Two mechanisms for the predissociation of the C 2X: state of N$ ar8 discussed -the accidentai mechanism nnd a direct, homogeneous process C -f B 'c:. The matrix elements for the latter channel are dominated by a contribution from the nuclear kinetic energy operator, containing a Fran&-Condon integra
Excited states of gaseous ions. Transitions to and predissociation of the C2Σ+u state of n+2
✍ Scribed by J.C. Lorquet; M. Desouter
- Publisher
- Elsevier Science
- Year
- 1972
- Tongue
- English
- Weight
- 470 KB
- Volume
- 16
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
ii configuration interaction study of different electronic states of IQ; has been perkmned. The position in cncrsy and the refati;e $rtensity of the photoe!ectron bands of the "Zi 4 states has been calculated and cumpared ivith espariment. The C-X:, state is predissoc~te~ by a U, state, as previously suppo.sed. However, owins to the attractive nature of the '%'I,, state a ciuuble crossinp occurs. Several predissociation mechanisms of the C state can therefore take place; thcP Efctimcs have ken calm&ted.
Our interest in the excited states of the 8; ion de& with two specific problems concerning the C2c~ state: the activity of this state in the photoelectron spectrum and its predissociatiun properties. We shall consider these two Points successively. 2. ne photoeLectron spectru.m Edqvist et al. have stated [l] that the C2Z: state of% was undetectable in photoelectron spectroscopy. A similar statement was also made by Potts [2]. This situation may be understood since the predominant electronic configurarion of the electronic structure of the C state is: r$ c%; . ..@Q (3tTy)t &r$ ('Q 111 and differs then from that of the ground state of the neutrai nrolecufe by two ntolecuIar orbit&, N2 XlSi . ..~?ouj2(3~~)~(ll.,)'~ . ('-1 On the other tiand, the 5 state of NG q_ 52c:...(=*~)l(j"gjl?(i,u)?! (3) 136 .' '.
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📜 SIMILAR VOLUMES
The large isotopic effect recently found in the decay of the C 'Cc state of Nf is interpreted by an indirect (accidental) predissociation mechanism. The C \*X; state interacts with a bound intermediate state, itself predissociated by a repulsive state. The competition between fluorescence and predis