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Submitted on 1 Jan 1979
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DOUBLY EXCITED STATES OF THE LiI ISOELECTRONIC SEQUENCE
K. To, E. Knystautas, R. Drouin, H. Berry
To cite this version:
K. To, E. Knystautas, R. Drouin, H. Berry. DOUBLY EXCITED STATES OF THE LiI ISOELECTRONIC SEQUENCE. Journal de Physique Colloques, 1979, 40 (C1), pp.C1-3-C1-5.
�10.1051/jphyscol:1979101�. �jpa-00218380�
JOURNAL DE PHYSIQUE
Colloque C1, supplkment au n o
2,Tome
40,fkvrier 1979, page C1-3
K.X. To,
E.
Knystautas, andR.
Drouin Universite Laval, Quebec, Canada G l K 7P4and
H.
G. BerryDepartment of Physics, University of Chicago, Chicago, 60637 and Argonne National Laboratory, Argonne, 60439, USA
Rdsuml. Nous presentons les niveaux d'lnergie des systSmes multi-excitls de la sequence iso6lectronique 2 Li I, jusqu's Ne VIII. Les identifications sont basses sur de
recents experimentaux et theoriques, qui suggsrent une rlvision des termes
Abstract. We present the term level diagams of the doubly excited quartet systems of the L i I isoelectronic sequence up to NeVIII. The identifications are based on recent theoretical and experimental work which suggest a revision particular1 y, of the 2 ~ 3 ~
4 ~ 0
terms.The three electron doubly-excited quartet system of been reclassified i n O V I where the data are taken from the L i I isoelectronic sequence has been extensively investi- several sourcesfb9 and recent unpublished work at gated using the beam f o i l technique.' However, identifi- Argonne. The reclassifications in fluorine and neon are cations have been hampered by low light intensities in most based mostly on work at ~ a v a l , ~ O f ' ~ but with comparable such transitions and by typically large line widths of the results by Pegg eta[.* i n fluorine and Buchet eta~.~inneon.
beam foil spectra. Several questions remain, the most out-
4
o standing of which i s the classification of the 2snpP
(n23) levels for a l l isoelectronic sequence members. Crossley and other recent calculation2 suggest that earlier experimental identifications of the low members of the sequence of 2s3p4 ~ 0
may be in error. Our results here for higher membersof the sequence tend to confirm the theoretical values, but only i n N V (see figure) are definite closed loops of transi- tions to this level observed. Our observations i nB
I11 also suggest agreement with theory, but the relevant transitions are of very weak intensity and may possibly be blended.We present below energy level diagams for the quartet terms for all ions L i I to NeVIII. The lines identi- fied are taken from many different sources. Thus, the LiI transitions are from the recent work sf Bromander et a l a 3 reported in this Conference. The Be I1 transitions are from Hontzeas et a1.4 and earlier work quoted therein. Note
4 o
that the
P
term has been reassigned. More wbrk in the vacuum ultraviolet spectra of lithium and beryllium i s4 o needed to verify the theoretical predictions in the
P
terms.The B I11 transitions are taken from
TO,^
and unpublished work at Edmonton (Berry and Pinnington) and at Lyon (Berry and Subtil). The carbon and nitrogen transitions have been measured recently at Argonne and Laval. Worki s continuing on these spectra. Several transitions have
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1979101
JOURNAL DE PHYSIQUE
207.51(
d
( I S ~ ~ ~ ~ P O )In future work, we shall include a more complete
l i s tof energies, quantum defects and wavelengths for all ions
UD
to Ne VIII.
References
h his work
i ssupported in part by the U.S. Department of Energy and the National Science Foundation.
1. H. G. Berry, Rep. Prog. Phys. 12, 5 (1975). -
2.