Two new bimetallic complexes, [Cp*2Yb]2(μ-1,3-(2,2‘-bipyridyl)-5-tBu-C6H3) (1) and [Cp*2Yb]2(μ-1,4-(2,2‘-bipyridyl)-C6H4) (2), and their corresponding two-electron oxidation products [1]2+ and [2]2+
have been synthesized with the aim of determining the impact of the bridging ligand geometry on the
electronic and magnetic properties of these materials. Electrochemistry, optical spectroscopy, and bulk
susceptibility measurements all support a ground-state electronic configuration of the type [(f)13-(πa*)1-(πb*)1-(f)13]. Density functional theory calculations on the uncomplexed bridging ligands as doubly reduced
species also indicate that the diradical electronic configuration is the lowest lying for both meta- and
para-bis(bipyridyl) systems. The electrochemical and optical spectroscopic data indicate that the electronic
coupling between the metal centers mediated by the diradical bridges is weak, as evidenced by the small
separation of the metal-based redox couples and the similarity of the f−f transitions of the associated
dicationic complexes ([1]2+ and [2]2+) relative to those of the monometallic [Cp*2Yb(bpy)]+ analogue.
The magnetic susceptibility data show no evidence for exchange coupling between the paramagnetic
metal centers in the neutral complexes, but do indicate weak exchange coupling between YbIII and ligand
radical spins on each of the effectively independent halves of the bimetallic complexes. These findings
are in contrast to those reported recently for CoIII/II dioxolene bimetallic complexes bridged by these
same bis(bipyridyl) ligands. The difference is attributed in part to the dominant singlet diradical character
of the bridging ligands in the ytterbocene complexes. These experimental and theoretical results are
consistent with expectations for organic diradical spin orientations for meta versus para substituents
across a phenylene linker, but this effect does not induce significant longer-range superexchange or
electronic interactions between the metal centers in these systems.