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Metal−Metal Bonding and Correlated Metallic Behavior in the New Deficient Spinel Ga<sub>0.87</sub>Ti<sub>4</sub>S<sub>8</sub>
28
Citations
14
References
2008
Year
EngineeringTheoretical Inorganic ChemistryChemistryElectronic StructureTransition Metal ClustersMetal−metal BondingTransition Metal AtomsMaterials ScienceInorganic ChemistryMaterials EngineeringCrystalline DefectsChemical BondMetallurgical InteractionFirst Ti MemberCorrelated Metallic BehaviorCrystallographyTransition Metal ChalcogenidesApplied PhysicsCondensed Matter PhysicsCluster ChemistryMain Group Chemistry
We have synthesized and characterized the first Ti member of the AM4X8 (A = Ga, Ge; M = V, Nb, Ta, Mo, X = S, Se) family of compounds that exhibit a deficient spinel structure with tetrahedral transition metal clusters. Single-crystal X-ray structure determination of Ga0.87Ti4S8 (space group F−43m, a = 9.9083(11) Å) revealed the presence of Ga vacancies and a partial declustering of the transition metal atoms compared to other members of the family. This declustering is likely associated to the decrease of the electronic filling of the clusters from 7 to 11 electrons in known AM4X8 compounds to ∼3 electrons in Ga0.87Ti4S8. XPS measurements show that the valence band of Ga0.87Ti4S8 is more dispersed than that of the Mott insulator GaV4S8, which suggests a strengthening of the transfer integrals induced by the slackening of the transition metal clusters. A Fermi step consistent with a metallic character is observed in Ga0.87Ti4S8 while a gap appears (0.2 eV) below the Fermi level in the Mott insulator GaV4S8. The resistivity measured on crystals of Ga0.87Ti4S8 showed a metallic behavior with a small residual resistivity ratio. Ga0.87Ti4S8 exhibits large electronic specific heat (γ = 58 mJ K−2 mol−1) and Pauli susceptibility. All these measurements as well as the Wilson and Kadowaki-Woods ratios demonstrate that Ga0.87Ti4S8 exhibits a correlated metal type behavior and is no longer a paramagnetic Mott insulator like other members of the family.
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