2006
DOI: 10.1016/j.cplett.2005.10.023
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Dipole and quadrupole (hyper)polarizability for the asymmetric stretching of carbon dioxide: Improved agreement between theory and experiment

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Cited by 33 publications
(27 citation statements)
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“…31 The denominator factor u LR (R e , θ ) is the same function evaluated at R e = R e (θ ). The other coefficients for excited states are fixed by C 0,υ 3 =1 6 and the ratio C n,υ 3 =0 λ /C 0,υ 3 =0 6 at the ground state of CO 2 .…”
Section: A Potential Energy Surfacementioning
confidence: 99%
“…31 The denominator factor u LR (R e , θ ) is the same function evaluated at R e = R e (θ ). The other coefficients for excited states are fixed by C 0,υ 3 =1 6 and the ratio C n,υ 3 =0 λ /C 0,υ 3 =0 6 at the ground state of CO 2 .…”
Section: A Potential Energy Surfacementioning
confidence: 99%
“…Without entering into further detail on this issue, it is worthwhile noting that this value was found to be in excellent agreement with refined calculations for the isotropic spectrum, but also to match, in order of magnitude, the result reported in the sole prior study of this overtone. To this end, intermode coupling, involving the two stretching vibrations ν 1 and ν 3 , and anharmonicity effects (electro-optical and mechanical) had to be incorporated, along with quality ab initio data 25,26 for the polarizability anisotropy derivatives. 24 In Secs.…”
Section: B Symmetriesmentioning
confidence: 99%
“…This surface is usually expressed as a Taylor series on the vibrational coordinates. The polarizability derivatives can be determined from ab initio calculations [18,19] or, more frequently, empirical values can be obtained from a fit to experimental transition moments [6,20].…”
Section: The Calculated Raman Spectrummentioning
confidence: 99%