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Low temperature magnetic phase diagram of the cubic non-Fermi liquid system Celn(3-x)Sn(x)

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Fil.: Pedrazzini, P. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Caroca-Canales, N. Max-Planck Institute for Chemical Physics of Solids; Alemania
Fil.: Gómez Berisso, M. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Deppe, M. Max-Planck Institute for Chemical Physics of Solids; Alemania
Fil.: Sereni, J.G. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
Fil.: Geibel, C. Max-Planck Institute for Chemical Physics of Solids; Alemania

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Centro Atómico Bariloche

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eng

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In this paper we report a comprehensive study of the magnetic susceptibility (X), resistivity (ρ), and specific heat (Cp), down to 0.5 K of the cubic CeIn3-x Sn x alloy. The ground state of this system evolves from antiferromagnetic (AF) in CeIn3 (TN=10.2K) to intermediate-valent in CeSn3, and represents the first example of a Ce-lattice cubic non-Fermi liquid (NFL) system where TN (x) can be traced down to T = 0 over more than a decade of temperature. Our results indicate that the disappearance of the AF state occurs near xc≈0.7, although already at x≈0.4 significant modifications of the magnetic ground state are observed. Between these concentrations, clear NFL signatures are observed, such as ρ(T) ≈ ρ0 + ATn (with n < 1.5) and Cp (T)α‒ Tln (T) dependencies. Within the ordered phase a first order phase transition occurs for 0.25 < x < 0.5. With larger Sn doping, different weak ρ(T) dependencies are observed at low temperatures between x = 1 and x = 3 while Cp/T shows only a weak temperature dependence.

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The European Physical Journal B – Condensed Matter. Vol. 38, no. 3 (2004), p. 445-450

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