The SCF perturbative method de&eloped for the calculation of static pohrizabilities is extended to the frequency-dependent case. Calcuhtions are reported for helium and methane. The helium results are compared \vith those of other x+orkers.
Calculation of frequency-dependent polarizabilities using coupled-cluster response theory
✍ Scribed by Rika Kobayashi; Henrik Koch; Poul Jφrgensen
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 506 KB
- Volume
- 219
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
✦ Synopsis
Coupled-cluster singles and doubles linear response (CCLR) calculations have been presented for frequency-dependent dipole polarizabilities and the results compared with the results from a CI-like approach to the equation of motion (EOMCC). The frequency-dependent polarizabilities are similar in the two approaches for single molecule calculations on small systems. However, the CCLR approach gives size-extensive polarizabilities, whereas the EOMCC approach does not. EOMCC calculations can therefore give unphysical polarizabilities, e.g. EOMCC calculations on a sequence of non-interacting LiH systems gave a negative polarizability for 20 or more non-interacting LiH systems. The CCLR approach is shown to be an attractive "black box" approach for the calculation of accurate frequency-dependent polarizabilities.
📜 SIMILAR VOLUMES
## Abstract Time‐dependent coupled cluster theory, with unrestricted electron spins and full treatment of orbital rotation, is used to calculate polarizabilities at imaginary frequencies for Li, Ar, HCl, CO, N~2~, O~2~, and H~2~O, and to obtain dispersion energy coefficients for their pair interact
We propose and implement in this paper a highly correlated method for computing dynamic polarizability of closed-shell atoms and molecules and the van der Waals coefftcient C, of atoms within the framework of coupled cluster based linear response theory (CC-LRT). Excitation energies (EE), oscillator
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.
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
We extended the dynamic response theory in the Møller᎐Plesset Ž . Ž . perturbation theory MPPT based on the quasi-energy derivative QED method for closed-shell systems to that for open-shell systems. In this study we perform the Ž . calculations of frequency-dependent polarizabilities ␣ y; for nonde