Kohn-Sham (KS) and Hartree-Fock (HF) determinants were used as the true man
y-body wave functions for calculations of molecular energies, vibrational f
requencies, and excited electronic states. The results justified common pra
ctice, encountered in the sum over states theories, in which these two dete
rminants are used as the first-order approximation of the wave function. Ho
wever, a distinct behavior with respect to the second-order perturbation ca
lculation was observed for the two cases. The Raleigh-Schrodinger perturbat
ion theory, which is formally identical to the Levy-Gorling formalism and a
nalogous to the usual HF/Moller-Plesset approach, leads to rather discourag
ing results for the KS determinant. On the other hand, the rigid KS orbital
s are more suitable for modeling of excited electronic states, which was in
dicated by the obtained transition energies for model molecules. (C) 2000 J
ohn Wiley & Sons, Inc.