An atom-atom partitioning of the (super)molecular Coulomb energy is propose
d on the basis of the topological partitioning of the electron density. Ato
m-atom contributions to the molecular intra- and intermolecular Coulomb ene
rgy are computed exactly, i.e., via a double integration over atomic basins
, and by means of the spherical tensor multipole expansion, up to rank L=l(
A)+l(B)+1=5. The convergence of the multipole expansion is able to reproduc
e the exact interaction energy with an accuracy of 0.1-2.3 kJ/mol at L=5 fo
r atom pairs, each atom belonging to a different molecule constituting a va
n der Waals complex, and for nonbonded atom-atom interactions in single mol
ecules. The atom-atom contributions do not show a significant basis set dep
endence (3%) provided electron correlation and polarization basis functions
are included. The proposed atom-atom Coulomb interaction energy can be use
d both with post-Hartree-Fock wave functions and experimental charge densit
ies in principle. The Coulomb interaction energy between two molecules in a
van der Waals complex can be computed by summing the additive atom-atom co
ntributions between the molecules. Our method is able to extract from the s
upermolecule wave function an estimate of the molecular interaction energy
in a complex, without invoking the reference state of free noninteracting m
olecules. We provide computational details of this method and apply it to (
C2H2)(2); (HF)(2); (H2O)(2); butane; 1,3,5-hexatriene; acrolein and urocani
c acid, thereby covering a cross section of hydrogen bonds, and covalent bo
nds with and without charge transfer. (C) 2001 American Institute of Physic
s.