Field-insensitive heavy fermion features and phase transition in the caged-structure quasi-skutterudite Sm3_3Ru4_4Ge13_{13}

preprint2016arXivOpen access

Abstract

The robust field-insensitive heavy fermion features in Sm3_3Ru4_4Ge13_{13} and the magnetic phase transition at TN≈T_N \approx 5~K are studied using magnetization M(T)M(T), specific heat Cp(T)C_p(T), resistivity ρ(T)ρ(T) and thermal conductivity κT(T)κ_T(T). The average crystal structure of Sm3_3Ru4_4Ge13_{13} conforms to the cubic space group Pm3ˉnPm\bar{3}n however, signatures of subtle structural distortions are obtained from the x ray data. The magnetic susceptibility, χ(T)χ(T), follows a modified Curie-Weiss law indicating the presence of crystal fields of Sm3+^{3+} and the significance of van Vleck terms. No sign of ferromagnetism is observed in M(H)M(H) of Sm3_3Ru4_4Ge13_{13} which yields only 0.025~μBμ_\mathrm{B}/f.u.-Sm at 2~K, 7~T. The Sommerfeld coefficient, γ≈γ\approx 220~mJ/mol-Sm K2^2, estimated from the analysis of low temperature specific heat suggests the formation of heavy quasi particles at low temperature. Though a lnTT dependence of ρ(T)ρ(T) is observed till 60~K, the resistivity behavior is accounted for by assuming a two-band model for activated behavior of charge carriers. The field scans of resistivity, ρ(H)ρ(H), below TNT_N display significant nonlinearity while those above the TNT_N are more metal-like. Low values of thermal conductivity, κT(T)κ_T(T), are observed in Sm3_3Ru4_4Ge13_{13} however, displaying an anomaly at TNT_N which signifies magnetoelastic coupling. A fairly high value of Seebeck coefficient, S≈S \approx 40~μμV/K is observed at 300~K. We identify Sm3_3Ru4_4Ge13_{13} as a low charge carrier density system with unusual field-insensitive heavy fermion features very similar to the filled skutterudites.

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