1981
DOI: 10.1080/00268978100101831
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The quadrupole moments of carbon dioxide and carbon disulphide

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Cited by 95 publications
(33 citation statements)
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“…In this communication, we study relativistic effects on the Buckingham birefringence for the series of molecules CX 2 (X = O, S, Se, Te). For CO 2 , CS 2 and CSe 2 , we compare our results with previous nonrelativistic ab initio [17] data and with experiment [29][30][31][32][33][34]. The atomic-orbital-driven (AO-driven) scheme recently introduced by Bast et al [35] for calculating time-dependent molecular properties with one-, two-and four-component relativistic methods is extended to first-order frequency-dependent magnetic perturbations with London atomic orbitals (LAOs) [36][37][38][39][40], thereby ensuring gaugeorigin independence of the calculated results.…”
mentioning
confidence: 58%
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“…In this communication, we study relativistic effects on the Buckingham birefringence for the series of molecules CX 2 (X = O, S, Se, Te). For CO 2 , CS 2 and CSe 2 , we compare our results with previous nonrelativistic ab initio [17] data and with experiment [29][30][31][32][33][34]. The atomic-orbital-driven (AO-driven) scheme recently introduced by Bast et al [35] for calculating time-dependent molecular properties with one-, two-and four-component relativistic methods is extended to first-order frequency-dependent magnetic perturbations with London atomic orbitals (LAOs) [36][37][38][39][40], thereby ensuring gaugeorigin independence of the calculated results.…”
mentioning
confidence: 58%
“…As discussed for linear birefringences elsewhere [8][9][10][11], this difficulty arises from the extreme sensitivity of the infinite-temperature extrapolation performed on the experimental data to estimate b(x). From comparison with experimentally derived data, it is therefore not possible to draw definite conclusions regarding the reliability of the various XC functionals for the mixed hyperpolarizabilities that determine the [29,30,34] have been included. For C, O and S we have used the u-aug-cc-pVDZ and u-aug-cc-pVTZ (''u-'' meaning uncontracted) basis sets of Dunning [90,91], for Se and Te the augmented allelectron u-DZ and u-TZ basis sets of Dyall [92,93].…”
Section: The Temperature-independent Part Of the Buckingham Birefringmentioning
confidence: 99%
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