Recently, two different but conceptually similar basis set Ž . superposition error BSSE free second-order perturbation theoretical schemes were developed by us that are being based on the chemical Hamiltonian Ž . approach CHA . Using these CHA-MP2 and CHA-PT2 methods, a comparison is made between th
Comparative study of errors in HeH− interaction energy calculations
✍ Scribed by A. S. Shalabi; Kh. M. Eid; M. A. Kamel; A. A. El-Barbary
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 205 KB
- Volume
- 68
- Category
- Article
- ISSN
- 0020-7608
No coin nor oath required. For personal study only.
✦ Synopsis
Basis set truncation error BSTE , size extensivity Error SEE , zero point Ž . Ž . y vibrational energy ZPVE , and basis set superposition error BSSE of HeH weak van der Waals interaction energy were determined and compared at the self-consistent field Ž . Ž .
Ž . SCF , many-body perturbation theory MBPT , and coupled cluster CC methods using even-tempered functions. Isotope substitution effects and the role of bond function Ž . augmentation were taken into account. Apart from core correlation energy error CCEE , which is absent from HeH y interaction energy, the results confirm that BSTE is the most Ž . important source of error, followed by SEE of the truncated configuration interaction CI expansion, ZPVE and BSSE in a descending order. Introducing quadrable excitations to the truncated CI expansion reduces the magnitude of SEE by ; 45.7%, and BSSE correction is not necessary even at the electron correlation level. While bond function augmentation reduces BSSE at the Hartree᎐Fock, it has an oscillating behavior at the electron correlation level.
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