-2.4431-04
3.lS01E-03
2.1183E-07
7.7IeE-05
7.8251-05
14.0000
110.483
1I4.0lS0
lS3.811
-1.14116-04
2.7001-03
lS.81171-08
5.0101-05
5.0871-05
IlS.OOOO
217.811S
221.272
5lS.03
-4.lSlIll-05
2.1071-03
1 . 2l13E -08
3.527E-05
3.528E-05
18.0000
24".IOlS
2"8.484
4l1.lIO
-li. "lS7E -OlS
1 . lSlIl1 - 03
5.lIIH-l0
2.5511-05
2. 55 tE -05
20.0000
272.118
275.lSlIlS
..... lI7
1.128E-05
1.3l101-03
Il.4501-10
1.11121-05
1.11121-05
18
IN III
8F
EOa 1.4834E-Ol
CAYO>
N'"
7.8421
MU'
· 11I71i1
(AYO)
E (IV)
E PHOT (EV)
LAMIIOA
lA)
lL/R/L-11
(L/R/L+I)
SIGMA L- 1
SIGMA L+ 1
SIGMA (M81
.0000
.000
1.IUll
11221!.811
-3.71i10E+00
1.33Ii1E+Ol
7.704E-Ol
1.282E+Ol
1.3118E+OI
.2000
2.721
".712
2831.10
-8.811I1E-Ol
3.22I1E+00
9.1i11I3E-02
1.781E+00
1.88IE+00
.4000
5.442
7.434
1887.U
-3.1i151E-Ol
1.31i10E+00
3.125E-02
5. l111i1E -0 1
5.47IE-OI
.8000
10.8S1
12.8711
1i182.1i13
-1.384E-OI
4.524E-Ol
Il.848E-03
9.482E-02
1.013E-Ol
1.0000
13.808
15.587
71i14.1i13
-1iI.21i10E-02
2.1i188E-Ol
3.1125E-03
4.8331-02
5.28I1E-02
2.0000
27.212
21i1.203
424.57
-2.037E-02
7.171E-02
3.284E-04
5.31i12E-03
5.718E-03
4.0000
114.424
511.415
211i1.78
-3.038E-03
2.073E-02
1.403E-05
8.701E-04
8.848E-04
8.0000
81.835
83.827
148.211
-1.300E-03
1.0321-02
3.804E-06
3.11i17E-04
3.23I1E-04
10.0000
138.058
138.0eo
88.81
-3.51i12E-04
3.70IilE-03
4.71i18E-07
Il.81Ii1E-05
Il.887E-05
14.0000
lIiI0.483
182.474
114.42
-8.213E-05
1 .1iI40E-03
3.41i17E-08
2.800E-05
2.804E-05
18.0000
217.885
21'.888
118.44
-3.223E-05
1 . 512E -03
Il.144E-Olil
1.803E-05
1.804E-05
18.0000
244.IiIOII
2411.81i18
50.22
-5.021E-OII
1.214E-03
1.878E-l0
1. 30llE -05
1. 308E -05
20.0000
272.118
274.101i1
45.23
8.873E-08
1iI.1iI80E-04
5.5114E-l0
'.785E-08
iii. 7811E-08
III III
lOF
EO' iii. 2880E-02
(AYOI
N'"
Il.8384
MU'
· 18111
E (AYO)
E (EV)
E PHOT (EV)
LAM80A tA)
lL/R/L-1 )
(L/R/L+I)
SIGMA L- 1
SIGMA L+ 1
SIGMA (M51
.0000
.000
1.2811
1i1800.85
-8.01i18E+00
1 . 81i14E +0 1
1.288E+00
1.828E+OI
1.758E+Ol
.1000
1.381
2.828
4722.08
-1.811E+00
15.105E+00
2.320E-Ol
3.514E+00
3.74I1E+00
.2000
2.721
3.888
3110.34
-8.1iI08E-Ol
3.050E+00
8.51Ii1E-02
1.332E+00
1.417E+00
.4000
5.442
15.707
1848.41i1
-3.588E-Ol
1.202E+00
2.3011-02
3.482E-Ol
3.712E-OI
.8000
8.1114
Il.428
1315.00
-1.1iI04E-Ol
15.213E-Ol
Il.202E-03
1.307E-Ol
1.388E-Ol
.8000
10.8815
12.150
1020.48
-1.183E-Ol
3.885E-Ol
4.42IE-03
5.1i125E-02
8.3I1IE-02
1.0000
13.1108
14.871
833.75
-7.1588E-02
2.383E-Ol
2.387E-03
3.034E-02
3.270E-02
2.0000
27.212
28.477
435.311
-1.842E-02
5.528E-02
2.088E-04
3.128E-03
3.332E-03
4.0000
54.424
55.1I111i1
222.114
-2.341E-03
1.1147E-02
8.217E-08
4. 785E-04
4. 887E -04
Il.0000
81.8315
82.1iI01
140.58
-1iI.822E-04
7.710E-03
2.087E-08
1.711Ii1E-04
1 . 780E -04
8.0000
108.847
110.112
112.110
-5.19I1E-04
4.387E-03
8.004E-07
7.541E-OII
7.821E-OII
10.0000
138.0elil
137.324
80.2'
-2.1577E-04
2.7721-03
2.8110E-07
3.788E-05
3.818E-OII
12.0000
183.271
1114.1138
75.38
-1.320E-04
1 .1iI38E-03
7.723E-08
2.21Ii1E-05
2.227E-OII
14.0000
l1i10.483
1iii 1 .748
84.lle
-8.11Ii1E-05
1.44Ii1E-03
1.1i133E-08
1.447E-OII
1 . 448E -011
111.0000
217.11811
218.880
1111.113
-2.343E-05
1.124E-03
3.238E-OII
Il.1i132E-01I
1iI.1iI38E-08
18.0000
244.808
248.172
50.37
-5.338E-015
Il.038E-04
1. 8llli11- 10
7.221E-OII
7.22lE-08
20.0000
272.118
273.383
411.311
15.142E-08
7.387E-0"
2.778E.-IO
5.357E-015
Il.3117E-08
IN III
12F
EO'
8. 4231i1E-02
(RYOI
N"·
11.8385
MU'
· 18311
E (RYOI
E (EV)
E PHOT lEV)
LAIIIIO"
lAI
lL/R/L-I)
IL/A/L+I)
SIGMA L- 1
SIGMA L+I
SIGM"
(Mil)
.0000
.000
.874
141811 .112
-8.711IE+00
2.41i18E+Ol
1.81Ii1E+00
1 .liIllIiIE+O 1
2.141E+OI
.01100
.1180
1.5114
71i178.815
-3.40IlE+00
1.052E+Ol
".8112E-Ol
15.182E+00
8.887E+00
.2000
2.721
3.51i15
3448.155
-8.310E-Ol
2. 7411E+00
15.887E-02
iii. 7211E-Ol
1.038E+00
.4000
Il.442
15.318
lIiI82.1i13
-3.01i17E-Ol
1.018E+00
1.83IE-02
2.3501-01
2.513E-Ol
.8000
8.184
Il.038
1371.110
- 1 . 804E -0 1
5.13I1E-Ol
8.280E-03
8.558E-02
1iI.184E-02
1.0000
13.808
14.480
8515.215
-15.321E-02
1.1iI2Ii1E-Ol
1.115eE-03
1.1i134E-02
2.080E-02
2.0000
27.212
28.0815
441.45
-1.32Ii1E-02
4.372E':02
1.338E-0"
1.1i128E-03
2.0112E-03
4.0000
114.424
55.288
224.22
-1.847E-03
1.202E-02
5.080E-08
2. 887E -04
2.1i118E-04
8.0000
108.847
101il.721
113.00
-4.033E-04
3.31i18E-03
".807E-07
4.1150E-05
4.1I1i18E-05
12.0000
183.271
111".145
75.53
-1.01IilE-04
I.II08E-03
4.1188E-08
1. 338E -05
1 .341 E-05
14.0000
l1i10.483
lIi11.3117
114.71i1
-4.7121-011
1 . 12IE-03
1.144E-08
8.840E-05
8.852E-08
18.0000
217.8811
218.B81i1
511.73
- 1 .1iI1iI1 E-011
8. 745E -04
2.332E-OII
8.003E-08
8.005E-08
18.0000
244.808
245.780
110.45
-3.444E-08
7.001E-0"
7.853E-l1
4.3341-08
4.33.E-08
20.0000
272.118
272.882
411.42
4.7781-08
5.7771-0..
1.877E-IO
3.271E-08
3.272E-08
IN !JI
18F
EO'
3.11885E-02 (AYO)
N'"
15.8348
MU'
· 18114
E (AYO)
E (EV)
E PHOT
(EV)
LAMIOA (Al
U/RIL-I)
(L/A/L+I)
SIGMA L-I
SIGMA L+I
SIGMA (Mil)
.0000
.000
.488
211387.211
-1.112I1E+Ol
3.8811+01
3.0117E+00
2.814E+Ol
2.liIlliIl+01
.0400
.1144
1.033
12007.00
- ... 474E+00
1. 271E+OI
5.1188E-Ol
5.1i11I8E+00
8.5451+00
.2000
2.721
3.210
3883.03
-15.722E-Ol
2.137E+00
3.eOSl-02
5.283E-Ol
5.854E-OI
.4000
5.442
5.1i131
201il0.57
-2.301E-01
7.37I1E-Ol
8.41I1E-03
1.118E-Ol
1.243E-OI
.11000
8.1114
8.852
1433.011
-1.153E-OI
3.822E-OI
3.100E-03
4.077E-02
4.387E-02
1.0000
13.808
14.084
878.81i1
-4.428E-02
1.330E-Ol
7.442(-04
8.liIllIiIE-03
1iI.703E-03
2.0000
27.212
27.700
447.80
-8. 11581 -03
2.840E-02
15.2581-011
8.853E-04
iii. 278E-04
4.0000
54.424
54.1i112
225. 7iii
-1.24I1E-03
7.liIllIiIE-03
2.207E-08
1 . 241i1E -04
1.2721-04
Il.0000
81.835
82.124
1110.17
-4.890E-04
3.1i188E-03
5.2881-07
4. 83Ii1E-OII
4.81i12E-01I
10.0000
138.011i1
1311.1148
80.80
-1.311I1E-04
1.4271-03
8.714E-08
1iI.187E-08
1. 005E -05
14.0000
180.483
l1iI0.1iI71
84.1i12
-3.02lE-OII
7.415E-04
4.81i1IE-01iI
3.77IE-08
3.775E-08
111.0000
217.1185
218.183
158.83
-1. l1i12E-05
Il.7801-04
8.35IE-IO
2.818E-08
2.818E-08
18.0000
244.1iI08
2411.315
150.53
-2.0441-08
4.8221-04
2.781E-Il
1. 883E-08
1.883E-08
20.0000
272.118
272.807
48.48
4.8881-08
3.8081-04
1.738E-l0
1.420E-08
1.420E-08
IN III
20F
EO'
2. 2871i1E-02
(AYO)
N'"
lli1.8337
MU'
.1883
E ( RYO)
E (EV)
E PHOT (EV)
LAM80A (A)
lL/A/L-1)
(L/A/L+I)
SIGMA L-l
SIGMA L+I
SIGMA (M5)
.0000
.000
.311
38830.05
-2.300E+OI
Il.42I1E+Ol
4.438E+00
3.210&:+01
3.733E+OI
.0200
.2'T2
.1183
212112.12
-8.283E+OO
2.144E+Ol
1 .073E+00
iii. 830E+00
l. 070E+OI
.0400
.1544
.8511
14482.43
-4.420E+00
1.20IilE+OI
4.1I01E-OI
4.41i101+00
4.1i140E+00
.1000
1. :Ill 1
1.572
7415.1i18
-1. 4112E+00
4.33I1E+00
1.. 811i1E-02
1.128E+00
1 .22I1E+00
.2000
2.721
3.032
4088.112
-5.358E-Ol
1.872E+00
2.3431-02
3.044E-OI
3.27li1E-01
.4000
5.442
5.7114
21114.11
-1.754E-OI
Il.555E-OI
4.785E-03
8.375E-02
8.SllE-02
.8000
10.885
11.188
1107.41
-1I.018E-02
1.544E-OI
7.778E-04
Il. 887E - 03
1.03I1E-02
1.0000
13.808
13.1i117
880.81i1
-3.27Ii1E-02
iii. 782E-02
4.02Ii1E-04
4.782E-03
5.185E-03
2.0000
27.212
27.123
4110.48
-8.115U-03
2.144E-02
3.280E-OII
4.1141E-0"
4.888E-04
4.0000
114.424
54.7311
228.52
-1iI.278E-04
Il.77l1E-03
1.28Ii1E-OII
8.!l1l4E-05
Il. 88 IE-OII
8.0000
81.835
81.1i147
1!l1.30
-3.823E-04
2.888E-03
2.8871-07
2.4111E-05
2.480E-OII
10.0000
'38.0elil
1311.370
1iI0.1iI2
-iii. 710E-OII
1.0111&:-03
3.483E-08
5. 487E -011
Il.522E-08
14.0000
180.483
180.71i14
84.1i18
-3.31i17E-01I
Il. 220E-04
5.U8E-Olil
1.887E-OII
1.872E-08
18.0000
217.1I1i111
218.0011
111.87
-iii. 24I1E-OII
4.258E-04
5.0IeE-l0
1.41Ii1E-08
1.420E-015
18.0000
244.808
245.218
110.118
7.883E-08
3.2881-04
4.083E-l0
1iI.!l0IilE-07
1iI.513E-07
20.0000
272.118
272.430
411.51
1.03I1E-05
2.81i14E-04
7.88I1E-IO
8.11i14E-07
8.20IE-07
17
SN IV
55
EO' 2.8373E+00 CAYO)
N••
2.3747
MU'
2. 11253
E (AYD)
E (EV)
E PHOT (EV)
LAMIlDA
(Al
(L/A/L-O
(L/A/L+I)
SIOMA L·l
SfaMA
L+l
SIOMA (MS)
.0000
.000
38.104
321.18
.000
2.408E-Ol
.000
1. 40lE -01
1.40IE-Ol
1.0000
13.101
52.210
237.41l
.000
1.1l32E-Ol
.000
1.102E-Ol
1.102E-Ol
2.0000
27.212
15.815
188.38
.000
1.437E-Ol
.000
8.537E-02
8.537E-02
8.0000
10 •. 8~7
1~7.~51
84.08
.000
5. 1l07E -02
.000
2.813E-02
2.813E-02
20.0000
272.118
310.722
38.110
.000
2.247E-02
.000
8.855E-03
8.81151-03
SN IV
15
10' 1.3881E+00 IAYD)
N.'
