The A 1 P -X 1 S / system of the PN molecule has been reexamined via high resolution conventional spectroscopy, at higher rotational J-values than those in previous studies. It is shown that perturbations occurring in the A 1 P (£ Å 0 to 3) levels give access to information concerning the (e 3 S 0 ,
TheA(3Π1) State of ClF
✍ Scribed by Vadim A. Alekseev; D.W. Setser; Joel Tellinghuisen
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 202 KB
- Volume
- 195
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The A( 3 ⌸ 1 ) state of ClF is studied (1) in emission from the (1 3 P 2 ) ion-pair state in a high-pressure discharge, (2) from its role in perturbations of the B( 3 ⌸ 0 ϩ) and AЈ( 3 ⌸ 2 ) states, and (3) in direct absorption from the X( 1 ⌺ ϩ ) ground state. The last of these is obtained via a UV-labeling technique and represents the first observation of the A 4 X transition. The emission spectrum yields extensive assignments for the 0 -4, 0 -5, and 1-4 bands of  3 A, with both e and f lines identified. The well-known perturbation in v ϭ 7 of the B state is attributed to interaction with v ϭ 9 of A. A newly identified perturbation in B( ) involves coupling with A(8). The known perturbation in B( ) may involve A( ), but other assignments cannot be ruled out. Approximate potential curves are derived for all three valence states and used to compute the vibrational factors for the perturbations, permitting extraction of the electronic coupling strengths. The B-A coupling elements are within ϳ10% of expectations for rotation-electronic coupling within a Hund's case (a) 3 ⌸ manifold, but the strength of the perturbation between A(5) and AЈ( ) is only about 30% of predictions for this model.
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