Abstract
The electronic structure of the Rh6(CO)16 molecule is discussed within the framework laid down in previous Papers. In contrast to the “rare gas” formalism, by which the molecule appears to have an excess of two electrons, the present approach finds it deficient in two electrons. It is argued that as a consequence of metal–metal interaction an orbital of A2 symmetry (in Td) is destabilised and consequently unoccupied.