DFT calculations
have been carried out for coordinatively saturated
neutral and charged carbonyl complexes [M(CO)
n
]
q
where M is a metal atom of groups
2–10. The model compounds M(CO)
2
(M = Ca, Sr, Ba)
and the experimentally observed [Ba(CO)]
+
were also studied.
The bonding situation has been analyzed with a variety of charge and
energy partitioning approaches. It is shown that the Dewar–Chatt–Duncanson
model in terms of M ← CO σ-donation and M → CO
π-backdonation is a valid approach to explain the M–CO
bonds and the trend of the CO stretching frequencies. The carbonyl
ligands of the neutral complexes carry a negative charge, and the
polarity of the M–CO bonds increases for the less electronegative
metals, which is particularly strong for the group 4 and group 2 atoms.
The NBO method delivers an unrealistic charge distribution in the
carbonyl complexes, while the AIM approach gives physically reasonable
partial charges that are consistent with the EDA-NOCV calculations
and with the trend of the C–O stretching frequencies. The AdNDP
method provides delocalized MOs which are very useful models for the
carbonyl complexes. Deep insight into the nature of the metal–CO
bonds and quantitative information about the strength of the [M] ←
(CO)
8
σ-donation and [M(d)] → (CO)
8
π-backdonation visualized by the deformation densities are
provided by the EDA-NOCV method. The large polarity of the M–CO
π orbitals toward the CO end in the alkaline earth octacarbonyls
M(CO)
8
(M = Ca, Sr, Ba) leads to small values for the delocalization
indices δ(M–C) and δ(M···O) and
significant overlap between adjacent CO groups, but the origin of
the charge migration and the associated red-shift of the C–O
stretching frequencies is the [M(d)] → (CO)
8
π-backdonation.
The heavier alkaline earth metals calcium, strontium and barium use
their s/d valence orbitals for covalent bonding. They are therefore
to be assigned to the transition metals.