Relativistic configuration interaction calculations of the low-lying states (O\*(I), 1.2. O\*(H)) arising from I?=' con@uratio? of BiH and the corresponding h-s states ('z-, 1 A. 'E+) are carried out These states are found to be bound and the calculated spectroscopic properties are compared with the
Relativistic configuration interaction calculations on the low-lying electronic states of Hl
โ Scribed by D.A. Chapman; K. Balasubramanian; S.H. Lin
- Publisher
- Elsevier Science
- Year
- 1985
- Tongue
- English
- Weight
- 307 KB
- Volume
- 118
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Relativisuc configuration interaction calculations are described for stx low-lying elertroruc states of J-II. The spearox+ proper~~~ or these states are calculated and compared with available experimental results. 1_ Intioduction The hydrogen iodide molecule has been of considerable experimental and theoretical interest for a number of years [ l-6]_ The reported electronic spectra of HI consist of absorption continua near 46000 cm-l [7] and 23000 cm-l [8], as well as absorption bands which extend from approxunately 55555 cm-l to above the first dissociation limit [ l,S] _ The first ultraviolet continuum is broad and featureless, peaking around 45000 cm-l [6]. Mulliken [3] has assigned this absorption as due to three transitions: the parallel transition l E+ p' + %a', and two per-p endicular transitions 1X& + II1 and lZ& + %I1 [6]. Clear, Riley and Wilson [6] have described photofragmentation spectroscopy studres of HI and DI photolysis at 37550 cm-l in which the absorption continuum is decomposed into contributions from the 31T1, 3n,-,+ and lllr states. Huber and Henberg [9] have assigned these states to an absorption continuum starting at approximately 28000 cm-l with maximum absorption at approxrmately 46000 cm-l The interest in performing relativistic calculations on the HI molecule arises as a result of the large spinorbit interactron present in the iodine atom. The HI molecule has a closed-shell ground state, and promotion of erther a u or rr electron to the antibonding a* orbital leads to 9 X-s states which are split by spin-orbit interaction into 14 w--w states (see table 1) ' Alfred P. Sl-Fellow_
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