Perturbations in the A 1Π- X 1Σ+ system of the BeS molecule. The a 3Π i state
Identifieur interne : 004073 ( Main/Exploration ); précédent : 004072; suivant : 004074Perturbations in the A 1Π- X 1Σ+ system of the BeS molecule. The a 3Π i state
Auteurs : B. Pouilly [France] ; J. M. Robbe [France] ; J. Schamps [France] ; R. W. Field [États-Unis] ; L. Young [États-Unis]Source :
- Journal of Molecular Spectroscopy [ 0022-2852 ] ; 1982.
Abstract
The states responsible for all perturbations observed by Cheetham et al. [Trans. Faraday Soc. 61, 1308–1316 (1965)] in the BeS A1Π-X1Σ+ system were electronically (a3Π2, a3Π1, and X1Σ+) and vibrationally assigned. Cheetham et al. had incorrectly suggested that perturbations presently assigned as A1Π(vA) ∼ a3Π2(va = vA + 2) were A1Π ∼ 1Δ. Molecular constants for the newly identified a3Πi state, which is the lowest energy excited state of BeS, as well as electronic parameters for A ∼ X, A ∼ a, and a ∼ X interactions were determined. Principal constants (in cm−1) for A1Π and a3Π are a3Π A1Π Te 7 100 (75) 7 961.64 (26) ωe 737 (5) 762.13 (7) ωeχe 4.1 (2) 4.09 (4) re(A ̊) 1.9190 (10) 1.9087 (2) (1σ uncertainties in parentheses). A coherent picture of the perturbations in A1Π could be drawn only by combining fragmentary spectroscopic data from Cheetham et al. with new ab initio calculations of spin-orbit and rotation-electronic perturbation parameters, spin-orbit splittings, and energy separations of isoconfigurational a3Π and A1Π states.
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DOI: 10.1016/0022-2852(82)90213-2
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<front><div type="abstract" xml:lang="en">The states responsible for all perturbations observed by Cheetham et al. [Trans. Faraday Soc. 61, 1308–1316 (1965)] in the BeS A1Π-X1Σ+ system were electronically (a3Π2, a3Π1, and X1Σ+) and vibrationally assigned. Cheetham et al. had incorrectly suggested that perturbations presently assigned as A1Π(vA) ∼ a3Π2(va = vA + 2) were A1Π ∼ 1Δ. Molecular constants for the newly identified a3Πi state, which is the lowest energy excited state of BeS, as well as electronic parameters for A ∼ X, A ∼ a, and a ∼ X interactions were determined. Principal constants (in cm−1) for A1Π and a3Π are a3Π A1Π Te 7 100 (75) 7 961.64 (26) ωe 737 (5) 762.13 (7) ωeχe 4.1 (2) 4.09 (4) re(A ̊) 1.9190 (10) 1.9087 (2) (1σ uncertainties in parentheses). A coherent picture of the perturbations in A1Π could be drawn only by combining fragmentary spectroscopic data from Cheetham et al. with new ab initio calculations of spin-orbit and rotation-electronic perturbation parameters, spin-orbit splittings, and energy separations of isoconfigurational a3Π and A1Π states.</div>
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