The levels with \(v\) from 1 to 9 in the \((8 d)^{\prime} \Delta_{8}\) state of \(\mathrm{Na}_{2}\) have been observed by means of optical-optical double-resonance (OODR) fluorescence excitation spectroscopy. The intermediate levels in the \(B^{1} \Pi_{u}\) state are justified by numerical calculati
Optical-Optical Double-Resonance Excitation Spectra of the (6d)1Δg and (7d)1Δg Rydberg States in Na2
✍ Scribed by Y.L. Pan; S. Dianping; L.S. Ma; D. Liangen; Z.G. Wang
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 294 KB
- Volume
- 169
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The levels with (v \leqslant 14,27 \leqslant J \leqslant 57) in the ((6 d)^{\prime} \Delta_{g}) and ((7 d)^{\prime} \Delta_{g}) Rydberg states of (\mathrm{Na}{2}) have been observed using optical-optical double resonance (OODR) fluorescence excitation spectroscopy. The intermediate levels in the (B^{1} \Pi{u}) state are identified by numerical calculations with the molecular constants for (B^{1} \Pi_{u} \leftarrow X^{1} \Sigma_{g}^{+})transitions and confirmed by the complementary (A^{\prime} \Sigma_{u}^{+} \leftarrow X^{\prime} \Sigma_{g}^{+})polarization spectra. Absolute vibrational numberings of the ((6 d)^{1} \Delta_{g}) and ((7 d)^{1} \Delta_{g}) states are determined by comparing the observed OODR excitation intensities of transitions ({ }^{1} \Delta_{g} \leftarrow) (B^{\prime} \Pi_{u}) with that of the simulated Franck-Condon factors. The Dunham coefficients and the Rydberg-Klein-Rees (RKR) potential energy curves of the ( (6 d)^{\prime} \Delta_{R}) and (7d) ({ }^{\prime} \Delta_{R}) states are reported. (c) 1995 Academic Press. Inc.
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