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The order–disorder transition of Ti<sup>3+</sup>–Ti<sup>3+</sup>pairs in Ti<sub>4</sub>O<sub>7</sub>and (Ti<sub>1–x</sub>V<sub>x</sub>)<sub>4</sub>O<sub>7</sub>
64
Citations
8
References
1980
Year
Magnetic PropertiesCoulomb RepulsionWigner GlassEngineeringSolid-state ChemistryQuantum MaterialsMaterial PhysicMaterials ScienceSolid-state IonicPhysicsCrystalline DefectsCrystal MaterialQuantum ChemistryCrystallographyCondensed Matter TheorySolid-state PhysicOrdered PhaseNatural SciencesApplied PhysicsCondensed Matter PhysicsDisordered Quantum SystemOrder–disorder TransitionCritical Phenomenon
Abstract Studies of electrical resistivity, specific heat, magnetic susceptibility and structural data are reported for Ti4O7 and (Ti1–xVx)4O7 single crystals (0 0·35 at.%, the disordered phase is stabilized down to the lowest temperatures obtained. The ordered phase is described in terms of a crystallization of charges related to interatomic Coulomb repulsion; the intermediate phase may be considered as a Wigner glass involving a random potential due to the disordered charges. The excitations of the Ti3+–Ti3+ pairs may be viewed as bipolarons, responsible for the transport properties of the intermediate disordered phase. The stabilization of the disordered phase by small concentrations of V is attributed to the increase of background disorder such as the forma...
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