3.4188
MU'
2.5802
E IAYD)
E lEV)
E PHOT lEV)
LAMIDA (A)
(L/A/L-l)
IL/A/L+1 )
SIOMA L- 1
SIOMA L+l
SIOMA (Mil)
.0000
.000
18.815
111.07
.000
4.07IE-Ol
.000
1.844E-0'
1. 8.4E -0 1
1.0000
13.808
32.221
3 ••.• 0
.000
2.2~I-01
.000
1.0381-01
1.0:18E-Ol
2.0000
27.212
~1l.827
270.51
.000
1.4731-01
.000
1.2.4E-02
1.244E-02
10.0000
131.058
154.874
80. 18
.000
3.100E-02
.000
8. 341E -03
8.341E-03
18.0000
2.~.801
283.521
47.01l
.000
1. 578E -02
.000
4. 111 E -03
4.111E-03
SN IV
85
10' 5.401IE-Ol
(RYD)
N··
5.4400
MU'
2.5500
E (AYD)
E (EV)
E PHOT (EV)
LAMIOA (A)
(L/A/L-l)
(L/A/L+I)
SIOMA L- 1
SlOMA L+l
SIQMA (MS)
.0000
.000
7.31l1
1881l.41
.000
8.18lE-Ol
.000
3.08.e-Ol
3.084E-Ol
1.0000
13.101
20.882
581.48
.000
2.32.3E-Ol
.000
7.1011-02
7.10IE-02
4.0000
54.424
81.7.0
200.18
.000
5.370E-02
.000
1.1201-02
1. 120E-02
1.0000
81.135
88.lIt2
138.32
.000
3.273E-02
.000
Il.890E-03
5.880E-03
SN IV
105
10' 2. 8811E-0 1 IAYD)
N.'
7 .• 4117
MU'
2.55.3
E (AYD)
E (EV)
E PHOT (EV)
LAMIlOA
~ A )
(L/A/L-Il
(L/A/L + 1 )
SIOMA L-l
SIQMA L·'
SIQMA (MI)
.0000
.000
3.827
31117.44
.000
1. 30lE +00
.000
4.2081-01
4.2"E-Ol
.5000
1.803
'0.730
11511.5.
.000
3 .• ,91-01
.000
8.832E-02
8.8321-02
1.0000
13.101
17 .533
707.17
.000
1.872E-Ol
.000
4.2.d-02
4.2 •• E-02
•. 0000
~ .• 24
58.310
212.48
.000
3.7031-02
.000
5. 028E -03
5.028E-03
SN IV
125
10.
1.78241-01
(AYD)
N.·
Il.4481
IIIU'
2.11518
E (AYD)
E IIVI
1 PMOT
lEV)
LAQOA
(A)
IL/A/L-Il
(L/A/L+')
SIGMA L-l
SIGMA L+l
SIOMA (MI)
.0000
.000
2 .• 38
508•. 13
.000
1.8~1+00
.000
5.322E-Ol
5.322E-Ol
.4000
5.442
7.811
1ll73.22
.000
4 . .213E-Ol
.000
8.0021-02
8.0021-02
.8000
10.885
13.323
1130.58
..000
2.0821-01
.000
3.13lE-02
3.13lE-02
1.0000
13.101
11.045
772.71
.000
1.8081-01
.000
2.8101-02
2.1101-02
2.0000
27.212
28.851
.18.18
.000
1.78.1-02
.000
8.5841-03
8.584E-03
4.0000
5 •. 424
51 .•12
218.05
.000
2.7101-02
.000
2.825E-03
2.825E-03
.
SN IV
Ils
10' 8 .•~.41!-02 (nO)
N••
13.4501
MU'
2.5488
E (AYD)
E (EV 1
E PHOT (IV)
LAMIOA (Al
(L/A/L-l)
(L/A/L+ Il
SIGMA L-l
SlaMA L·l
SIQMA (MI)
.0000
.000
1.203
10303.33
.000
3. 1721.00
.000
7.1071-01
7.1071-01
.1000
1.381
2.514
.'35.75
.000
1.2181+00
.000
2.39d-Ol
2.384E-Ol
.4000
5.442
I.~I
".5.15
. 000
3.3481-01
.000
4.885E-02
4.81111-02
1.0000
13.101
14 .•09
837.22
.000
1. 0881-01
.000
1.lo.E-02
1. 10~1-02
2.0000
27.212
28 .• 15
431.3.
.000
4.3091-02
.000
3.3181 -03
3.3181 -03
SN IV
205
EO' 5.2538E-02
(AYD)
N••
17.4508
MU'
2.5481
E (AYD)
E (EV)
E PMOT
lEV)
LAMIDA (Al
(L/A/L-l )
(L/A/L·11
SIGMA L-l
SIQMA L·l
SIQMA (MI)
.0000
.000
.715
1734•. 47
.000
4.720E+00
.000
1.001E+00
1.0011+00
.0500
.880
1.385
8187.00
.000
1.8801+00
.000
3.4721-01
3 .• 72E-0 1
.2000
2.721
3 .• 38
310•. 42
.000
5.8281 -0 1
.000
7.328E-02
7.328E-02
.1000
8. 184
8.878
1381.48
.000
1.5411-01
.000
1.325E-02
1.325E-02
.8000
10.885
11.100
1018.88
.000
1.015E-Ol
.000
8.113E-03
8.113E-03
1.0000
13.101
14.321
81!! . 78
.000
7.815E-02
.000
5.4871-03
5 .• 87E - 03
SN IV
5P
EO' 2. 2U8E +00
( AYD)
N.·
2.1581
MU'
2.3.08
E (AYD)
1
(EV)
1 PHOT (IV)
LAMIOA (A)
(L/A/L-Il
CL/A/L+I)
SIGMA L-l
SIQMA L+ 1
SIOMA (MB)
.0000
.000
30.7811
402.70
5 .• 78Ii-Ol
-2.5471-01
1.8341-01
8.3711-02
2.771E-Ol
.4000
5.U2
31.231
342.21
4.2431-01
- 1.3781-01
1.3181-01
2.8741-02
1 . 1113E- 0 1
.8000
10.8.11
41. 873
287.52
3 .• 08E-01
-7."41-02
1.01I1E-Ol
8.7.81-03
1.1021-01
1.0000
13.108
44.38.
279.28
3.0881-01
-4.1421-02
8.8741-02
~.3101-03
IL3101-02
1.4000
111.0.8
48.837
248.78
2.11801-01
- 1 . IlIIII - 02
Il.8511-02
5.7871-04
7.0081-02
1.8000
21 .7Il8
52.11118
2311.80
2.3781-01
-5.4001-03
8.2151-02
8.421E-OII
8.2221-02
1.8000
24.~81
55.278
224.28
2.1871-01
3. 1l5' E-03
5.580E-02
3.0881-05
5.583E-02
2.0000
27.212
58.000
213.77
2.0.0E-Ol
1 . 08U -02
5.0541-02
2.8311-04
5.0.3E-02
3.0000
40.818
71.108
173. HI
'.4731i-Ol
3.1881-02
3.2541-02
3.0121-03
3.5111l1-02
7.0000
811 . 2. 1
128.030
Il•. 38
8.20151-02
3.8831-02
1.01IlE-02
8.37IlE-03
1.8541-02
8.0000
108.847
138.838
88.78
5.311E-02
3.8211-02
8.21101-03
8.5421-03
1.1l78E-02
8.0000
122.453
153.242
80.81
4.1l131-02
3.8441-02
8.8:10E-03
8.527E-03
1.531l1-02
SN IV
Il'
EO'
1.1841 E+OO (RYD)
N••
3.7074
MU'
2.2828
E (RYDI
1
(EV)
E PHOT (IV)
LAMIlOA
(A)
(L/A/L-\\l
(L/A/L+I)
SIOMA L-l
SIOMA L·l
SIOMA (MBI
.0000
.000
15 .•38
782.82
1. 027E +00
-8.033E-Ol
3.488E-OI
2.415E-Ol
5.1114E-01
.4000
5.442
21.281
582. 112
Il.35IlE-Ol
-::.811l1-01
1.8011-01
8.101E-02
2.41IE-Ol
1.0000
13.808
211.444
421.08
3.758E-OI
-8.2401-02
8.7111-02
8.3751-03
8.5481-02
1.4000
18.048
34.887
355.40
2.858E-Ol
-3.3801-02
5.873E-02
1. 8.0E -03
8.1411-02
1.15000
21.788
37.108
328.88
2.534E-Ol
-1.8701-02
5.0571-02
5.5121-04
5.1121-02
1.8000
24.481
40.328
307.4.
2.285E-OI
-7.2821-03
4.3331-02
8.810E-OII
4.3421-02
2.0000
27.212
43.050
288.00
2.0.0E-Ol
1.4511-03
3.751E-02
3.788E-08
3.752E-02
3.0000
40.818
1lO.81l8
218 .• 4
1. 318E -0 1
2.290E-02
2.05!5E-02
1.2441-03
2. l7I1E -02
5.0000
1l8.030
83.888
147.84
7.082E-02
2.8821-02
8.810E-03
3.1241-03
1.1831-02
7.0000
85.241
111.080
111.82
•. 588E-02
2.7881-02
4.8551-03
3.51l8E-03
8.424E-03
8.0000
108.847
124.888
98.~4
3.820E-02
2.1518E-02
3.810E-03
3.57 lE -03
7.:181E-03
8.0000
122.453
138.282
".81l
3.255E-02
2.41l0E-02
3.070E-03
3.50IlE-03
8.5781-03
,.
