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Photolysis Production and Spectroscopic Investigation of the Highest Vibrational States in H(2) (X(1)Σ(g)(+)v = 13, 14)

[Image: see text] Rovibrational quantum states in the X(1)Σ(g)(+) electronic ground state of H(2) are prepared in the v = 13 vibrational level up to its highest bound rotational level J = 7, and in the highest bound vibrational level v = 14 (for J = 1) by two-photon photolysis of H(2)S. These states...

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Detalles Bibliográficos
Autores principales: Lai, K.-F., Beyer, M., Salumbides, E. J., Ubachs, W.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2021
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7883349/
https://www.ncbi.nlm.nih.gov/pubmed/33502853
http://dx.doi.org/10.1021/acs.jpca.0c11136
Descripción
Sumario:[Image: see text] Rovibrational quantum states in the X(1)Σ(g)(+) electronic ground state of H(2) are prepared in the v = 13 vibrational level up to its highest bound rotational level J = 7, and in the highest bound vibrational level v = 14 (for J = 1) by two-photon photolysis of H(2)S. These states are laser-excited in a subsequent two-photon scheme into F(1)Σ(g)(+) outer well states, where the assignment of the highest (v,J) states is derived from a comparison of experimentally known levels in F(1)Σ(g)(+), combined with ab initio calculations of X(1)Σ(g)(+) levels. The assignments are further verified by excitation of F(1)Σ(g)(+) population into autoionizing continuum resonances, which are compared with multichannel quantum defect calculations. Precision spectroscopic measurements of the F-X intervals form a test for the ab initio calculations of ground state levels at high vibrational quantum numbers and large internuclear separations, for which agreement is found.