Abstract.
In this paper we report a comprehensive study of the magnetic susceptibility (\(\chi\)), resistivity (\(\rho\)), and specific heat (\(C_{\rm P}\)), 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 (\(T_{\rm N} = 10.2 \)K) to intermediate-valent in CeSn3, and represents the first example of a Ce-lattice cubic non-Fermi liquid (NFL) system where \(T_{\rm N}(x)\) 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 \(x_{\rm c}\approx 0.7\), although already at \(x\approx 0.4\) significant modifications of the magnetic ground state are observed. Between these concentrations, clear NFL signatures are observed, such as \(\rho(T)\approx\rho_0 + A T^n\) (with n < 1.5) and \(C_{\rm P}(T)\propto-T\ln(T)\) dependencies. Within the ordered phase a first order phase transition occurs for 0.25 < x < 0.5. With larger Sn doping, different weak \(\rho(T)\) dependencies are observed at low temperatures between x = 1 and x = 3 while \(C_{\rm P}/T\) shows only a weak temperature dependence.
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Received: 15 March 2004, Published online: 28 May 2004
PACS:
71.20.Lp Intermetallic compounds - 71.27. + a Strongly correlated electron systems; heavy fermions - 75.20.Hr Local moment in compounds and alloys; Kondo effect, valence fluctuations, heavy fermions
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Pedrazzini, P., Gómez Berisso, M., Caroca-Canales, N. et al. Low temperature magnetic phase diagram of the cubic non-Fermi liquid system CeIn \(\mathsf{_{3-x}}\)Sn\(\mathsf{_x}\) . Eur. Phys. J. B 38, 445–450 (2004). https://doi.org/10.1140/epjb/e2004-00138-5
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DOI: https://doi.org/10.1140/epjb/e2004-00138-5