SN IV
8P
EO' 4.88118E-0'
(RYO)
N.· !l.7321
MU'
2.28711
1
(RYO)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-I)
(L/R/L+ 1 )
SIGMA L- 1
SIGMA L+ 1
SIGMA (MS)
.0000
.000
8.82!5
1871.35
2.3113E+00
-'.8!50E+00
7.1I48E-Ol
7.!5!5I1E-Ol
1.!5!51E+00
.2000
2.721
Il.347
1328.13
1 . 3!5!5E+00
-7.8!54E-Ol
3.5113E-OI
2.2114E-Ol
5.887E-Ol
.4000
5.442
12.088
1027.41
8.877E-Ol
-4.147E-Ol
1.11112E-Ol
8. 8115E-02
2.88IE-Ol
.8000
10.885
17 .510
708.08
4.7117E-OI
-1.513E-OI
8.440E-02
1.880E-02
1.0121-01
1.0000
13.108
20.231
812.84
3.77I1E-OI
-1I.578E-02
8.0521-02
7.773E-03
8.82I1E-02
1.4000
111.048
25.874
4'2.113
2.552E-OI
-3.753E-02
3.502E-02
1.515E-03
3.854E-02
I.IJOOO
21.7811
28.3115
438.85
2.182E-Ol
-2. 174E-02
2.78lE-02
5.823E-04
2.837E-02
1.8000
24.4111
31. 118
3118.48
t.88lE-OI
- 1. 0811E-02
2.258E-02
1 . 4811E -04
2.271E-02
2.0000
27.212
33.837
388.42
1.822E-OI
-2.7118E-03
1.884E-02
1.10IlE-05
1.885E-02
2.2000
211.1133
38.5511
3311. 14
1.42I1E-OI
2.1124E-03
1.584E-02
r . 30llE -05
1.585E-02
2.4000
32.B54
311.280
31!l.85
1.271E-OI
7.118E-03
1.32111-02
8.337E-05
1.337E-02
2.8000
35.375
42.001
21tll. 20
1.13I1E-OI
1.022E-02
1.142E:-02
1 . 838E -04
1 . 18lE -02
3.0000
40.818
47.443
281.34
Il.348E-02
1.422E-02
8.88lE-03
4.020E-04
Il.083E-03
5.0000
88.030
74.855
188.08
4.504E-02
1.802E-02
3. 173E-03
1.015E-03
4. 18eE -03
8.0000
81.835
88.281
140.48
3.451E-02
1.720E-02
2.2021-03
1.01l3E-03
3.2115E-03
7.0000
115.241
101.887
121.71
2.752E-02
1.81IE-02
1.8181-03
1.107E-03
2.723E-03
8.0000
108.847
115.473
107.37
2.280E-02
1 . 500E - 02
1 . 235E -03
1.08llE-03
2.3241-03
Il.0000
122.453
1211.0711
118.01
1.811I1E-02
1.3118E-02
Il.748E-04
1.054E-03
2.028E-03
SN IV
10P
EO' 2.871 IE-Ol
(RYO)
N·· 7.73118
MU'
2.2804
E (RYO)
E (EV)
E PHOT (EV)
LAMBDA
(A)
(L/R/L·1l
(L/R/L+t)
SICMA L- 1
SIGMA L+ 1
SIGMA (MS)
.0000
.000
3.834
3411.85
4.25I1E+00
·3. 133E+00
1.38lE+00
1 .41141+00
2.878E+00
.2000
2.721
8.355
11150.88
1.883E+00
-1I.1I28E-OI
3.770E-OI
2.824E-OI
8.3114E·OI
.4000
5.442
Il.077
1388.00
Il.28I1E-Ol
-4.503E-OI
1.844E-OI
7.71 OE-02
2.415E·OI
.8000
8.184
11. 798
1050.113
8.010E-Ol
-2.3117E-OI
8.11271-02
2.83I1E-02
1.177E·Ol
1.0000
13.a08
17.240
7 111.17
3.IIIIE-OI
-8.403E-02
3.8113E-02
5.100E-03
4.203E-02
1.4000
111.048
22.882
548.82
2.028E-Ol
-3.141E-02
1.1154E·02
Il. 375E -04
2.048E·02
1.8000
21.7811
25.404
488.08
1.881 E-0 1
-1.814E·02
1.5041·02
3.50lE-04
1. 5311E-02
1.8000
24.4111
28.125
440.84
1.42IE-Ol
-11.1821-03
1.18111·02
Il. 811 tE -OS
1.1118E·02
2.0000
27.212
30.848
401.115
1.220E-Ol
·2 .1I38E -03
Il.813E·03
1.114E·05
Il.8241 ·03
2.2000
28.1133
33.587
3811.37
1.08tE-OI
1 . 484E -03
7.11171-03
3.014E-08
7. 820E -03
2.4000
32.854
38.288
341.87
Il.334E·02
4.817E-03
8.823E-03
3.240E-05
8.855E-03
3.0000
40.811
44.452
278.'2
Il. 8114E-02
Il.757E-03
4.1721-03
1.773E·04
4.348E-03
8.0000
81.835
85.270
145.40
2.338E-02
1.150E-02
Il.78IE-04
4.72tE-04
1 . 448E -03
7.0000
115.241
118.878
125.40
1.848E-02
1.070E-02
7.0721-04
4.738E-04
r , 181 E-03
8.0000
108.847
112.482
110.23
1.507E·02
Il.1I0'E-03
!l.354E-04
4. 827E -04
Il . 118 tE • 04
SN IV
12P
EO'
1.8858E-OI
(RYO)
N.· Il.74211
MU'
2.2571
(RYO)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-I)
(L/R/L+ 1 )
SIGMA L·I
SIGMA L+l
SIGMA (MS)
.0000
.000
2.2113
5408.32
8.511I1E+00
-5.024E+00
2.0112E+00
2.425E+00
4.517E+00
.2000
2.721
5.015
2472.54
i . 7'4E +00
- 1 .077E+00
3.37I1E-Ol
2.438E-OI
5.817E-OI
.4000
5.442
7.738
1802.78
8.70tE-OI
·4.272E-Ol
1.227E-Ol
5.11 14E· 02
1.811E·OI
.8000
8.184
10.457
t lU . 811
5.280E-OI
-2.124E-OI
8.080E-02
1.1I77E-02
8. 038E -02
.8000
10.885
13.178
1140.1!5
3.575E-OI
-1.18tE-OI
3.!l28E-02
7.708E·03
4.211I1E-02
1.0000
13.808
15.8'11
7711.12
2.814E-Ol
-8.1188E·02
2.278E-02
3.232E-03
2.51111l-02
1.4000
111.048
21.342
580.88
1.80tE-Ol
-2.5301-02
1 . 148E ·02
5.723E-04
1.203E-02
1.8000
21.7811
24.083
515.28
1.312E-OI
·'.484E·02
8.870E-03
2.133E·04
8.883E-03
1.8000
24.4111
28.784
482.111
1.098E-OI
-7.3.111-03
8.783E-03
8.144E·05
8.825E-03
2.0000
27.212
211.505
420.22
8.354E-02
-2.5181-03
5. 40U -03
7.824E-08
5.415E-03
2.2000
2'.833
32.228
384.74
8.085E·02
8."2E·04
4.412E·03
1.072E-08
4.4131 ·03
2.4000
32.854
34.'48
354.78
7.072E-02
3.303E-03
3.8821-03
1. 588E -0!5
3.878E-03
3.0000
40.818
43.111
287.80
!l.00U-02
7.182E-03
2.285E-.03
'.285E-05
2.318E-03
4.0000
14.424
58.717
218.81
3.20IE-02
8.890E-03
1. 217E-03
1 . 878E -04
1.405E-03
5.0000
88.030
70.323
178.31
2.28IE·02
8.835E-03
7.5301 -04
2.300E-04
Il.830E-04
8.0000
81.835
83.82'
147.73
1.703E·02
8.323E-03
5.0118E-04
2.438E-04
7.532E-04
7.0000
115.241
17.535
127. 12
1.340E-02
7.711E-03
3.871E-04
2.435E-04
8.105E-04
SN IV
18P
EO' •. 4882E-02
( RYO)
N.·
13.7457
MU'
2.2543
E (RYO)
E (EV)
E PHOT (EV)
LAM8DA
(A)
(L/R/L-l)
(L/R/L+I)
SIGMA L- 1
SIGMA L+ 1
SIQIIIIA
(MB)
.0000
.000
t . 152
10781.10
1.283E+OI
-'.1I85E+00
3.848E+00
4.7I3E+00
8.84IE+00
.2000
2.721
3.873
3201.01
1.870E+00
-1.017E+00
2.284E-OI
1.877E·OI
3.'4 tE·Ol
.4000
5 .•• 2
8.5'5
1880.14
8.85U-OI
·3.400E-OI
8.4118E-02
3. tl5E-02
'.880E-02
.8000
8.184
Il.318
1330.'4
3.8481-01
-1.587E-OI
2.888E-02
'.58.E·03
3.845E-02
.8000
10.885
12.037
1030.05
2.504E-OI
-8.35.E-02
1.581 E -02
3.!l181-03
1. '33E-02
1.0000
13.808
14.758
840.12
1.78tE-OI
-4.7115E·02
'.802E-03
1.422E·03
1.122E-02
1.2000
18.327
17.4711
709.33
1.3.2E-Ol
-2.847E·02
8.58.1-03
5. '34E ·0.
7.188E·03
1.8000
21.78'
22.1122
5.0. I t
'.5.01-02
·'.1J77E-03
3.50tE-03
8. 81t E·05
3.511IE-03
1.8000
2•. 41t
25.843
4'3.11
7.088E-02
- •. 8311-03
2.8871-03
2.820E·05
2.7231-03
2.0000
27.212
28.38.
437.13
5. lUlU - 02
- 1. 747E-03
2.134E·03
3.828E-08
2.138E-03
2.2000
28.833
31.085
388.'8
5. 1411E-02
4.5031-04
1 . 728E -03
2.841E-07
1. 728E -03
2.4000
32.814
33.808
3115.15
4.480E-02
2.0111-03
1.421E-03
5.728E-08
1.4271-03
2.8000
35.315
38.128
33'."3
3 .... 3E·02
3.0841-03
1.1'01-03
1 . 45ISE - 08
1.2041-03
3.0000
"0.818
41 .1170
295."2
3.138E·02
4.4171-03
8.857E-04
3.4301-05
Il. OOOE -04
5.0000
lS8.030
8'.182
118.22
1. 3110E ·02
5.31181-03
2.7118E-04
8.444E-05
3.8"3E-0"
8.0000
81.835
82.788
14'.18
1. 041 E·02
5.084E·03
1.880E-04
8.8I5E-05
2. 770E ·0..
7.0000
t!5. 24 1
'8.3114
128.83
8. 188E -03
4.883E-03
1.3.. 71·0.
8. U8E ·05
2.233E-0"
9.0000
122."53
123.805
100.31
5.5131-03
3.18'1-03
7.870E-05
8.240E-05
1. 81IE-0"
SN IV
20P
EO- Il. 0802E -02 (AYD)
N•• 17.74158
MU-
2.2!532
E (AYD)
E (EV)
E PHOT 1EV)
LAM15DA (A)
(L/A/L-I)
(L/A/L+l)
SIGMA L-l
SIGMA L+l
SICMA (118)
.0000
.000
.15111
171137.150
2.03n+Ol
-1.1537E+OI
15.008E+00
7.7151E+00
1.377E+Ol
.1000
1.3151
2.052
15042.81
3.317E+00
-2.280E+00
4.727E-Ol
4.415al-Ol
Il.IIIU-OI
.4000
!5.442
15.134
2021.4.
!5.304E-Ol
-2.83I1E-Ol
3.1514E-02
1.78I1E-02
5.403E-02
.15000
8.1154
8.8511
1400.22
2.81515E-Ol
-1.172E-Ol
1.!524E-02
!5.0eIlE-03
2.033E-02
.8000
10.a811
11.11715
1071.07
1.82eE-OI
-15. 122E-02
8.112E-03
1.8181-03
Il.112I1E-03
1.0000
13.15015
14.2e7
887.21
1.284E-Ol
-3.472E-02
4.113eE-03
7.218E-04
5.1581E-03
1.4000
111.048
le.7311
1528.11
7.48eE-02
-1.20eE-02
2.31111-03
1.208E-04
2.440E-03
1.15000
2 1 . 7ell
22.481
11112.02
15.038E-02
-1I.1I0IE-03
1.71I1E-03
4.481E-0!5
1. 7150E -03
2.0000
27.212
27.1103
444.311
~.208E-02
-1.272E-03
1 . 03!lE -03
1. 8110E-015
1. 037E-03
2.2000
211.1133
30.524
404.811
3.15015E-02
2. 8117E-04
8.341E-04
1.047E-07
8. 3412E -04
2.4000
32.1554
33.3411
371.82
3.13IE-02
1.373E-03
15.848E-04
2.15a2E-08
15.875E-04
3.0000
40.818
41.11011
2e8.70
2. 182E-02
3.0415E-03
4. 1311E-04
1.1I14E-05
4.301 E-04
!5.0000
88.030
158.721
180.42
Il.!58n-03
3.712E-03
1. 323E -04
3.11158E-OII
1.720E-04
Il.0000
81.83!5
82.327
1110.80
7,.17I1E-03
3.477E-03
8. es8E-0!5
4.1'70E-OII
1.308E-04
7.0000
ell.241
115.1133
1211.24
5.1520E-03
3.2IlE-03
15.34I1E-0!5
~. '.51-011
1.0.eE-04
SN IV
50
EO- 1 .• '73IE+00 IAYDI
N••
3.21111'7
MU- .
1. '7043
E (AYD)
E (EV)
E PHOT (EV)
LAMIIDA lA)
(L/A/L-I)
(L/A/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA IMII)
.0000
.000
20.042
818.152
•. 354E-Ol
- 1. !515!5E+OO
Il.!5!5IE-02
1.81101+00
1.II.15E+OO
1.0000
13.8015
33 . .,.8
3158.•8
2.080E-OI
-'7.4.!5E-OI
3.!5I1IE-02
'7.03IE-OI
'7.3110E-OI
2.0000
2'7.212
.'7.254
28a.38
1.2'7IE-OI
-3.312E-OI
1.111111-02
1. lUSSE -0 1
2.148E-Ol
3.0000
40.818
150.8150
203.72
8.8'77E-02
-1..e'7E-OI
1 . 2 OllE-02
!5.14SE-02
Il.351E-02
•. 0000
5•. 424
74.488
1815.80
15.815n-02
-15.421E-02
8.31I1E-03
1.1581-02
1 . 1I110E - 02
5.0000
88.030
88.0'72
140.78
!5.251E-02
-2.083E-02
15.10.E-03
1.4141-03
'7.!518E-03
5.2000
70.7111
1I0.7e3
138.58
5.028E-02
-1.475E-02
!5.'7'70E-03
'7.44.E-04
8.515E-03
5.15000
'715.1113
1115.2315
128.84
4.1127E-02
-4.8eIlE-03
5.1801-03
8.'708E-OII
5.215n-03
!5.8000
78.e14
118.1157
125.all
4.447E-02
-7.8.4E-04
4.1118E-03
2.2118E-OII
~. e21 E-03
15.0000
81 .8311
101. 0'78
121.11.
