The nature of the Ga−Ga bond in the naked dianion PhGaGaPh2- and its Na+-coordinated
counterpart is discussed using the recently proposed formalism based on the analysis of
domain-averaged Fermi holes. The analysis shows clearly that three electron pairs, i.e., two
σ and one π, contribute to the Ga−Ga bonding interactions in the free dianion PhGaGaPh2-
and in the sodium-complexed species (PhGaGaPh)Na2. The eigenvalues and the eigenvectors
of the Fermi hole indicate, however, that the Ga−Ga bonding situation does not correspond
to classical triple bonds and should not be interpreted using classical bonding models. The
reason is that only one of the three electron pairs involved in Ga−Ga bonding, namely that
contributing to the Ga−Ga π bond, corresponds to an “ordinary” shared electron pair bond
in the sense of Lewis. The bonding interactions of the other two pairs are much more complex
and have no classical counterparts. The eigenvalues and the eigenvectors of the latter Fermi
holes cannot be considered as fully bonding, but they have partial lone-pair character. This
is why the calculated bond orders yield values which are close to a weak double bond.
Essentially the same bonding picture holds also for the Na+-coordinated species, but the
coordination of sodium causes further weakening of the contributions of all three electron
pairs to the Ga−Ga bonding. This weakening yields an effective reduction of the multiplicity
of the Ga−Ga bond. The calculated bond order therefore has a value which is otherwise
typical for single bonds.
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