Abstract
The basis set superposition error is investigated in terms of the first-order symmetry adapted perturbation theory (SAPT). The analysis of the first-order SAPT contribution to the interaction energy reveals the origin of the basis set truncation effects at both the one-electron and many-electron levels of approximation. This helps to formulate the necessary conditions which ensure that the calculated interaction energy is free of the basis set superposition contributions. At the level of the one-electron approximation used for both the interacting system and its subsystems a part of the basis set truncation errors can be eliminated by using what is called the dimer-centred basis set. In order to remove all contributions which arise from the symmetrization of the product of wave functions of the subsystems one needs to redefine their reference states. This means that for the interacting system represented by a single HF determinant, the subsystems must be considered at the level of full CI in the orbital space spanned by all occupied orbitals used to describe the dimer. Then, the interaction energy becomes completely free of the basis set superposition contributions. These general considerations are exemplified by calculations of the first-order SAPT interaction energy in helium and H2 dimers at different levels of approximation for monomers. Also the convergence of the calculated energies to the complete basis set limit is investigated.
Acknowledgement
The authors wish to thank Professors W. Andrzej Sokalski and Grzegorz Chałasiński for discussions and helpful advises.
This work was facilitated by the NSF-EPSCoR grant No. 94-4-756-01 and the NSF-CREST grants No. 9805465 and 9706286. This work does not necessarily reflect the policy of the government and no official endorsement should be inferred.