•. 2'78E-02
2.87I1E-03
4.8'771-03
3.1'701-011
4.708E-03
8.0000
108.84'7
128.8110
1115.20
3.042E-02
2.34IE-02
2.lIl1eE-03
2.151531-03
5.1582E-03
14.0000
1110.483
210.52'
58.811
1.482E-02
2.1I'78E-02
1.1152E-03
'7.0281-03
8.IIIOE-03
111.0000
204.0811
22 •. 131
!51S.32
1. 3411E-O~
2.81115E-02
1. 025E -03
'7.08.1-03
8. lllE-03
115.0000
21'7.15118
237.737
112. 15
1.234E-02
2.808E-02
Il.104E-04
'7.05.I-oa
'7.1I8.E -03
SN IV
150
EO- 8.11332E-Ol
IAYD)
N••
4.3302
MU'
1 . 15a1l8
E IAYDI
E (EV)
E PHOT (EVI
LAMBDA CAl
(L/A/L- 1)
(L/A/L+I)
SIGMA L- 1
SIGMA L+I
SIGMA CM8)
.0000
.000
11. 810
10157.110
15.1127E-Ol
-2.08.E+00
1.400E-Ol
1 .11021+00
2.042E+00
.5000
15.803
18.413
8'73.38
3.4'7l!-01
-1.2158E+00
5.5'7I1E-02
1.1115E+00
1.172E+00
1.0000
13.15015
25.218
4111 .159
2.184E-Ol
-'7.888E-Ol
3.023E-02
5.1187E-Ol
!5.8811E-OI
3.0000
40.818
!52 .• 28
238.4e
7.524&-02
-1.302E-OI
7.480E-03
3.348E-02
4.0e5E-02
4.0000
54.424
1511.0a.
18'7.78
5.388E-02
-5.508E-02
4.818E-03
7.5.eE-03
1.23n-02
5.0000
88.030
7e.ll40
155 .•8
4.101E-02
- 1. 888E -02
3.3'7eE-03
1.01581-03
4 .•• 7E-03
Il.8000
78.1114
110.5211
138.1115
3.412E-02
-2.I1153E-03
2.8501-03
2.1I'7'7E-05
2.8'7eE-03
15.0000
81.835
113.2415
132.11'7
3.21511E-02
-15.11841E-OII
2'.50lSE-03
1. 71SE -08
2.50IlE-03
15.2000
84.35'7
115 .•87
1211.20
3.1315E-02
2 .•8.E-03
2.3721-03
2.232E-0!5
2.3e.E-03
8.4000
87.0'78
118.U8
125.53
3.011E-02
4.7.7&-03
2.24I1E-03
8.38411-05
2.333E-03
15.15000
811.7.11
101.4011
122.215
2.811.E-02
8.'7115E-03
2.13111-03
1.74.E-04
2.310E-03
8.0000
108.8.'7
120 .•118
102.113
2.2113E-02
1 . 5'7.E -02
1.537E-03
1.1251-03
2.882E-03
12.0000
1153.2'71
174.881
70.110
1.302E-02
2. II OE-02
'7.45111-04
2 . 113 SE -03
3.1582E-03
14.0000
leO .•8a
202.0113
81.31
1.080E-02
2.04lE-02
5.5e8E-04
3.1'74E-03
3.'734E-03
111.0000
204.0811
215.81111
5'7.48
Il.S115E-03
1.1I84E-02
•. 1I10E-0.
3.200E-03
3. etl E-03
115.0000
217.15115
22e.305
54.0'7
8.15'781-03
I.IIII1E-02
•. 338E-04
3.184E-03
3.1518E-03
SN IV
80
EO- 3.lIe8IE-01
(AYD)
N.· 8.3510
MU'
1.84110
E CIIYDI
E (IV)
E PHOT (EV)
LAMBDA 1Al
t L/A/L-I )
IL/A/L+I)
SIGMA L-l
SIGMA L+l
SIQMA (M8)
.0000
.000
5.311'7
22e'7.2.
1.330E+00
-3.120E+00
2.311111-01
1.1181&+00
2.22lE+00
.5000
15.803
12.200
1018.27
3.8Ial-01
-1.305E+00
4.47IE-02
7.8.0E-Ol
8.28n-Ol
1.0000
13.15015
le.003
852 .•8
1.1I152E-OI
-8.882E-OI
1.8.0E-02
3.1I1eE-Ol
3.383E-OI
2.0000
2'7.212
32.150e
380.22
8.784E-02
-2.284E-Ol
15.3251-03
8.41IE-02
7.048E-02
4.0000
54.424
lIe.821
207.215
3.58I1E-02
-3.802E-02
1.113'71-03
3.2150E-03
Il.1117&-03
Il.0000
158.030
'73.42'7
lU.815
2.U15E-02
-1.3381-02
1.302E-03
~.1I5111-04
1.7I1U-03
Il.8000
'78.eI4
8•. 311
1.7.015
2.115111-02
-2.1118E-03
Il. 1115ei -04
2.708E-05
1.024E-03
8.0000
81.8311
87.033
142.48
2.0'70E-02
- 1. 0411E -03
Il.375E-04
3.1513E-015
Il.41lE-04
15.2000
84.387
811.'7114
138.1.
l.e7I1E-02
5. e151lE -04
8.833E-04
1 . 20SE -oe
8.84U-04
15.4000
8'7.0'78
112.4711
134.08
1.8114E-02
2.0.IIE-03
8.338E-04
1 ..... E-08
8.485E-04
15.8000
112.520
Il'7 .• ,7
128.152
1.7.lE-02
•. 485E-03
7.4153E-0.
'7.381E-OII
8.19I1E-04
7.0000
115.2.1
100.8311
123.20
1.8'731-02
5.4158E-03
7.0'77E-04
1.13.1-0.
8.21 lE-04
10.0000
1315.0811
'.1.4515
87.85
1.0131-02
1.18IE-02
3.ll471-04
7 .••11-04
1.10111-03
13.0000
1715.8'77
182.2'74
158.02
15.II".E-oa
1.210E-02
2.20IlE-04
1.007E-03
1.228&-03
1•. 0000
1110.483
1115.880
153.30
8.233E-03
1. 183E -02
1.1113E-04
1 .0331 -03
1. 225E -03
15.0000
204.0811
20e."815
511. III
5.033E-03
1.1.81-02
1.1I'71E-04
1.04U-03
i , 2081 -03
115.0000
21'7.811!5
223.0112
lS5 .5a
!5.11I1E-03
1.1101-02
1.415111-04
1.03151 -03
1.1831-03
18.0000
244.e015
250.304
4e.53
4.28111-03
1.028E-02
1.18IE-04
Il.e7IE-04
1.114E-03
20.0000
2'72.118
2'77 .!5111
.... 158
3.8.3E-03
9.4'715E-03
Il.3!58E-05
Il.3e15a-0..
1.033E-03
20
SN IY
10D
10' 2.211051-01
(RYD)
N.· 8.357a
MU'
1. 8421
E (AYD)
1
(EY)
E PHOT (EV)
LAMBDA
(A)
(L/R/L-l)
(L/R/L+l)
SIGMA L-l
SiaMA L+l
SiaMA
(MB)
.0000
.000
3.118
3a78.51
2.102E+00
-4.11131+00
3.481E-Ol
2.0381+00
2.3821+00
.5000
Il.803
9.a19
12411.94
3.538E-Ol
-1.1781+00
3. 12lE -02
5.174E-Ol
5.4171-01
1.0000
13.8011
1&.722
741.44
1.&On-Ol
-5.4011-01
1.088E-02
1.840E-Ol
1.a4IE-Ol
2.0000
27.212
30.328
408.81
&.584E-02
-1.70n-Ol
3. 304E -03
3.331E-02
3.8112E-02
3.0000
40.818
43.1134
282.21
3. 7UE' 02
-1I.1I117E-02
1.588E-03
7.3831-03
8.1151 E -03
4.0000
54.424
57.540
215.48
2.543E-02
-2.7251-02
a.354E-04
1.1111 E-03
2.54 7E -03
5.0000
118.030
71.1411
174.27
1.85111-02
-a.1I53E-03
Il.17al-04
2.500E-04
8.117I1E-04
5.'000
7' .a14
82.031
1!51 . 15
1.507E-02
-2.283E-03
4.882E-04
1.1112E-05
4.8431-0.
8.0000
81. B35
84.752
1411.2a
1 . 438E -02
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4.31141-04
3.042E-OII
4.424E-04
8.2000
84.357
87.473
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1.72n-04
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8.4000
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1.310E-02
1.188E-03
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4.784E-0&
3 .1I41E -04
8.8000
sa . 71111
112.1115
133.44
1.254E-02
2.0801-03
3.873E-04
1.5151 -05
3.825E-04
8.0000
108.847
11'.a84
110.74
Il.524E-03
5. aUE-03
2.553E-04
1.518E-04
4.08111-04
14.0000
1110.483
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114.04
4.215E-03
7.a2I1E-03
8.11481-05
4.585E-04
5.450E-04
15.0000
204.0111
207.205
511. 84
3.804E-03
7.8110E-03
7.S3SE-OS
4.820E-04
S.374E-04
lB.OOOO
217.811S
220.811
58. 1S
3.4541-03
7.42I1E-03
8.820E-05
4. 5115E - 04
S.257E-04
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1 . 411 04 E- 0 1 (RYD)
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1.83811
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2.028
8114.17
2.111111+00
-S.221E+00
4.S5I1E-Ol
2.084E+00
2.S40E+00
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8.803
8.831
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3.01131-01
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2.124E-02
3.425E-Ol
3.838E-Ol
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4.123E-03
5.010E-03
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5.0000
88.030
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3.371E-04
1.402E-04
4.773E-04
8.0000
81.1135
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2. 382E -04
2.0871-08
2.403E-04
8.2000
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2. 12I1E-04
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112.S20
114.S48
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8.884E-03
2.047E-03
1.8781-04
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2.02SE-04
8.0000
108.847
110.875
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4.3S5E-03
1.3721-04
7.a27E-05
2.185E-04
10.0000
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138.087
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5.070E-03
5.777E-03
8.a24E-OS
1. 738E -04
2.830E-04
14.0000
1110.483
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3.084E-03
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4.·803E-OS
2.421E-04
2.881E-04
15.0000
204.0811
2011.117
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2.782E-03
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2.438E-04
2.83I1E-0.
18.0000
217.8115
219.722
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Il.832E-Ol
2.172E+00
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1.033E-02
1.1128E-Ol
1.72I1E-Ol
1.0000
13.808
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8.877E-02
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2.1I04E-03
•. 7117E-02
S.088E-02
2.0000
27.212
28.287
438.83
3.2118E-02
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7.72lE-04
7.730(-03
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3.0000
40.818
41.873
2118.10
1.830E-02
-3.%2SE-02
3.52SE-04
1. 842E -03
1.III104E-03
4.0000
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223.48
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2.018E-04
3.S45E-04
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88.030
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8.058E-03
4.548E-04
8.131E-OS
Il.874E-07
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Il.8000
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110.854
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8.1172E-04
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8.788E-08
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8.0000
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112.81
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2.878E-03
5.2741-0S
2.1171E-05
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12.0000
183.271
18 •. 3211
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3.8111E-03
2.38lE-OS
8.443E-05
1.082E-0.
14.0000
190.483
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15.0000
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3.448E-03
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1.072E-04
18.0000
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Il.230E-02
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8.438E-02
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27.212
27.857
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9.785E-04
4.0000
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8.433E-03
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5.0000
88.030
88.57S
180.S.
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Il.110E-OS
8.0000
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82.281
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4.73111-07
4.504(-05
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4.1a3E-OS
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2.a88E-04
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8.8000
81. 71111
110.444
137.0a
4.0401 -03
5.9281-04
3.710i-OS
1.11181-08
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108.847
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113.24
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2.5110(-05
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13.0000
178.877
177.522
811.84
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2.S27E-03
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4.278E-05
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14.0000
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1111.128
84.87
1. 328E-03'
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2.382E-03
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217.811S
218.340
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2.308E-03
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2.474E-03
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ll.41I1E-03
10.0000
138.01111
1110.472
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3. 7411E -02
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7.!l7I1E-03
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3.241 E-02
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8.187E-03
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4.8000
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74.8111
188.03
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3.4731-02
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77.3117
180.20
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70.7111
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2.883E-07
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73.472
82.8311
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Il. 722E-02
1.2110E-08
2.812E-02
2.8'2E-02
7.0000
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104.808
118.112
2.344E-03
8.8201-02
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1.747E-02
1.74I1E-02
10.0000
138.01111
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2.llll8E-03
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2. 783E-01I
8.112I1E-03
8.853E-03
11.0000
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151.032
77.118
2.1!S1Ii-03
3.1081-02
2.80IE-oI
7.027E-03
7.01lIlE-03
12.0000
183.271
172.838
71.82
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3.0I15E-02
2.73IE-0!l
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SN IV
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8.1112
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4.781E+00
3.14IE-Ol
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4.087E-02
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2.0000
27.212
33.723
387.88
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1.401E-Ol
1.4141-01
3.0000
40.8'8
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281.117
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2.137E-04
8. 730E-02
8.751E-02
4.0000
54.424
80.113!l
203.47
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1.3110E-Ol
2.1I1E-01I
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ll.1I881-02
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70.711
77.282
180.47
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Il.113E-08
2.475E-02
2.47!lE-02
Il.4000
73."72
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8.1188E-02
7.388E-07
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5.8000
78. 1113
82.70!S
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1.828E-08
2.18IE-02
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101 .7113
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1.428E-02
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122.4113
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2.488E-03
4.334E-02
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10.0000
138.01111
142.171
88. Ils
2.4411-03
3.8115E-02
2. 288E -011
8.1188E-03
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158. '77
711.311
2.341E-03
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Il.710E-03
12.0000
183.271
1811.713
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2.217E-03
2.770E-02
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1.483E-02
1.483E-02
!l.2000
70.75'
74.382
188.811
8.4331-0!l
7. 183E-02
8.2110E-OII
1.3781-02
1.378E-02
!l.4000
73.472
77.103
180.81
3.88!lE-04
8.811E-02
2.811lE-07
1. 284E -02
1.284E-02
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78. 1113
711.824
1!l1l.32
8. 28U -o.
