Publicación: Nonmonotonous evolution of the Kondo temperature in the phase diagram of Ce(Pd1-xCux)(2)Si-2
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Fil.: Gómez Berisso, M. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Zwicknagl, G. Max-Planck-Institut fu¨r Physik komplexer System; Alemania
Fil.: Trovarelli, O. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Geibel, C. Max-Planck-Institut fu¨r Chemische Physik fester Stoffe; Alemania
Fil.: Pedrazzini, P. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Steglich, F. Max-Planck-Institut fu¨r Chemische Physik fester Stoffe; Alemania
Fil.: Sereni, J.G. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
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Centro Atómico Bariloche
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eng
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The evolution of the behavior of the Ce 4f electron with the Cu content in the alloy Ce(Pd1−xCux)2Si2 was investigated by determining its structural, magnetic, transport, and thermal properties. Results obtained on 15 samples with compositions distributed along the whole concentration range allow us to draw a magnetic phase diagram showing three distinct regions. The first region at low Cu concentrations corresponds to the antiferromagnetic-ordered regime. The fast suppression of this magnetic order between x=0.2 and x=0.25 suggests the presence of a critical point which separates this region from the second one at larger x values where no magnetic order is observed. The main characteristic of this second region, which extends up to x=0.7, is a pronounced increase of the Kondo temperature TK, from TK≈15 K at x=0.25 to TK≈50 K at x=0.7. This is in contrast with the fast decrease of TK in the region with x>0.7. In this region a small anomaly with a ferromagnetic character is observed in the specific heat arround 4 K. The change in the evolution of TK with x coincides with a change in the composition dependence of the c lattice parameter of the tetragonal structure, pointing to a structure-related origin of this unusual TK(x) behavior. This nonmonotonous TK(x) dependence is reproduced using local-density-approximation band-structure calculations, which show a maximum of the hybridization strength between conduction electrons and Ce 4f states for intermediate Cu concentrations. Such a TK(x) dependence which contradicts the monotonous dependence observed in all other Ce-based alloy systems is the hallmark of the Ce(Pd1−xCux)2Si2 alloy, which cannot be described as a Fermi-liquid system in the nonmagnetic region.
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Physical Review B – Condensed Matter and Materials Physics. Vol. 58, no. 1 (1998), p. 314-321