𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Second-order Møller-Plesset perturbation theory calculations with relativistic effective core potentials including spin-orbit operators

✍ Scribed by Sang Yeon Lee; Yoon Sup Lee


Publisher
Elsevier Science
Year
1991
Tongue
English
Weight
584 KB
Volume
187
Category
Article
ISSN
0009-2614

No coin nor oath required. For personal study only.

✦ Synopsis


The two-component Hartree-Fock method using relativistic effective core potentials (RECP) is extended to include electron correlations by second-order Moller-Plesset perturbation theory (MPZ). The present method simultaneously treats electron correlation and all the relativistic effects in REP including spin-orbit effects. It is possible to estimate differential correlation effects on molecular properties due to the relativity and/or the spin-orbit interactions at the MP2 level using the present method. Test calculations have been performed for HX, X2, XY (X, Y = Br, I), and PbHl molecules. Spin-orbit and electron-correlation effects are rather small for the equilibrium bond lengths and dissociation energies of the tested molecules, but exhibit interesting trends.


📜 SIMILAR VOLUMES


Kramers' unrestricted Hartree–Fock and s
✍ Yong Suk Kim; Sang Yeon Lee; Won Seok Oh; Bo Hyun Park; Young Kyu Han; Su Jin Pa 📂 Article 📅 1998 🏛 John Wiley and Sons 🌐 English ⚖ 181 KB 👁 1 views

The Kramers' restricted Hartree᎐Fock KRHF and second-order Ž . Møller᎐Plesset perturbation KRMP2 methods using relativistic effective core potentials Ž . RECP with spin᎐orbit operators and two-component spinors are extended to the unrestricted forms, KUHF and KUMP2. As in the conventional unrestrict

Relativistic and electron-correlation ef
✍ Terutaka Yoshizawa; Masahiko Hada 📂 Article 📅 2009 🏛 John Wiley and Sons 🌐 English ⚖ 179 KB

## Abstract Isotropic and anisotropic magnetizabilities for noble gas atoms and a series of singlet and triplet molecules were calculated using the second‐order Douglas‐Kroll‐Hess (DKH2) Hamiltonian containing the vector potential **A** and in part using second‐order generalized unrestricted Møller