8.470E-02
8.432E-07
, . 200E -02
1.200E-02
Il.8000
78.1114
82.11411
1110.20
8 .• !llE-04
Il.1!l8E-02
1.58SE-08
1.123E-02
1. 124E-02
7.0000
115.2.1
118 .• 73
125 .• 0
1.802E-03
4.705E-02
8.835E-08
7.880E-03
7.887E-03
8.0000
108.847
112 .• 7.
110.23
1.828E-03
3.872E-02
1.010E-0!l
8.084E-03
8.084E-03
10.0000
138.0511
1311.lIll0
88.78
1. 840E -03
2.782E-02
1.274E-05
3.828E-03
3.838E-03
11.0000
1••. 885
1!l3.2118
80.88
1.783l-03
2.377E-02
1.283E-05
3.10IlE-03
3. 122E-03
12.0000
1113.271
11'8.1102
74.211
1 . 8ll1Sl - 03
2.084E-02
1 . 248E -011
2 .IIUE -03
2.588E-03
SN IV
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8.834E+00
1.4110E·OO
8.450E·oO
7.1140E+00
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8.803
Il. 105
1381.78
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1.304E+00
3.740E-02
5.583E-Ol
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1.0000
13.808
15.110.
7711.41
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8.533E-03
1.778E-Ol
1.843E-Ol
2.0000
27.212
211.514
420. 10
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8.2115E-04
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3.0000
40.818
43. 1111
287.8.
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2.213E-02
2.222E-02
4.0000
114 .• 24
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218.57
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7.'25,E-02
1.102E-01I
1.278E-02
1.280E-02
4.8000
8!l.308
87.810
183.38
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8.112E-02
8.485E-07
Il.070E-03
Il.071E-03
!l.0000
88.030
70.331
1711.211
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Il.787E-02
1.322E-07
8. 31111E -03
8.311I1E-03
5.2000
70.751
73. 0112
1811.72
1.87U-O!l
5.453E-02
5.1128E-l0
7.801E-03
7.801E-03
5.4000
73."72
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183.83
2. 535E - 04
5. 187E-02
1.311 E-07
7. 2811E-03
7.2I15E-03
!l.8000
78.1114
81.2111
152.88
8.248E-0.
4.8115E-02
8.533E-07
Il.3.8E-03
8.3.7E-03
8.0000
81 .11311
83.1137
1.7.71
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•.•• 3E-02
1 . 338E - 08
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5.1152E-03
Il.0000
122 .• 113
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2 .•• 8E-02
8. 788E-OII
2. 880E-03
2. e.7E-03
10.0000
138.0511
138.381
8ll.81
1.3111E-03
2.07I1E-02
7.213E-08
2.1.7E-03
2. 1511E-03
Il.0000
1.11.8115
1!l1 .1187
8 1 . 511
1.332E-03
1.788E-02
7.25éE-0.
1.7 •• E-03
1. 751E-03
12.0000
1.3.271
1811.573
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1.258E-03
1.!l!l2E-02
7.05"E-08
1 .• 32E-03
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1.5815
7817.41
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1.080E+Ol
2.324E+00
Il.1I48E+00
8.1172E+00
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2.721
4.307
2878.57
- 1. 250E+00
2.884E+00
1.812E-Ol
1.28I1E+00
1 .• 1I7E+00
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7.028
1784.08
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1.440E+00
4.730E-02
5.23lE-Ol
5.70.E-Ol
1.0000
13.11015
15. 1112
8115.13
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4.547E-Ol
4.511E-"3
1.128E-Ol
1.173E-Ol
2.0000
27.212
28.7118
430.84
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t , 15UE-O 1
4.0115E-04
2.1182E-02
3.0231;-02
3.0000
40.818
42.404
282.311
-7,I.7E-03
Il.418E-02
5.833E-05
1.3111E-02
1.387E-02
•. 0000
54.424
515.010
221. 37
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Il.2115E-02
7.015E-015
7.771E-03
7.778E-03
•. 8000
155.308
1515.884
185.38
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4.783E-02
4.255E-07
5.4815E-03
5.48I1E-03
5.0000
118.030
118.11115
178.10
-2.288E-04
4.51 1E-02
8.812E-08
5.087E-03
5.087E-03
8.2000
70.751
72.337
171.40
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4.2154E-02
3.203E-13
4.722E-03
4. 722E -03
5.4000
73.472
75.058
1115. 18
1.880E-04
4.03I1E-02
7.147E-08
4.3111E-03
4.3871;-03
5.8000
711.183
77.778
1511.41
3.535E-04
3.833E-02
2.11181;-07
4.103E-03
4.103E-03
Il.0000
81.1535
83.222
148.88
5.820E-04
3.411I1E-02
7.855E-07
3.588E-03
3.51171;-03
7.0000
115.241
1115.827
128.05
Il.45BE-04
2.773E-02
2.333E-015
2.1173E-03
2.1575E-03
10.0000
1311.01111
137.1145
80.08
1.078E-03
1.1518E-02
4.312E-OII
1. 284E -03
1 . 2118E -03
11.0000
148 . 11115
151 .251
81.87
1.040E-03
1.3111E-02
4.402E-OII
1.050E-03
1 . 055E - 03
12.0000
1153.271
1154.8117
75.21
Il.7117E-04
1.2015E-02
4. 23I1E-015
8.1I11E-04
8. 883E-04
SN IV
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2.388E+00
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7.247E-Ol
8.524E-Ol
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1.015E+00
2.787E-02
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2.803E-Ol
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14.488
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5.188E-02
5.414E-02
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27.212
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1.148E-0\\
1.825E-04
1.328E-02
1.3"8E-02
3.0000
40.818
41.700
287.33
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Il.308E-02
2.887E-05
5.1158E-03
5.88I1E-03
4.0000
54."24
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224.18
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4.144E-02
3.248E-08
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3.414E-03
4.8000
85.308
88.1111
187.32
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3.182E-02
2.028E-07
2.407E-03
2.401E-03
5.0000
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88.1112
171.82
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3.000E-02
4.884E-08
2.2215E-03
2.227E-03
5.2000
70.751
71.833
173.08
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2.834E-02
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2.883E-02
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2.54I1E-02
1.018E-07
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7.0000
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88.124
128.811
Il.285E-04
1.838E-02
1.023E-08
1.187E-03
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108.847
1011.730
1 12.811
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1 .507E-02
1.532E-08
8.848E-04
8.1181E-04
10.0000
138.0811
138.11"2
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1.071E-02
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Il.1110E-03
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12.0000
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184.153
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1.841E-08
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8.720E-03
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5. 750E-01l
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3.785E-02
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111.327
211. 1117
473.82
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ll.8eeE-04
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27.212
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40.818
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2.215E-02
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413.811
1 .881 E-0 1
ll.813E-03
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4.241E-05
1.778E-02
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27.212
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8.470E-04
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15.0000
118.030
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4. 787E -04
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18.327
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70.751
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1. 1110E-03
7.5118E-03
10.0000
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13.0000
1711.177
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111.0000
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1.857E-02
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7.14111-03
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15.424
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5.2000
70.751
18.145
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2.28IE-03
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3.181E-02
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5.35I1E-02
8.0000
108.847
123.1184
100.24
.000
3.153E-02
.000
7.7:1U-03
7.725E-03
111.0000
217.11811
232.531
53.32
.000
1.3321-02
.000
2.58d-03
2.584E-03
TE VI
lOS
EO' 5.8804E-Ol
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N·· 7.7522
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2.2478
E ( AYO)
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8.150
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8.221E-Ol
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4.354E-Ol
4.354E-Ol
1.0000
13.11011
2 1 . 7511
H8.88
.000
2.430E-Ol
.000
8.073E-02
8.073E-02
4.0000
54.424
112.574
1S18. 14
.000
5.373E-02
.000
1.135E-02
1.13I1E-02
Il.0000
81.11311
&SI.7811
138.08
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3.208E-02
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5.807E-03
Il.807E-03
TE YI
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N·· 8.7115"
MU'
2.2450
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(L/R/L+')
SICMA L-l
SIOMA L+l
SIGMA
(Mil)
.0000
.000
• 5.147
2408.77
.000
1.33I1E+00
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5.7I18E-Ol
5.7118E-Ol
1.0000
13.11011
18.753
11111 . '5
.000
2.210E-Ol
.000
5.75I1E-02
5.75I1E-02
4.0000
114.424
58.1171
208.13
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4.142E-02
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Il.4221-03
Il.422E-03
10.0000
1311.05S1
141.2011
87.81
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1.208E-02
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1.2UE-03
1.2.8E-03
TE VI
ll1S
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1.8021E-Ol
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N·· 13.71173
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2.2427
E (AYO)
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lL/A/L-ll
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4780.83
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8.811I1E-Ol
1.811I1E-Ol
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Il.803
8.381
1320.27
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3.74I1E-Ol
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8.27I1E-02
8.27I1E-02
1.0000
13.11011
Ill. le.
7115.114
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1.1182E-Ol
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2.813E-02
2.813E-02
2.0000
27.212
2S1.800
4111.011
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Il.812E-02
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8.84I1E-03
•. 84I1E-03
4.0000
114.424
57.012
217.48
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2 . III1U - 02
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2.551E-03
2 .UI E- 03
TE VI
20S
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1.14181-01
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N·· 17.7583
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2.2417
E (AYDI
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LAMIOA (A)
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SlaMA L-l
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1.1153
7982.110
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3.5152E+OO
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1.232E+00
1.232E"00
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2.721
4.274
2800.118
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8.2121-01
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1.147E-01
1. 84 7E-0 1
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5.442
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1772.311
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4.032E-Ol
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7.147E-02
1. (l000
13.11011
15. 1118
817.80
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1.281E-Ol
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1 . 1181E - 02
1.1188E -02
2.0000
27.212
28.71111
431.03
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5.008E-02
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4.113111-03
4.I13I1E-03
TE VI
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2.07811
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(L/R/L+l)
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57.428
215.80
2.825E-Ol
1.1181-02
1.02IE-Ol
3.4I1U-04
1.033E-Ol
1.0000
13.11011
71.034
174.55
2.0Sl41-01
4.4' lE -02
Il.5221-02
5.780E-03
7. IOlE -02
2.0000
27.212
84.838
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5.492E-02
4.48I1E-02
1.070E-02
5.511I1E-02
5.0000
118.030
125.457
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5.487E-02
1.847E-02
1. 5UE -02
3.1128E-02
Il.0000
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131.0113
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7.3351-02
5.227E-02
1.5117E-02
1.5S121-02
3. 1118E- 02
7.0000
SlII.241
152 . 1I11S1
81. 21
Il.347E-02
4.81541-02
1.281E-02
1.570E-02
2.85U-02
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122.453
178.881
118.83
4.824E-02
4.43lE-02
SI. 1371-03
1.478E-02
2.383E-02
TE VI
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2.0315
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318.1111
5.23111-01
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4.81S1E-03
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3.7I18E-07
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8.1114
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315.78
3.11841-01
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7. 88!E -05
1.0571-01
