The computational scheme for the evaluation of the second-order electric susceptibility tensor in periodic systems, recently implemented in the CRYSTAL code within the coupled perturbed Hartree–Fock HF scheme, has been extended to local-density, gradient-corrected, and hybrid density functionals coupled-perturbed Kohn–Sham and applied to a set of cubic and hexagonal semiconductors. The method is based on the use of local basis sets and analytical calculation of derivatives. The high-frequency dielectric tensor and second-harmonic generation susceptibility have been calculated with hybrid functionals PBE0 and B3LYP and the HF approximation. Results are compared with the values of and d obtained from previous plane-wave local density approximation or generalized gradient approximation calculations and from experiment. The agreement is in general good, although comparison with experiment is affected by a certain degree of uncertainty implicit in the experimental techniques.

Calculation of the first static hyperpolarizability tensor of 3D periodic compounds with a local basis set. A comparison of LDA, PBE, PBE0, B3LYP and HF results

ORLANDO, Roberto;LACIVITA, VALENTINA;
2010-01-01

Abstract

The computational scheme for the evaluation of the second-order electric susceptibility tensor in periodic systems, recently implemented in the CRYSTAL code within the coupled perturbed Hartree–Fock HF scheme, has been extended to local-density, gradient-corrected, and hybrid density functionals coupled-perturbed Kohn–Sham and applied to a set of cubic and hexagonal semiconductors. The method is based on the use of local basis sets and analytical calculation of derivatives. The high-frequency dielectric tensor and second-harmonic generation susceptibility have been calculated with hybrid functionals PBE0 and B3LYP and the HF approximation. Results are compared with the values of and d obtained from previous plane-wave local density approximation or generalized gradient approximation calculations and from experiment. The agreement is in general good, although comparison with experiment is affected by a certain degree of uncertainty implicit in the experimental techniques.
2010
132
24
244106-1
244106-9
R. Orlando; V Lacivita; R. Bast; K. Ruud
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/133493
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