کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
---|---|---|---|---|
5372969 | 1504193 | 2016 | 14 صفحه PDF | دانلود رایگان |
- CO2â¯Rg, Rg = He, Ne, Ar, Kr and Xe complexes.
- High-level ab initio calculations.
- Purpose-oriented Gaussian basis sets are used on CO2 and Rg.
- Interaction-induced dipole moment.
- Interaction-induced dipole (hyper)polarizability.
We have obtained a quantitative, synthetic picture of the interaction-induced (hyper)polarizability in the sequence of the weakly bound complexes CO2â¯Rg, Rg = He, Ne, Ar, Kr, Xe. The properties are calculated from finite-field Møller-Plesset perturbation theory and coupled cluster calculations. We rely on flexible, prepared purpose-oriented atom- and molecule-specific basis set of Gaussian-type functions. We obtained interaction-induced electric properties for both the most stable T-shaped configuration and the less stable L-shaped one. Our interaction-induced first and second hyperpolarizabilities for the most stable (T-shaped) configurations, at the second order Møller-Plesset perturbation theory level are β¯int/e3a03Eh-2 (CO2â¯Rg) = 1.14 (He), 2.02 (Ne), 2.50 (Ar), 0.50 (Kr) and â5.32 (Xe). For the second hyperpolarizability at the same level of theory γ¯int/e4a04Eh-3 (CO2â¯Rg) = â11.66 (He), â25.88 (Ne), â108.16 (Ar), â206.75 (Kr) and â460.42 (Xe). In the vicinity of the equilibrium configuration, with the Rg atom displaced on the x axis for T-shaped configuration, the first hyperpolarizability changes as dβ¯dRee3a02Eh-2 (CO2â¯Rg) = â1.07 (He), â1.86 (Ne), â0.71 (Ar), 2.65 (Kr) and 9.96 (Xe). For the second hyperpolarizability dγâ¾dRee4a03Eh-3 (CO2â¯Rg) = 7.94 (He), 20.34 (Ne), 65.00 (Ar), 118.48 (Kr) and 239.84 (Xe).
Journal: Chemical Physics - Volume 475, 22 August 2016, Pages 90-103