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40.11211
3011.20
3.3811-01
1.3371-02
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3.0421-06
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12.245
43.3411
2811.04
3.0521-01
2. UU-02
8.457E-02
1.013E-03
8.I158E-02
1.0000
13.11011
44.7011
277.33
2.8021-01
2.772E-02
7.889E-02
1.43S1E-03
8.033E-02
3.0000
40.818
71.118
17:1.40
1.344E-Ol
5.033E-02
2.721E-02
7.1131E-03
3.48I1E-02
4.0000
54."24
811.524
144.87
1.017E-Ol
6.es8E-02
1.852E-02
8.457E-03
2 . 1IS18 E- 02
5.0000
118.030
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125.07
8.024E-02
6.5110E-02
1.337E-02
8 . 5S1U - 03
2. l87E-02
8.0000
81.11311
112.7311
108.Sl8
Il.533E-02
4.22IE-02
1.008E-02
8.613E-03
1.8481-02
7.0000
811.241
1211.362
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5.448E-02
3.80111-02
7.85I1E-03
8.077E-03
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21
TE VI
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27.231S
4511.22
3.725E-Ol
4.1143E-03
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27.212
40.842
303.57
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3.0117E-02
2.188E-03
3.31IE-02
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3.7113E-02
1. 5118E-02
3.28IE-03
1 .1I24E - 02
4.0000
54.424
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3.!lI!lE-02
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3. !l23E-03
1.30IlE-02
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81.880
151.83
8.078E-02
3.170E-02
8.314E-03
3.437E-03
1.7!l2E-03
TE VI
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1.111172
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7.1148
1821.17
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8.283E-Ol
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2.721
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1.238E+00
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3.328E-Ol
4.087E-02
3.738E-Ol
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1.243E-Ol
3.381E-03
1.277E-Ol
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7.03IE-04
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13.1108
21 .254
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8.21I1E-02
3.80lE-0!l
Il.223E-02
1.1000
14.1187
22.814
541.28
3.38I1E-Ol
1.1118E-03
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1.2000
111.327
23.117!l
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7.838E-03
4.8110E-02
Il.170E-0!l
4.11118E-02
1.3000
17.888
2!l.338
4811.37
2.787E-Ol
1.271E-02
4.121E-02
1.718E-04
4. 1311E-02
2.0000
27.212
34.a80
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1.113I1E-Ol
2.727E-02
1 .1I53E -02
1.081&'-03
2.082E-02
3.0000
40.818
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Il.443E-02
2.8!lIlE-02
Il.0!l3E-03
1.1180E-03
1 .071 E-02
4.0000
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112.072
11111.75
Il.283E-02
2.!l88E-02
!l.100E-03
1 . 7311E -03
8. 8311E-03
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118.030
7!l.1I78
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4.!l14E-02
2.287E-02
3.230E-03
1 . 1158E- 03
4.888E-03
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1 .111135
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4.8112
2!l34.!l1l
3.152E+00
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1.018E+00
2.1132E-Ol
1.311E+00
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2.721
7.813
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1.50aE+00
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3.1128E-Ol
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4.181E-Ol
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8. 1114
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1.025E-Ol
3.8111 E- 03
1.082E-Ol
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Il. 8110E - 02
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17.137
723.110
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3.1114E-04
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1.0000
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1170.28
3.414E-Ol
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4.!I 1TE-02
8.310E-05
4.528E-02
1.1000
14. _117
11.8sa
1124.38
3.031E-Ol
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3.822E-02
4. U8E -011
3.823E-02
1.2000
111.327
21.2111
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2.713E-Ol
3. 837E -03
3.270E-02
1 . 1711E - O!l
3.2'71 E- 02
1.3000
17.888
22.!l71
5411.11
2.444E-Ol
S.280E-03
2.82!1E-02
Il. 48!lE-0!l
2.832E-02
1.4000
11.041
23.140
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2.2181-01
1.18n-02
2.482E-02
1.40IE-04
2.47I1E-02
3.0000
40.818
45 . '71 0
271.25
7.504E-02
2.211E-02
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1.3831,-04
8.327E-03
4.0000
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201.03
4.88lE-02
1.172E-02
2.138E-03
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3.103E-03
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88.030
72.121
170.03
3.4!121-02
1.72!l1-02
1.820E-03
1.08IE-04
2.72I1E-03
7.0000
115.241
100.133
123.a2
2.048E-02
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8.800E-04
7.!lI5IE-04
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1.83421-01
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1.381
3.8158
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1.723E-Ol
8.473E-Ol
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2.721
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1.74"E+00
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8.184
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13.3ao
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3.818E-02
Il.12TE-04
3.1180E-02
1.0000
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770.03
2.1132E-Ol
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2.338E-02
a. 1113E-05
2.3dE-02
1.1000
14.1117
17.482
710.03
2.2I8E-Ol
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1.112111-02
1.370E-O!l
1.130E-02
1.2000
111.327
18.823
8!l8.71
2.024E-Ol
Il. 171 E-04
1.111I5E-02
3.003E-07
1.1I1!lE-02
1.3000
17.888
20.183
1114.30
1.800E-Ol
4.30n-03
1.370E-02
1 . !l811E - O!l
1. 37IE - 02
1 .5000
20.401
22.104
1541.32
1.485E-Ol
1.17'71-03
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8.082E-015
1.024E-02
1.8000
21 . 7811
24.2111
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1.320E-Ol
1. 0711E -02
8.8111E-03
1.177E-04
8.17IE-03
3.0000
40.818
43.313
288.25
4.111E-02
1. 438E -02
2.2110E-03
3.750E-04
2.U!lE-03
4.0000
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217.83
3.1112E-02
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3.800E-04
1.!l72E-03
5.0000
118.030
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7.240E-04
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1.07H-03
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1.1018E-Ol
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MU·
1.1811
E (RYD)
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LAMIlDA (AI
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1.510
8211.38
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2.107E+00
1.21I1E+00
4.123E+00
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1.381
2.871
4311.211
3.2821+00
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8.47I1E-Ol
1 . 7118E - 0 1
8.274E-Ol
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2.721
4.231
21130.315
1.714E+00
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2.8015E-Ol
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7.453E-Ol
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8.010E-02
8.14IE-03
8.1I04E-02
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8.1'14
1.873
1281.71
4.27aE-Ol
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3.7081-02
1.787E-03
3.18T1-02
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10.88!l
12.31!l
1000.32
2.81I1E-Ol
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2.0e3E-02
3.8I1IE-04
2.102E-02
1.0000
13.8011
1!l.118
820.24
2.01aE-Ol
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1.210E-02
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14.1187
18.478
712.51
1.7415E-Ol
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t . 052E -02
1 . 130E -015
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1.2000
18.327
17.137
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8. '7141-03
2.0115E-Oa
8.714E-03
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7.327E-03
1.4000
11.048
20.515a
803.10
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4. 80TE -03
Il.2251-03
1 .IIIOE -05
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2.0000
27.212
28.722
431.118
Il.847E-02
1.I83E-03
2.820E-03
1 . illE -04
2.140E-03
3.0000
40.818
42.328
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1.017E-02
1.12IE-03
1.8315E-04
1.313E-03
4.0000
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155.134
221.117
2. 231E -02
8. liTE -03
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7.723E-04
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LAMIDA (A)
(L/R/L-l)
(L/R/L+I)
SIGMA L- 1
S1aMA
L+l
SIGMA (MB)
.0000
.000
41.151
301.25
2.101E-Ol
-5.551E-Ol
1.541E-02
4.182E-Ol
5.531E-Ol
1.0000
13 ••0.
54.1.3
228.40
1.140E-Ol
-2.351E-Ol
4. 110E -02
1.141E-Ol
1.5.4E-Ol
2.0000
21.212
.8.3.11
111.35
1.240E-Ol
-1I.1.0E-02
2 .•41E-02
2.455E-02
5.01l.E-02
3.0000
40.818
81 .1115
151. 25
Il.40lE-02
-3.040E-02
1.82/E-02
2.85.E-03
2.101E-02
3.4000
411.2110
81.418
141.83
8.524E-02
-1.3.8E-02
1.5111E-02
•. 110E-04
1 .e58E-02
3 .•000
48.1181
110. 1311
131.55
8. 135E -02
- •. 111E-03
1.500E-02
1.558E-04
1.515E-02
3.8000
51.102
112.8110
133.52
1.115E-02
- • . • 25E-04
, .411 E-02
1 . 5311E -O.
1.411E-02
4.0000
54.424
115.15.'
1211.12
1.44lE-02
4. 144E -03
1. 330E -02
8.11lE-05
1. 338E -02
5.0000
.8.030
1011.181
113.155
•. 011E -02
2.381E-02
1.013E-02
2. 3411E -03
1.248E-02
8.0000
I l .135
122.1.a
100.111
5.0821-02
3.441E-02
1.1I11E-03
5.481E-03
1.345E-02
8.0000
108.841
UO.005
82 .•5
3. 145E -02
4.2111E-02
5.288E-03
1. 04 lE -02
1.510E-02
12.0000
1113.211
204.42.
110.•5
2.32I1E-02
4.24I1E-02
2.188E-03
1 . 3112E -02
1.II11E-02
13.0000
1111.811
218.034
5 •. 81
2.10IlE-02
4.128E-02
2.431E-03
1.40lE-02
1 .1I44E -02
14.0000
1110.483
231.1140
53.53
1.1120E-02
3.11113E-02
2.141E-03
1 . 311aE -02
1 .1I01E -02
TE VI
110
EO·
1.18.'E+00 (RVD)
N·.
4.48115
MU'
t .5105
E (RVDI
E (EV)
E PHOT (EV)
LAMIDA (A)
(L/R/L-I)
(L/R/L+I)
SIGMA L- 1
SI GlllA L+l
SIGMA (MB)
.0000
.000
24.302
510.20
4.-418E-Ol
-1I.533E-Ol
1.1112E-Ol
8.32I1E-Ol
Il.518E-Ol
.5000
•• 803
31. 105
3118.111
2.118.E-Ol
-5.405E-Ol
•. 1111 E-02
3.421E-Ol
4.124E-Ol
1.0000
13 ••0.
31.1108
321.08
2.185E-Ol
-3.252E-Ol
4.550E-02
1.511E-Ol
1 . Il1111 E -0 1
2.0000
21.212
51.514
240 .•11
1.350E-Ol
-1.254E-Ol
2.3.0E-02
3.054E-02
5.413E-02
3.0000
40.818
.5.1111
1110.40
Il.351E-02
-4. 3.IIE -02
1.433E-02
4 .e'.(-03
1.11021-02
3.8000
51.102
7 •. 004
,.3.,3
7.353E-02
-1.117E-02
1. 033E -02
3.518E-04
1.01lIlE-02
4.0000
54.424
78.725
151.411
•. 1I.0E-02
-5.535E-03
Il.581E-03
Il.084E-05
Il.1118E-03
4.2000
57.145
81.447
152.23
• . • 02E-02
- •. '.41-04
8.1122E-03
1.1.'E-O.
8.1123E-03
4.4000
511.8 ••
84. 1118
141.31
•. 2721-02
3 .e82E -03
8.323E-03
4.302E-05
8.3.'E-03
4 .•000
.2.587
IlS. 8811
142.70
5.1I.IIE-02
7.444E-03
7.182E-03
1.815E-04
7 .1I.4E -03
•. 0000
81 .e315
105.1131
117.04
4.38.E-02
2. 351E -02
5.123E-03
2.218E-03
7.34lE-03
12.0000
'.3.211
187.513
••. 10
1.804E-02
3.070E-02
1.535E-03
• . •eIlE-03
8.200E-03
13.0000
1111.811
201.11'
1 .• '1E-02
2 .1I12E -02
1.323E-03
•. 101E-03
8.023E-03
. ' .e3
14.0000
1110.483
214.184
51.13
1.4.0E-02
2.'88E-02
1.151E-03
•. 1I50E-03
7.80lE-03
1•. 0000
211 .•85
241.118.
51.23
1. 21lE-02
2.8dE-02
8.II11E-04
•. 388E-03
7.27I1E-03
TE VI
80
EO-
8.485d:Ol
(RVD)
N·· 8.5135
MU-
1 .48.5
E <RYD)
E (EV)
E PHOT·(EV)
LAMBtlA (A)
(L/R/L-l )
(L/R/L+I)
SlQMA
L- 1
SIGMA L+l
SIGMA
(MB)
.0000
.000
11.545
1073.113
8.1I11lE-Ol
-1.1153E+00
2.307E-Ol
1 .•1I0E+00
1.8111 E+OO
.5000
•. 803
18.348
. ' 5 . ' 5
4.218E-Ol
-7.1I08E-Ol
8.1111E-02
4.32.E-Ol
5.14.E-Ol
1.0000
13 .•08
25. 151
4112.117
2.53111-01
-3.117I1E-Ol
4.07.E-02
1.501E-Ol
1.1I0IlE-Ol
2.0000
27.212
38.757
3111.111
1.210E-Ol
- 1. 2111E -0 1
1.512E-02
2.451E-02
4.02I1E-02
3.0000
40.818
52.3.3
23 •. 18
7.8.lE-02
-4.43111-02
8.13aE-03
3. 8a 1E-03
1.202E-02
3.8000
51.102
.3.248
111•. 03
5.82lE-02
-1.4.IIE-02
5.387lt-03
5.145E-04
5.1I02E-03
4.2000
57.1415
.8.1180
180.50
5.10111-02
-5. &40E -03
4.502E-03
8.23I1E-05
4.584E-03
4.4000
511.8.15
11. 411
173 .• 2
4.80lE-02
-2.050E-03
4.131E-03
1 . 13/E- 05
4.148E-03
4 .•000
.2.587
14.132
'.7.25
4. 525E -02
1.044E-03
3.815E-03
3.041E-0.
3.818E-03
4.8000
.5.308
7 •. 854
'.'.33
4.213E-02
3.117E-03
3.528E-03
4.002E-05
3.58'E-03
5.0000
.8.030
711.575
155.81
4.0.41-02
•. 02I1E-03
3.211E-03
1 . OIlOE-04
3.381E-03
•. 0000
81 .•35
113. 181
133.0.
3. 15lE-02
1.372E-02
2.325E-03
• . • 'OE-04
2.118.E-03
8.0000
108.147
120.3a2
102.1111
2.103E-02
1 .1I1.E -02
1.338E-03
1 .•• 'E-03
3.005E-03
10.0000
13 •. 0511
147 .e04
14.00
1.15251-02
1.1113E-02
8 .•321-04
2.1 •• E-03
3.030E-03
12.0000
'.3.211
174.81.
70.a2
1.1118E-02
1.880E-02
5.III1I1E-04
2.32I1E-03
2.112I1E-03
13.0000
11 •. 811
188.422
8l5.80
1.038E-02
1. 814E-02
5. 104E -04
2.331E-03
2.U1E-03
14.0000
'110.483
202.028
.'.31
Il.300E-03
1.143E-02
4.3112E-04
2.314E-03
2.153E-03
TE VI
100
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(AYo)
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MU·
1.4114
1
(RYD)
E (EY)
E PHOT (EV)
LAMloA
(A)
(L/R/L-I)
(L IR/L. 1)
SIGMA L- 1
SIGIIIA L+ 1
SIGMA
1Ml51
.0000
.000
•. 145
'.38. 111
1.4.'E+00
-3.204E+00
3 .•47E-Ol
2 .e "E+00
2.1115E+00
.SOOO
•. 803
13.548
1115. 11
4.1221-01
-8.1131E-Ol
7.5114E-02
4.080E-Ol
4.838E-Ol
1.0000
13.80.
