posted on 1998-05-12, 00:00authored byDavid E. Root, Mark J. Henson, Tim Machonkin, Pulakesh Mukherjee, T. D. P. Stack, Edward I. Solomon
The four-electron reduction of dioxygen to water by trinuclear
copper clusters is of great biological
significance. Recently we reported the crystal structure of a
trinuclear model complex in which the three
coppers provide the four electrons necessary to fully reduce dioxygen,
generating two μ3-oxo bridges. This
complex is best described as a localized, mixed-valence
Cu(II,II,III) system which has
C2v effective
symmetry.
The magnetic properties of this trinuclear cluster have been
investigated by MCD and SQUID magnetic
susceptibility. The two Cu(II) ions are found to be
ferromagnetically coupled with a triplet/singlet splitting
of
14 cm-1. Density functional calculations
reproduce these geometric, electronic, and magnetic properties
of
the trinuclear cluster and provide insight into their origin.
Since the trinuclear copper complex has a 3+
charge, the Cu3O2 core is one electron too
oxidized to permit each atom to be in a preferred oxidation
state
(2+ for Cu and 2− for O). The extra hole in this highly
oxidized Cu3O2 cluster is found to be localized
on
one Cu, which is therefore a Cu(III) ion, rather than on an O
ligand (which would then be an oxyl) due to the
strong stabilization of the oxo valence orbitals which derives from
bridging to the Cu(II) centers. The
communication between the coppers is weak, as it involves superexchange
through the oxo bridges which
provide nearly orthogonal orbital pathways between the copper ions.
This leads to a ferromagnetic interaction
between the two Cu(II) ions and weak electronic coupling between
the Cu(III) and the Cu(II) ions. In the
idealized D3h high
symmetry limit which would be the favored geometry in the case of
complete electronic
delocalization, the triplet ground state is orbitally degenerate and
subject to a large Jahn−Teller distortion [E‘
⊗ e‘] toward the observed
C2v structure. This
combination of a large Jahn−Teller distortion and weak
electronic
coupling leads to localization of the Cu(III) on one metal
center.