Journal of the Physical Society of Japan · 1990 · 56 citations · 12 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsElectronic MaterialsMagnetic MaterialsMagnetic Properties Of SolidsMagnetism In SolidsMetalsSemiconductor Device MaterialsSemiconductor PhysicsBand Structure CalculationCarrier ConcentrationConductionFermi FunctionFermi LevelFermi SurfaceMagnetoresistanceMetal-semiconductor Interfaces
The magnetoresistance and the de Haas-van Alphen (dHvA) effect in CeSn 3 have been measured in the field up to 150 kOe and at temperature down to 0.45 K. The magnetoresistance does not show a tendency to saturate in all field directions. This result claims that CeSn 3 is a compensated metal with an equal carrier concentration of electrons and holes, and electron and hole Fermi surfaces possess no open orbits. In contrast to an uncompensated metal LaSn 3 , the 4 f electrons in CeSn 3 become itinerant electrons. This is consistent with the dHvA data which are almost explained by the modified Fermi surface model based on the result of band calculation where the 4 f electrons are treated the same as the usual s , p , d conduction electrons.
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The fermi surface of CeSn3 and LaSn3
D. D. Koelling · Solid State Communications · 1982 · 111 citations