20.3151
.011.24
2.44.E-Ol
-3.8110E-Ol
3.oeOE-02
1. , . , E-O 1
1.4."-01
2.0000
21.212
33."7
3.5.13
1.011E-Ol
-1.12.E-Ol
Il.1111E-03
1. 1123E -02
2 .•03E-02
3.0000
40.818
47.583
2.0 .•8
•. 234E-02
-3.7311-02
4 .•41E -03
2. 4111E -03
7.143E-03
3.8000
51.702
58.441
212.13
4.48lE-02
-1.2110E-02
2.1150E-03
3 .•115E-04
3.311E-03
4.2000
51.145
113.8110
1114.0.
3.88.E-02
-5.8114E-03
2.42.E-03
7.80IlE-05
2.504E-03
....
4.4000
511.8••
"
18 •. 13
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-2.811 E -03
2.213E-03
2.011E-05
2.234E-03
4 •• 000
.2.581
.11.332
118.83
3.41lE-02
-4.515(-04
2.021E-03
5.412E-07
2.028E-03
4.8000
.5.308
12.053
112.08
3.208E-02
1 .e '4E-03
1.8.3E-03
1.013E-0.
1.810E-03
5.0000
.8.030
74.115
1.5.81
3.023E-02
3.3'4(-03
1.118E-03
3.241E-05
1.150E-03
•. 0000
81. .35
88.3"
140.28
2.311(-02
Il.222E-03
1.1112E-03
2.834E-04
1.41.E-03
8.0000
10'.847
115.15112
101.28
1.513E-02
1.322E-02
• . •48E -04
1.820E-04
1.421E-03
Il.0000
1411.e115
15 •. 410
79.21
Il.310E-03
1.333E-02
3.452E-04
1.048E-03
1.383E-03
12.0000
'.3.211
110.0111
12.113
8.21lE-03
1. 2112E -02
2.881 E-04
1.011E-03
1.3!5I1E-03
13.0000
1111.811
183 .•22
87.52
1.2.IIE-03
1.245E-02
2.43I1E-04
1.013E-03
1.311E-03
14.0000
1110.483
1117.228
82.8.
•. 4I1lE-03
1. 1115E-02
2.088E-04
1.0.'E-03
1.210E-03
31
TE VI
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MU'
1. ~7~5
E (RYD)
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LAM5DA
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(L/R/L-I)
(L/R/L+l)
SIGMA L- 1
SIGMA L+l
SIGMA ~MB)
.0000
.000
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280~.211
2.155E+00
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5.1118E-Ol
3.III1I1E+00
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Il.803
11. 22~
110~. 53
4.732E-Ol
-8.1187E-Ol
8.318E-02
3.41BE-Ol
4.050E-Ol
1.0000
13.11011
18.027
1187.77
2.111I1E-Ol
-3.514E-Ol
2. 185E-02
8.3113E-02
.1.058E-Ol
2.0000
27.212
31.1133
3111 . 115
8.844E-02
-1I.413E-02
8.21I1E-03
1.057E-02
1.117I1E-02
3.0000
40.818
45.2311
274.07
4.11117E-02
-3.050E-02
2.80IlE-03
1.587E-03
4.3113E-03
3.8000
51.702
511.124
220.12
3.512E-02
-1. OIlIlE-02
1 . 7~OE -03
2.41I1E-04
1.182E-03
4.2000
57. 1~5
111 . 5811
201.311
3.027E-02
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1.418E-03
5.885E-05
1.475E-03
4.4000
511.81111
114.287
111~.811
2.824E-02
-2.715E-03
1.28I1E-03
1.78I1E-05
1.307E-03
4.11000
112.587
117.0011
185.03
2 .1I43E -02
-B.124E-04
1. 17I1E-03
1.887E-OII
1.178E-03
4.8000
85.308
81.730
177.81
2.480E-02
8.234E-04
1.078E-03
1.783E-OII
1.07I1E-03
5.0000
88.030
72.451
171.13
2.332E-02
2.210E-03
9.1I03E-04
1.334E-05
1.004E-03
8.0000
81 .1135
811.057
144.07
1.77IE-02
8. 738E-03
8.788E-04
1.~72E-0.
8.280E-0.
12.0000
1113.271
107.8112
73.1.
8.133E-03
9.551E-03
1.588E-0.
5.708E-0.
7.31~E-0~
13.0000
178.877
181.2118
88.311
5 .• 28E-03
9.1114E-03
1.342E-0.
5.77BE-0.
7.11I1E-0.
14.0000
1110.~83
1114.110.
113.81
•. 832E-03
8.815E-03
1.144E-04
5.711 E-O.
Il. 858E -O.
15.0000
20~. 081
208.510
511.48
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8.~34E-03
Il.B7I1E-05
5.5112E-0.
8.580E-04
TE VI
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1.7058E-Ol
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MU'
1.4712
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E PHOT (EV)
LAMIIDA
(A)
IL/R/L-O
(L/R/L+l1
SIGMA L- 1
SIGMA L+l
SIGMA (Mil)
.0000
.000
2.320
5343.20
3.855E+00
-8.335E+00
B.1I70E-Ol
Il.078E+00
8.1145E+00
.2000
2.721
5.042
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1. 0811E +00
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1.~1I3E-Ol
Il.8831-01
1.118E+00
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7.783
1517.18
5.38lE-OI
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5.1150E-02
3.270E-Ol
3.835E-Ol
1.0000
13.808
15.11211
778.50
1.87I1E-Ol
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1 . 124E -02
•. 381E-02
5.485E-02
2.0000
27.212
21.532
4111.13
8. 1511E -02
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2.814E-03
4.885E-03
7.81IE-03
3.0000
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287.~2
3.335E-02
-2.0114E-02
1.208E-03
7.13lE-04
1.1I1I1E-03
3.8000
51.702
5.,023
2211.51
2.321E-02
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7.31.E-0.
1.117E-04
8 .• 31E-0.
•. 0000
5 •.• 24
511.7.4
218.50
2.1.3E-02
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8.550E-0.
8.03llE-05
7.154E-0.
•.• 000
511.811ll
112.188
1111.38
1. 8411E-02
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5.3.8E-0.
Il.8110E-OII
5 .•• 5E-0.
•. 11000
82.5.7
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1.727E-02
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4 .• II.E-0.
1.53I1E-OII
4.880E-0.
•.• 000
111.308
87.11211
183.33
1.1118E-02
2.824E-0.
•.•• OE-O.
2.0331-07
•. 4~2E-0.
5.0000
88.030
70.350
178.24
1.517E-02
1. 1811E-03
•. 071E-0.
3.75lE-OII
•. 1OllE- O.
8.0000
81 .N5
83.1511
1.7.8.
1.1.3E-02
•. 15.E-03
2.75I1E-04
5 .• 7.E-05
3.308E-0.
•. 0000
108.8.7
111.18.
111.5:l
7.2I1.E-03
Il.13I1E-03
1 .•• 7E-0.
1.5.0E-0.
3.08111-0.
10.0000
138. OSII
13 •. 380
811.110
5. 150E -03
8.21181-03
'g.228E-05
2.0"E-0.
2.lllE-0.
12.0000
183.271
'85.5111
7•. 87
3 .• 71 E-03
5.118.E-03
8.238E-05
2.22.E-0.
2.847E-0.
13.0000
178 .• 77
1711. 1117'
811. 11
3 .• ,.E-03
5.740E-03
5.251E-08
2.22I1E-0.
2. 75 lE -o.
1•. 0000
1110 .••3
1112 .•03
8•. 31
3.03I1E-03
5.41I1E-03
4.475E-05
2.111I1E-0.
2.8.8E-04
TE VI
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1.048.E-Ol
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LAMIOA (A 1
(L/R/L-l)
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SIGMA L+l
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5.1153E+00
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1.2711+00
8 .••31-00
1.0111-01
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2.721
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3.82I1E-02
2.10IE-Ol
2 .• 118E-Ol
1.0000
13 .1108
15.032
82 •. 711
1.285E-Ol
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8.235E-03
2 .• 2I1E-02
3.052E-02
2.0000
27.212
2•. 1138
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•. 512E-02
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1 .• 1I8E-03
2.187E-03
•. 033E-03
3.0000
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2 .• 0.1-02
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Il. 137E-04
3.118111-0.
Il.U3l-0.
3 .•000
51.702
53.121
233.37
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3.117I1E-0.
5 .•3 lE-OS
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111.81111
111.2113
202.211
1.311IE-02
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2.1178E-0.
5.5551-011
2.73.E-0.
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112.587
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1.2301-02
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2. 433E -O.
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4.8000
115.30.
118.735
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1.1501-02
1.2112E-04
2.21.1-0.
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2.21I1E-04
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118.030
1111 .•511
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7.71101-0.
2.030E-04
1.5. . . -011
2.04I1E-04
Il.0000
81.135
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148.27
•. 01131-03
2.8114E-03
1.387E-0.
2.1123E-05
1.130E-0•
•. 0000
108 .•47
110.27.
112 .•3
5.1.21-03
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7.3281-05
7.138E-05
1 .•117E-0.
10.0000
131.058
137 .•811
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21.7B8
23.08'
537.47
8.7811E-04
1. 282E-Ol
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1.382E-02
1.3112E-02
2.0000
27.212
28.511
434.87
2.885E-03
1.022E-Ol
Il.U1E-08
1.070E-02
1.070E-02
3.0000
40.818
42.117
284.38
3.837E-03
Il.525E-02
1 . 1170E -015
Il.438E-03
Il.4158E-03
4.0000
54.424
515.723
222.51
3. UlE-03
4.8211E-02
t.7711E-05
4.283E-03
4.301E-03
5.0000
88.030
118.321
178.84
2.8511E-03
3.485E-02
1 .1131 E-05
3. 040E -03
3.058E-03
VII
5$
10- 8.22451+00
(llYD)
N·· 2.8057
MU'
2.1e43
E (lIYD)
E (IV)
E PHOT (EV)
LAMBDA
lA)
(L/R/L°1)
(L/R/L+')
SIOMA L-I
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148.40
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1. !lIBE-Ol
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1.223E-Ol
1.223E-01
1.0000
13.808
118.2e!l
128.14
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1.280E-Ol
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1.013E-Ol
1.013E-Ol
2.0000
27.212
111.1101
110.80.
