We have observed the rotational levels in the v ϭ 2, 3, 5, 6, 7, and 8 vibrational manifolds of the 2 1 ⌬ g state of 7 Li 2 via the A 1 ⌺ u ϩ intermediate levels by ⌬⌳ ϭ 2 transitions. This violation of the ⌬⌳ ϭ 0, Ϯ1 selection rule is due to the interaction with the G 1 ⌸ g state. Band-by-band depe
The (2p, 2p) 11Δg State of 6Li2: Fourier Transform Spectrum of the 11Δg-B1Πu Transition
✍ Scribed by C. Linton; F. Martin; P. Crozet; A.J. Ross; R. Bacis
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 461 KB
- Volume
- 158
- Category
- Article
- ISSN
- 0022-2852
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📜 SIMILAR VOLUMES
Large-scale CI calculations are carried out to obtain accurate potential energy surfaces for the . . . g 2 manifold (X 3 ⌺ g Ϫ , 1 1 ⌬ g , 1 1 ⌺ g ϩ ) of electronic states of NCN. Separation of the low-lying singlet states from the triplet ground state is computed in close agreement with the results
The first extensive analysis of the \(a^{1} \mathrm{I}_{\mathrm{g}} \rightarrow a^{\prime} \mathrm{\Sigma}_{u}^{-}-\)system of \({ }^{14} \mathrm{~N}_{2}\) is reported. The spectrum has been recorded by high-resolution Fourier transform spectrometry between 2500 and \(7500 \mathrm{~cm}^{-1}\) using
High-resolution Fourier transform spectra of the laser-induced fluorescence of 63 Cu 37 Cl 2 produced in a cell have been recorded following excitation of a single vibronic level of the E 2 ⌸ u electronic state. Fluorescence occurs in combination bands 1 v1 vЈ 1 2 v2 vЈ 2 3 v3 vЈ 3 to a broad spread
Optical-optical double resonance spectroscopy was used to study the 1 g ( 3 P 1 ) ion-pair state of I 2 correlating to I -( 1 S) + I + ( 3 P 1 ) at the dissociation limit. We gained access to the 1 g ( 3 P 1 ) state though the A 3 (1 u ) state in the (1 + 1) photon-excitation scheme. The pump laser
We report the analysis of the H1 u ( 3 P 1 ) state of I 2 by optical-optical double resonance. This state lies in the second tier of ion-pair states and its observation was achieved by using the (1 ϩ 2) photoexcitation sequence using the A 3 ⌸ 1u state as an intermediate. The molecular parameters we