Rotational line strengths in4Σ-4Π transition of diatomic molecules

Pramana ◽  
1985 ◽  
Vol 24 (3) ◽  
pp. 503-512
Author(s):  
T K Balasubramanian ◽  
V P Bellary
1973 ◽  
Vol 51 (12) ◽  
pp. 1300-1301 ◽  
Author(s):  
J. L. Féménias ◽  
C. Athénour ◽  
R. Stringat

Van Vleck's RAM method is used for calculating rotational line strengths in electric dipole transitions between electronic states of diatomic molecules arising from coupling cases which involve the nuclear spin.


1980 ◽  
Vol 60 ◽  
pp. 147-150
Author(s):  
I. Kcvács ◽  
I. Péczeli ◽  
A. Grandfiterre

1992 ◽  
Vol 97 (5) ◽  
pp. 2891-2899 ◽  
Author(s):  
Jinchun Xie ◽  
Richard N. Zare

1971 ◽  
Vol 49 (21) ◽  
pp. 2693-2703 ◽  
Author(s):  
J. B. Tatum ◽  
J. K. G. Watson

Rotational line strengths (Hönl–London factors) are calculated for 3Σ±–3Σ± electric dipole transitions, allowing for nonzero values of the splitting constant λ. If the 3Σ states are intermediate between Hund's coupling cases (a) and (b) only one transition moment is required, whereas if there is a tendency to case (c) four transition moments may be required. The resulting formulas are compared with the observed spectra of the diatomic molecules of the Group VI elements. The same formulas are valid for 3Σ±–3Σ± magnetic dipole transitions.


1984 ◽  
Vol 62 (12) ◽  
pp. 1610-1615 ◽  
Author(s):  
U. Sassenberg ◽  
A. S.-C. Cheung ◽  
A. J. Merer

Detailed calculations of the line strengths in a 5Σ – 5Π transition as a function of J show that the relative branch intensities in the A – X system of CrO, which do not follow the published formulae for 5Σ(b) – 5Π(a) transitions, can be explained very well in terms of strong spin uncoupling in the 5Π state, with a single perpendicular transition moment dominating. It is emphasized that spin uncoupling affects line strengths by an amount that increases very rapidly with multiplicity, so that algebraic formulae for the pure coupling cases quickly lose their value. An unusual cancellation effect occurs in the main branches of a 5Σ – 5Π transition, nine of which have intensities that drop to zero and then rise again with increasing J.


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