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8.!l08E-02
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10.0000
138.01111
220.1411
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4.7!lOE-02
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3.130E-02
3. 130E -02
Vil
8S
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N·· 3.U88
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E PHOT (EV)
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411.053
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2.431E-Ol
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1.88IE-Ol
1.881E-Ol
1.0000
13.80B
58.lIl1e
211.37
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1.151E-Ol
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1.138E-Ol
1.138E-Ol
2.0000
27.212
12.211!l
171. 57
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1.343E-Ol
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8.1113E-02
8.1113E-02
8.0000
108.U1
1113.1101
80.!l8
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4.1118E-02
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2.340E-02
2.340E-02
18.0000
211.8II!l
2112.748
41.19
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2.40BE-02
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Il.1172E-03
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111.382
840.38
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4.804E-Ol
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2.801E-Ol
2.8071-01
1.0000
13.808
32.1188
318.08
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2.3113E-Ol
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1.1!l8E-Ol
1.158E-Ol
2.0000
21.212
48.!l14
288.21
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1.41131-01
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8.28I1E-02
8.255E-02
8.0000
108.U7
128.2011
118.71
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3.!l08E-02
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Il.1I1!lE-03
Il.91!l1-03
14.0000
1110.483
209.U5
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1.111I1E-02
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4. 121E-03
4. 1271-03
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24.358
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Il.!le81-02
Il.!l1l8E-02
2.0000
21.212
37.1184
3211.!l1l
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1.328E-Ol
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4.11181-02
4.1eIlE-02
8.0000
81.83!l
a2.387
134.20
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3.888E-02
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7.812E-03
1.812E-03
12.0000
183.271
114.023
71.2!l
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1.4111E-02
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2.432E-03
2.432E-03
Vil
12S
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N·· Il.8773
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2.1227
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E PHOT (EV)
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8.834
1814.38
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1.123E+00
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5.41!lE-Ol
1.0000
13.808
20.440
808.80
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2.387E-Ol
.000
7.320E-02
1.320E-02
4.0000
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81 .2!l1
202.40
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4.803E-02
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8.180E-03
8.880E-03
8.0000
108.841
11!l.881
101.18
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1.1I08E-02
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2.8471-03
2.841E-03
VII
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2.543!lE-Ol
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N·· 13.81e1
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2.1203
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E (EV)
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LAMBDA
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1.1188E+00
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8.421E-Ol
8.421E-Ol
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8.803
10.284
1208.01
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4.1021-01
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1. 0811E-0 1
1. 085E-0 1
1.0000
13.808
11.081
128.48
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1.840E-Ol
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4.038E-02
4.038E-02
3.0000
40.818
44.218
280.02
.000
4.124E-02
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8.20aE-03
8.20IlE-03
8.0000
108.841
112.308
11 0.40
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1. 205E - 02
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1.02.E-03
1. 024E -03
VII
205
EO'
1.5328E-Ol
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N·· 11.8801
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2.11113
E (RYDI
E (EV)
E PHOT (EV)
LAIIIBDA
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3.001E+00
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1.1801+00
1.180E+00
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2.121
4.808
25111.80
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8.8881-01
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2.314E-Ol
2.314E-Ol
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5.442
1.528
1841.011
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4.!l83E-Ol
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Il.850E-02
Il.850E-02
1.0000
13.808
15 . 11111
1110.11
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1. !l211E-0 1
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2.305E-02
2.305E-02
2.0000
21.212
211.2111
423.20
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8.023E-02
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8.818E-03
8.878E-03
5.0000
88.030
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'18.83
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1.841E-02
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1.111!lE-03
1. (1I5E -03
Vil
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1.11108
E (RYD)
E (EV)
E PHOT (EV)
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(L/R/L+1)
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12.8118
110.8!l
2.2a2E-Ol
5.0541 -02
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1.713E-03
8.112E-02
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2.04!lE-Ol
5.I112E-02
8.841E-02
1.053E-02
1.884E-02
1.0000
13.808
88.282
143.13
1.148E-Ol
8.1I13E-02
5.!l221-02
1.388E-02
8.1I08E-02
4.0000
54.424
121.080
81.51
Il. !l08E -02
8.110E-02
2. 401E -02
1.188E-02
4.3114E-02
5.0000
88.030
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88.13
8.108E-02
5.8091-02
1. 831E -02
1.888E-02
3.828E-02
Il.0000
81.83!l
1!l4.2112
80.38
1.018E-02
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1.5112E-02
1 .1I52E -02
3.5.3E-02
Il.0000
122.453
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4.811!lE-02
4.1128E-02
Il.81!lE-03
1.15IE-02
2.118E-02
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2.11501E+00
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1 .11245
E (RYD)
E (EV)
E PHOT ( EV)
LAM8DA
lA)
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4. 038E -0 1
2.010E-02
1.31IE-Ol
8.1112E-04
1.318E-Ol
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5.4.2
45.581
212.01
3.283E-Ol
4.081E-02
1.0281-01
3.180E-03
1.081E-Ol
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10.88!l
51.024
243.00
2.7321-01
5.200E-02
1.1I11E-02
15.18IE-03
8.5115E-02
1.0000
13.808
53.145
230.118
2.510E-Ol
5.538E-02
1.0115E-02
8.1I0IlE-03
1.188E-02
2.0000
21.212
81.351
184.08
1.13I1E-Ol
8.118E-02
4.288E-02
1.0118E-02
5.324E-02
3.0000
40.818
80.11111
153. 15
1.290E-Ol
5.824E-02
2.823E-02
1.1110E-02
4.013E-02
4.0000
5 •. 424
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1.003E-Ol
5.524E-02
1.11841 -02
1.20IlE-02
3.203E-02
5.0000
88.030
108.188
1 i4.82
8.018E-02
5.083E-02
1.418E-02
1.115E-02
2.11113E-02
1.0000
1111.241
1315.380
111.58
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4.315E-02
8.1181E-03
1.058E-02
1. '511E -02
8.0000
108.841
148.1188
83.22
4.82I1E-02
3.981E-02
1.211E-03
Il.1I20E-03
1.120E-02
35
VII
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I.3183E+00
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8. 1013
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E (EV)
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17.1iI01i1
81i12.30
8.Ii1I5E-01
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2.1i182E-OI
7.282E-03
3.05BE-OI
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2.721
20.830
800.1iI1i1
7.053E-Ol
-3.880E-02
2.150E-OI
I.288E-03
2.183E-Ol
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5.442
23.352
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5.744E-OI
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iii. 284E -08
I.814E-Ol
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8.803
24.712
501.72
5. 221i1E-OI
1iI.01il8E-03
1. 415E-0 1
8. 581i1E-Oli
1.418E-Ol
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28.073
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1. 881i1E -02
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3.815E-0.
1. 254E-0 1
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10.885
28. 7iii4
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3.22IE-02
1iI.1iI28E-02
1 . 257E -03
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2.11i18E-03
8.2881-02
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5. l1i18E - 02
3 .• 971-02
5.10.E-03
4.0081-02
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1.81i18E-02
5.742E-03
2 .• 72E-02
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5 •. 424
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8.71i17E-02
•. 287E-02
1.173E-02
5.58Ii1E-03
I.72Ii1E-02
5.0000
88.030
88.1l38
14 •. 27
8.81Ii1E-02
3.788E-02
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5.180E-03
1.305E-02
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8. 101i18
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1223.08
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5 .• 72E-OI
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2.721
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118•. 23
1.044E+00
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1.374E-03
1.188E-Ol
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1.545E-Ol
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18.301
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5.71i13E-01
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1.218E-Ol
2.211 E-05
1.287E-OI
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7.250E-03
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10.885
21.022
511i1. 7IiI
•. 5115E-Ol
1.885E-02
1iI.211IlE-02
2.443E-04
Il.323E-02
1.0000
13.808
23.743
1122.20
3.74I1E-Ol
2.1I00E-02
8.IiIIiIIE-02
8.3e.E-0.
7.074E-02
2.0000
27.212
37.341i1
331 .117
1.757E-Ol
•. 234E-02
2 .• 141-02
2. 805E -03
2.81i15E-02
3.0000
40.818
50.1i155
2.3.32
1.045E-Ol
3.808E-02
1. 185E-02
3.01lIlE-03
1 .• 75E-02
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3.278E-02
8.701E-03
2.11021-03
Il.804E-03
8.0000
101.847
1 18 . 1185
104.20
2.557E-02
1.1137E-02
1 .830E -03
1.870E-03
3.501E-03
VII
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2.370E+00
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7.870E-Ol
8.808E-02
8.550E-Ol
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2.721
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1 . 325E +00
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3.31i1111-01
1 . 838E - 02
3.582E-Ol
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3.807E-05
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12.245
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880.78
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1.518E-02
8 .•• 4E-02
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1.0000
13.808
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3.800E-Ol
2.107E-02
5 .• 8.E-02
3.7.4E-0.
5.502E-02
2.0000
27.212
33.730
387.58
1.512E-Ol
3 .•• 11-02
1.818E-02
1.873E-03
1.713E-02
3.0000
40.818
47.33i!
281 .•3
1.583E-02
3.02.E-02
7.270E-03
1.113E-03
Il.083E-03
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5 •. 42.
80.1142
203 .• 5
5.110IE-02
2.553E-02
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1 . 884 E- 03
5 . 87. E- 03
8.0000
101.847
115.388
107.47
1.11.21 -02
1 .•55E -02
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2.721
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2043.72
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3.051 E-05
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30.557
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227.71
2.118lE-02
8.08lE-Ol
1.054E-03
1. 812E+00
1.1113E+00
1.0000
13.8011
1I8.084
182.18
2.873E-02
8.1173E-Ol
1.5131-03
1.0881+00
1.080E+00
2.0000
27.212
81.8eo
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2.774E-02
5.188E-Ol
1.883E-03
7.824E-Ol
7.841E-Ol
3.0000
40.818
811.288
130.111
2.582E-02
4.14I1E-Ol
1.711E-03
5.877E-OI
5.884E-Ol
4.0000
54.424
108.872
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2.388E-02
3.414E-Ol
1.114I1E-03
4.5118E-Ol
4.573E-Ol
10.0000
138.0118
180.507
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1.380E-02
1.434E-Ol
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VII
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385.77
3.5IIlE-02
8.7411-01
t.151E-03
8.300E-Ol
Il.312E-Ol
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13.808
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3.58lE-02
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1.823E-03
8.480E-Ol
8. 501lE -0 1
2.0000
27.212
81.108
202.118
3.187E-02
4.5821-01
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4. 801E-0 1
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40.8111
74.715
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2.754E-02
3.5.81-01
1.5281-03
3.383E-Ol
3.408E-Ol
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108.847
142.7411
88.88
1.4113E-02
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10.0000
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188.8117
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1. 178E-02
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545.81
4.388E-02
8.288E-Ol
1.1821-03
5.818E-Ol
5.830E-Ol
1.0000
13.808
38.322
341.38
4.1181-02
5.880E-Ol
1 . 8157E-03
4.223E-Ol
4.238E-Ol
2.0000
27.212
48.828
248.33
3.3871-02
4.058E-Ol
1.52I1E-03
2.8I1"3E-Ol
2.888E-Ol
3.0000
40.818
83.534
185.15
2.753E-02
3.054E-Ol
1. 287E -03
2.1UE-Ol
2.1411-01
5.0000
88.030
80. 7411
138.83
1.828E-02
1.8331-01
8.083E-04
1.21BE-01
1.2271-01
8.0000
81.835
104.351
118.82
1.852E-02
1.5HE-Ol
7.88n-04
8.573E-02
lL8110E-02
10.0000
1311.058
158.7711
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8.874E-03
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4.188E-04
4.280E-02
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12.155
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4.422E-02
Il. 742E -0 1
8.400E-04
I.H4E-Ol
1. 880E-0 1
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2.721
14.878
833.44
5.08I1E-02
8.854E-Ol
1 . 03 IlE -03
2. 381lE -0 1
2.371lE-Ol
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4.082
18.237
783.80
Il. 188E-02
8.4571-01
1.187E-03
2. 431E -0 1
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8.2211-01
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2.448E-Ol
2.4118E-Ol
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8.803
18.8118
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5.08I1E-02
5.810E-Ol
1.3251-03
2.4271-01
2.440E-Ol
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8.524
21.871
571.81
4.8771-02
Il.487E-Ol
1.388E-03
2.3271-01
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10.885
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538.13
4.744E-02
5.221lE-Ol
1.3871-03
2.280E-Ol
2.274E-Ol
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25.781
481.28
4.48I1E-02
4.778E-Ol
1.383E-03
2.1121-01
2.121lE-Ol
2.0000
27.212
38.387
314.115
3.238E-02
3.184E-Ol
1. 112E-03
1.433E-Ol
1.444E-Ol
4.0000
54.424
88.578
188.22
1.808E-02
1.738E-Ol
8.517E-04
7.208E-02
7. 273E- 02
10.0000
138.0118
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7.080E-03
5.8071-02
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3.087E-02
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7.823E-02
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15.3807
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.81113
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(L/R/L+l)
SIGMA L-l
SIGMA L+l
SI GIIIA
(MS)
.0000
.000
3.881
3388.34
5.8114E-Ol
-8.1I10E-Ol
3.214E-02
8.421E-02
Il.835E-02
.1000
1.381
5. 0~2
24811.30
3.80<4E-OI
-1I.085E-02
1 .1I85E -02
1. 4Il4E -03
2.114E-02
.1500
2.041
5.722
2188.110
3.238E-Ol
4.218E-02
1.814E-02
3.852E-04
1.850E-02
.2000
2.7: 1
8. ~02
11138.55
2.802E-OI
1.24I1E-Ol
1.354E-02
3.585E-03
1 . 712E -02
.3000
4.082
7.783
15117.20
2.188E-Ol
2.104E-OI
Il.1I112E-03
1.234E-02
2.233E-02
.7000
Il.524
13.208
1138.113
1. OIllE -0 1
2.483E-Ol
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2.877E-02
3.2118E-02
.8000
10.885
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851. 22
Il. 541E -02
2.37~E-Ol
3.578E-03
2.114I1E-02
3.308E-02
.11000
12.245
15.1128
778.50
8.488E-02
2.278E-Ol
3.07d-03
2.1181E-02
3.28I1E-02
1.0000
13.808
17.287
711.23
7.518E-02
2.114E-OI
2.812E-03
2 .1I3d -02
3.201E-02
2.0000
27.212
30.8113
~01.34
3.388E-02
1.385E-Ol
Il.541E-0~
2. 121E -02
2.222E-02
4.0000
54.~24
58.105
213.38
1.38I1E-02
7. 12.E -02
2.8112E-04
1.080E-02
1. 0811E-02
8.0000
81.835
85.318
145.33
1.883E-03
~.451E-02
1.34I1E-04
8.010E-03
8.205E-03
8.0000
108.841
112.B28
110.18
5.02d-03
3.078E-02
7.8~IIE-05
3.823E-03
3.1I00E-03
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SIGMA 1MB)
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2.318
5348.00
7.125E-OI
-1.138E+00
3.1101-02
2. BOSE-Ol
2.825E-Ol
.1000
1.3Bl
3.8111
3370.15
4.038E-Ol
-3.5I1U-Ol
1.813E-02
1.10n-02
3.31111-02
.1500
2.041
~.3511
2844.21
3.21lE-01
-1.27I1E-Ol
1.258E-02
2.582E-03
1.513E-02
.2000
2.721
5.040
2480.28
2.73IE-Ol
3.04IE-03
1.012E-02
1.873E-08
1.013E-02
.3000
4.082
Il.~OO
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2.022E-Ol
1.218E-Ol
1.041E-03
3.1581-03
1.080E-02
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8.803
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131111.30
1.283E-Ol
t.11I8E-Ol
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1.180E-02
1.584E-02
.8000
10.885
13.203
1138.01
1.815E-02
1.813E-Ol
2.205E-03
1. 511IE -02
1. 118E -02
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12.245
14.584
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8.1I04E-02
1. 73~E-0 1
1.810E-03
1.513E-02
1. 180E -02
1.0000
13.808
15.1124
178.80
8.IIIIE-02
1.852E-Ol
1. 808E -03
1.581E-02
1 . 722E -02
2.0000
21.212
211.530
~111.88
2. Blin -02
1.027E-Ol
5.381E-O~
1.11111-02
1.1731-02
4.0000
54.424
58.142
218.51
1.00H-02
5.18IE-02
1.54I1E-04
Il.4811E-03.
Il.8UE-03
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81.83!
83.1154
141.88
5.804E-03
3.208E-02
1.100E-05
3.102E-03
3.113E-03

Document Outline