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Heavy-Fermion and Semiconducting Properties of the Ternary Uranium Compounds U<sub>3</sub>T<sub>3</sub>Sn<sub>4</sub>and U<sub>3</sub>T<sub>3</sub>Sb<sub>4</sub>(T=Ni, Cu, Pd, Pt and Au)
59
Citations
9
References
1990
Year
EngineeringX 4U 3ChemistryInorganic MaterialElectronic StructureSemiconducting PropertiesBand GapMagnetismQuantum MaterialsNuclear MaterialsMaterials ScienceInorganic ChemistryPhysicsQuantum ChemistryTransition Metal ChalcogenidesNatural SciencesCondensed Matter PhysicsApplied Physics
We present results of magnetic, transport and calorimetric measurements on U 3 T 3 X 4 with T=Ni, Cu, Pd, Pt and Au and X=Sn and Sb. A heavy-fermion behavior manifests itself in U 3 T 3 Sn 4 , where the electronic specific-heat coefficient increases from 90 mJ/K 2 mol U for T=Ni and Pt to about 300 mJ/K 2 mol U for T=Cu and Au. We ascribe the mass enhancement to the dehybridization of 5 f electrons with the d electrons derived from the T atom. On the other hand, U 3 T 3 Sb 4 with T=Ni, Pd and Pt shows a semiconducting behavior with a band gap of about 0.2 eV, whereas U 3 Cu 3 Sb 4 is a metallic ferromagnet with T c =91 K. In these antimonides, 5 f electrons are localized because of the weak hybridization with the 5 p electrons from the Sb atom. These results indicate that the number of 5 p electrons in the present system determines whether the system shows heavy-fermion or semiconducting behavior.
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