Abstract
In the quantum theory of intermolecular forces, emphasis usually falls on long-range effects such as the dispersion interactions. At shorter range the electron distributions begin to overlap appreciably, serious non-orthogonality problems arise, and the nature of the interactions is less well understood. This paper is devoted to a general analysis of the short-range interactions between any pair of electronic systems, A and B, in states of arbitrary spin multiplicity and described by wavefunctions of arbitrarily high accuracy. The interaction energy is developed as a series of terms associated with interchange of 0, 1, 2, . . . electrons (arising from the use of a fully antisymmetric wave function): the final expression is written as a power series in the expectation value of the spin scalar product S
A
·S
B
, with numerical coefficients which are determined by the electron density, spin density, etc., of the separate systems. Numerical results are presented for two neon atoms (the closed-shell case, with spins
S
A
=
S
B
= 0) and for two nitrogen atoms (open shells with
S
A
=
S
B
= 3/2). The results, obtained from the use of one-determinant wavefunctions for the separate systems, are in good agreement with the best results so far available.
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