Journal of the Physical Society of Japan · 2005 · 373 citations · 8 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsElectronic MaterialsSolid State PhysicsAntiferromagnetic MaterialsAntiferromagnetismPhase TransitionsStrongly Correlated Electron SystemsSuperconducting MaterialsAmbient Pressure EffectsFermi SurfaceHeavy Fermion SystemsHeavy-fermion SuperconductorsHigh-pressure Phase TransitionsHigh-temperature SuperconductivityHigh-temperature SuperconductorsUnconventional Superconductivity
We carried out the de Haas–van Alphen (dHvA) experiment for an antiferromagnet CeRhIn 5 at high pressures up to 3 GPa. The cross-sectional areas of the Fermi surfaces due to main dHvA branches α i and β 2 at ambient pressure, which are well explained by two kinds of nearly cylindrical Fermi surfaces of a non-4 f reference compound LaRhIn 5 , are unchanged up to about 2.3 GPa, while the corresponding cyclotron masses m c * increase steeply above a pressure P * = 1.6 GPa where pressure-induced superconductivity sets in : m * c = 5.5 m 0 at ambient pressure, 20 m 0 at 1.6 GPa and 60 m 0 at 2.2 GPa for branch β 2 , for example. Above 2.4 GPa, new dHvA branches appear, which are in good agreement with the corresponding dHvA branches of a 4 f -itinerant heavy fermion superconductor CeCoIn 5 , indicating that the 4 f electron of CeRhIn 5 becomes itinerant and significantly contributes to the volume of the Fermi surface. The 4 f -electron character is thus changed from localized to itinerant at a critical pressure P c ≃2.35 GPa, where the superconducting transition temperature becomes a maximum.
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Superconductivity on the border of itinerant-electron ferromagnetism in UGe2
S. S. Saxena, P. Agarwal, K. Ahilan et al. · Nature · 2000 · 1.5K citations
Z. Fisk, M. Jaime, R. Movshovich et al. · Technische Universität Dortmund Eldorado (Technische Universität Dortmund) · 2001 · 248 citations · Full text