Publication | Closed Access
Electronic and Structural Instabilities in GaV<sub>4</sub>S<sub>8</sub> and GaMo<sub>4</sub>S<sub>8</sub>
129
Citations
10
References
2000
Year
Magnetic PropertiesEngineeringSolid-state ChemistryElectronic StructureMagnetic MaterialsMagnetismQuantum MaterialsMaterials ScienceFerromagnetic OrderingPhysicsStructural InstabilitiesQuantum ChemistryMagnetic MaterialCrystallographySolid-state PhysicFerromagnetismNatural SciencesApplied PhysicsCondensed Matter PhysicsTemperature-dependent Magnetic MomentDirect Heating
GaV4S8 was prepared by direct heating of the elements at 1123 K. The crystal structures were refined from single-crystal data at room temperature (RT-GaV4S8, GaMo4S8-type, F4̄3m, a = 9.661(1) Å, Z = 4) and by the Rietveld method at 20 K (LT-GaV4S8, R3m, a = 6.834(1) Å, αrh = 59.66(2)°, Z = 1). Magnetic measurements show weak paramagnetism with a temperature-dependent magnetic moment between 1.5μB(50 K) and 1.9μB(300 K) compatible with one unpaired electron per V4 cluster. Ferromagnetic ordering was detected below TC = 10 K. DC electrical conductivity measurements between 30 and 320 K reveal semiconducting behavior. GaV4S8 undergoes a structural phase transition at 38 K from cubic to rhombohedral symmetry, as known for GaMo4S8, but with an opposite change of the rhombohedral angle αrh. This behavior is explained by self-consistent band structure calculations and simple cluster orbital schemes for GaV4S8 in comparison with GaMo4S8. The results prove that the directions of the structural deformations are determined by orbital interactions and depend on the electron count in the tetrahedral metal cluster units.
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