While other third-row transition metals react more readily with CO, rhenium carbon monoxide is found to be
relatively less stable at both the complete active space multiconfiguration self-consistent field (CASMCSCF)
and the multireference singles + doubles configuration interaction (MRSDCI) computation levels. The
4Σ- state was found to be the ground state for both TcCO and ReCO complexes. Although at the CASSCF
level this state has negative D
e relative to the M(a6S) + CO(1Σ+) dissociation limit (M = Tc or Re), at a
more accurate MRSDCI level, the D
e's of the 4Σ- state were computed as 0.002 eV for TcCO, and 0.012 eV
for ReCO, with respect to the same dissociation limit. Spin−orbit effects for ReCO and TaCO split the
4Σ- nonrelativistic ground state into 1/2 and 3/2 Ω states. The energy difference for the two states is computed
as 981 cm-1. For the TaCO complex, the spin−orbit effects enlarge the energy difference between 4Δ1/2 and
6Σ+
1/2 to 1742 cm-1, compared with 691 cm-1 in the absence of spin−orbit effects. The computed properties
of all M−CO species (M = second- and third-row transition metals) and their nature of bonding for TcCO
and ReCO are discussed. It is shown that the curve crossing of the ground and excited states is an important
factor in the nature of charge transfer in these species. This combined with the extent of charge transfer from
CO to M, and the back transfer from M to CO through π-bonding, is found to be important to result in stable
complexes.