The reactions of Cd(S-1:5s(2), P-3,P-1:5s(1)5p(1)) and Hg(S-1:6s(2), P-3,P-
1:6s(1)6p(1)) with SiH4 have been studied through multiconfiguration self-c
onsistent-field (MCSCF) (with relativistic effective core potentials) follo
wed by extensive variational and perturbational second-order multireference
Moller-Plesset configuration interaction by perturbation selected by itera
tive process (CIPSI) calculations using extended Gaussian basis sets. It wa
s found that both metal atoms in their P-3(ns(1)np(1)) state break the Si-H
bond of silane spontaneously, leading directly to the MH + SiH3 final prod
ucts, in agreement with the experimental results of this reaction for Cd. O
ne important qualitative difference between the Cd and Hg(P-3) reactions is
that for the former an unstable intermediate was found, whereas for the la
tter no intermediate exists at all. Again, for both atoms, the P-1(ns(1)np(
1)) state is also inserted in the Si-H bond and the corresponding interacti
on surface shows an avoided crossing with the lowest-lying X (1)A' potentia
l surface, adiabatically correlated with the M(S-1:ns(2)) + SiH4 reactants.
This interaction leads eventually to the MH + SiH3 products. The structure
of these HMSiH3 intermediates, diabatically correlated with the M(P-1:ns(1
)np(1)) + SiH4 reactants, was carefully studied, as well as the dissociatio
n channels leading to the MH + SiH3 and H + MSiH3 products. Accurate energy
differences between all these species are also reported. The theoretical r
esults obtained for the mercury reaction are discussed in light of the very
recent experimental results of Legay-Sommaire and Legay [J. Phys. Chem. A
102, 8579 (1998)] for the insertion of Hg(P-3:4s(1)4p(1)) in SiH4 over N-2
and rare gas matrices. Our results confirm their conclusion that the photoc
hemical insertion of Hg(P-3) into the Si-H bond of silane proceeds without
any activation barrier. (C) 1999 American Institute of Physics. [S0021-9606
(99)30322-6].