Rovibrational Spectra of LiH2 +, LiHD+ and LiD2 + Determined from FCI Property Surfaces

Full configuration interaction (FCI) has been used in conjunction with the lithium [6s5p3d1f] (Iron, M. A.; et al. Mol. Phys. 2004, 101, 1345) and hydrogen aug-cc-pVTZ basis sets to construct an 83-point potential energy surface of the 1A1 ground state of 7LiH2 +. Vibrational and rovibrational wave...

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Published inThe journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Vol. 111; no. 20; pp. 4478 - 4488
Main Authors Page, Alister J, von Nagy-Felsobuki, Ellak I
Format Journal Article
LanguageEnglish
Published United States American Chemical Society 24.05.2007
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Summary:Full configuration interaction (FCI) has been used in conjunction with the lithium [6s5p3d1f] (Iron, M. A.; et al. Mol. Phys. 2004, 101, 1345) and hydrogen aug-cc-pVTZ basis sets to construct an 83-point potential energy surface of the 1A1 ground state of 7LiH2 +. Vibrational and rovibrational wave functions of the6,7LiH2 +, 6,7LiHD+, and 6,7LiD2 + ground states were calculated variationally using an Eckart−Watson Hamiltonian. For 7LiD2 +, rovibrational transition frequencies for K = 0, 1, 2 and J ≤ 10 are within ca. 0.1% of recent experimental values (Thompson, C. D.; et al. J. Chem. Phys. 2006, 125, 044310). A 47-point FCI dipole moment surface was embedded in the rovibrational Hamiltonian to calculate vibrational and rovibrational radiative properties. At 296 K, with v ≤ 4 and J ≤ 4, the 202 ← 303 rotational transition in the |001〉 band was found to have the greatest spectral intensity with respect to the ground electronic states of 6,7LiH2 +, 6,7LiHD+, and 6,7LiD2 +. In each case, the most intense rovibrational transitions have been assigned unequivocally using the J, K a, K c assignment scheme.
Bibliography:ark:/67375/TPS-CQM56R0D-C
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ObjectType-Article-1
SourceType-Scholarly Journals-1
ObjectType-Feature-2
content type line 23
ISSN:1089-5639
1520-5215
DOI:10.1021/jp066369d