On Fe–Fe Dumbbells in the Ideal and Real Structures of FeGa₃

The intermetallic phase FeGa₃ belongs to the rare examples of substances with transition metals where semiconducting behavior is found. The necessary electron count of 17 ve/fu can be formally derived from eight Fe–Ga and one Fe–Fe two-center–two-electron bond. The situation is reminiscent of the well-known Fe₂(CO)₉ scenario, where a direct Fe–Fe two-center–two-electron bond was shown to not be present. Fe–Fe interaction in FeGa₃ and its substitution variants represents the crucial point for explanation of electronic, thermal transport, and optical properties of this material. Chemical bonding analysis in position space of FeGa₃ and Fe₂(CO)₉ on the basis of the topology of the electron localizability indicator distribution, QTAIM atoms, two- and three-center delocalization indices, domain natural orbitals, IQA analysis, and an evaluation of the Fe–Fe dissociation energy yields a complete picture of the partially compensated Fe–Fe bond, which is nevertheless strong enough to be of decisive importance. Structural reinvestigation of differently synthesized single crystals leads to the composition Fe_1+xGa₃ (0 ≤ x ≤ 0.018), where the additional Fe atoms are predicted from DFT/PBE calculations to yield a magnetic moment of about 2 μ_B/Fe2 atom and metallic in-gap states. Accompanying magnetization and ESR measurements are consistent with this picture.