We rely on a finite-field approach to calculate the static dipole ((u) and quadrupole ( C) polarizability and the first (/3) and second ( y) dipole hyperpolarizability of methane. Our best, CCSD( T) values for LY, /II and the mean value of y and C, obtained at&=2.052 aowitha (lls7p4d2f/6s2pld)[6s4p4
A fourth-order many-body perturbation theory calculation of the first and second electric dipole hyperpolarizability of ammonia
β Scribed by George Maroulis
- Publisher
- Elsevier Science
- Year
- 1992
- Tongue
- English
- Weight
- 517 KB
- Volume
- 195
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
β¦ Synopsis
The electric dipole moment (p,), dipole polarizability (CQ) and first (Balk) and second (v,,& dipole hyperpolarizability of ammonia were obtained from finite-field self-consistent-field (SCF) and complete fourth-order many-body perturbation theory (MP4) calculations. With z as the C, axis, the following SDQ-MP4 results are reported: pLr= -0.6034 e u,,, at= 14.0 1 and Aa = 1.59 e* al EL', jk30.47 and A/3=8.87 e3 aa EC', y=3864 e4 at E,$. The triples (T4) contribution to the fourth-order correction for the above properties is estimated to be 0.0083 e a,,, 0.29 and 0. 25 e2 a,$ E;',4.42 and 5.43 e3 ai EC', 311 e4 ai Eh3, respectively.
π SIMILAR VOLUMES
The second-order multireference perturbation theory employing multiple partitioning of the many-electron Hamiltonian into a zero-order part and a perturbation is formulated in terms of many-body diagrams. The essential difference from the standard diagrammatic technique of Hose and Kaldor concerns t
The QED-MP2 model based on the quasi-energy derivative method in the second-order Moller-Plesset perturbation theory is formulated, and frequency-dependent (dynamic) polarizabilities [a(-w; o~)] for H20 and NH3 are calculated. Dynamic polarizabilities obtained for HzO agree with experimental values.