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Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1x_{1-x}Rux_x)4_4Sb12_{12}

Abstract

X-ray powder diffraction, magnetic susceptibility χ(T)\chi(T), and electrical resistivity ρ(T)\rho(T) measurements were made on single crystals of the filled skutterudite series Pr(Os1x_{1-x}Rux_x)4_4Sb12_{12}. One end of the series (x=0x = 0) is a heavy fermion superconductor with a superconducting critical temperature Tc=1.85T_{c} = 1.85 K, while the other end (x=1x = 1) is a conventional superconductor with Tc1T_{c} \approx 1 K. The lattice constant aa decreases approximately linearly with increasing Ru concentration xx. As Ru (Os) is substituted for Os (Ru), TcT_{c} decreases nearly linearly with substituent concentration and exhibits a minimum with a value of Tc=0.75T_{c} = 0.75 K at x=0.6x = 0.6, suggesting that the two types of superconductivity compete with one another. Crystalline electric field (CEF) effects in χdc(T)\chi_\mathrm{dc}(T) and ρ(T)\rho(T) due to the splitting of the Pr3+^{3+} nine-fold degenerate Hund's rule J=4J = 4 multiplet are observed throughout the series, with the splitting between the ground state and the first excited state increasing monotonically as xx increases. The fits to the χdc(T)\chi_\mathrm{dc}(T) and ρ(T)\rho(T) data are consistent with a Γ3\Gamma_{3} doublet ground state for all values of x, although reasonable fits can be obtained for a Γ1\Gamma_{1} ground state for xx values near the end member compounds (x=0x = 0 or x=1x = 1).Comment: 10 pages, 8 figures, submitted to Phys. Rev.

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    Last time updated on 02/01/2020