Formulae in terms of integrals and orbital energies are presented for
the evaluation of the second-, third- and fourth-order energies in ope
n-shell spin-restricted Moller-Plesset (RMP) perturbation theory. The
performance of RMP theory is evaluated by calculating equilibrium stru
ctures and harmonic vibrational frequencies of a large number of open-
shell systems and by calculating energies of reactions which have been
shown to be poorly described by spin-unrestricted Moller-Plesset (UMP
) theory. RMP theory removes the spin contamination present in the unr
estricted Hartree-Fock (UHF) reference of UMP theory. In cases where t
he spin contamination gives rise to large errors in UMP calculations,
such as for the harmonic frequencies of NO, CN, CO+ and FO2 and the en
ergies of reactions involving CN and FO2, RMP theory is shown to offer
a substantial improvement. In cases where the Moller-Plesset series e
xhibits large oscillations, such as for O2, O2+ and F2+, RMP theory is
shown to offer no improvement over UMP theory; in these cases good re
sults are achieved with higher-order methods such as quadratic configu
ration interaction and coupled-cluster theory.