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Electron-density studies of metal–metal bonds. I. The deformation density of V<sub>2</sub>O<sub>3</sub>at 295 K
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1980
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Metal–metal BondsEngineeringV AtomsTheoretical Inorganic ChemistrySolid-state ChemistryChemistryElectronic StructureV2o3 DiffersElectron SpectroscopyMaterials ScienceOxide ElectronicsChemical BondAtomic PhysicsPhysical ChemistryEπ Metal-metal BondQuantum ChemistryElectron-density StudiesTransition Metal ChalcogenidesNatural SciencesApplied PhysicsCondensed Matter PhysicsDeformation Density
The charge-density distribution in V2O3 differs from that in Ti2O3 mainly with respect to the deformation of the metal atoms. The V atoms show a positive deformation of up to 0.1 e Å-3 perpendicular to c in a plane containing three nearest V-atom sites across the edges of the surrounding O-atom octahedra, and a negative deformation of up to 0.3 e Å-3 parallel to c between the nearest V-atom site across the faces of the O-atom octahedra. These observations are in accordance with theoretical band-structure calculations and confirm the existence of an eπ metal-metal bond which is directed across the common edges of the metal-centred O-atom octahedra.