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Thermoelectric and Magnetic Properties of a Narrow-Gap Semiconductor FeGa<sub>3</sub>
74
Citations
19
References
2008
Year
SemiconductorsMagnetismMagnetic PropertiesFerromagnetismEngineeringPhysicsNatural SciencesSingle Crystalline SamplesCondensed Matter PhysicsQuantum MaterialsApplied PhysicsFega 3Thermoelectric MaterialSemiconductor MaterialCalculated Band GapMagnetic Materials
We report transport, thermal, and magnetic measurements on single crystalline samples of FeGa 3 prepared by a Ga self flux method. The electrical resistivity and Hall coefficient at temperatures above 300 K display semiconducting behaviors with energy gaps of 0.47 and 0.54 eV, respectively, whose values agree with the calculated band gap. In the saturation range 100–260 K, the carrier mobility µ exhibits an unusual dependence on temperature; µ( T )∝ T -5/2 . The thermopower has a large negative minimum of -350 µV/K at 300 K. The diamagnetic susceptibility weakly depends on temperature, which confirms the absence of localized magnetic moments. The T -linear coefficient of the specific heat is 0.03 mJ/(K 2 ·mol), being two orders of magnitude smaller than that reported for Fe-based Kondo semiconductors FeSi and FeSb 2 .
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