is checked for its ability to reproduce the experimental continuum of the Na 2 4 3 g (v = 12, N = 23) → a 3 + u bound-free transition observed by G. Lazarov, A. M. Lyyra, Li Li, and J. Huennekens (J. Mol. Spectrosc. 196, 259 (1999)). A significant difference between the experimental and simulated bo
The 43Πg State of Na2: Vibrational Numbering and Hyperfine Structure
✍ Scribed by G. Lazarov; A.M. Lyyra; Li Li; J. Huennekens
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 116 KB
- Volume
- 196
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The Na 2 4 3 ⌸ g state has been studied by continuous-wave (cw) perturbation-facilitated optical-optical double resonance (PFOODR) fluorescence excitation and resolved fluorescence spectroscopy. The absolute vibrational numbering was determined by resolved fluorescence to the a 3 ⌺ u ϩ state. The OODR excitation lines of the
vЉ, JЉ) transitions show hyperfine splittings, and the hyperfine coupling scheme of the upper 4 3 ⌸ g levels is case b S . Although this 4 3 ⌸ g state dissociates to the 3p ϩ 3p atomic limit, it is a Rydberg state at a small internuclear distance, and the hyperfine splitting is caused mainly by the Fermi contact interaction of the g 3s valence electron with the nuclei. The Fermi contact constant was determined to be b F ϭ 218.3 Ϯ 3.9 MHz.
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