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Weak interband-coupling superconductivity in the filled skutterudite LaPt4Ge12

J. L. Zhang, G. M. Pang, L. Jiao, M. Nicklas, Y. Chen, Z. F. Weng, M. Smidman, W. Schnelle, A. Leithe-Jasper, A. Maisuradze, C. Baines, R. Khasanov, A. Amato, F. Steglich, R. Gumeniuk, and H. Q. Yuan
Phys. Rev. B 92, 220503(R) – Published 15 December 2015
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Abstract

The superconducting pairing state of LaPt4Ge12 is studied by measuring the magnetic penetration depth λ(T,B) and superfluid density ρs(T) using a tunnel-diode-oscillator (TDO)-based method and transverse-field muon-spin rotation (TFμSR) spectroscopy. The penetration depth follows an exponential-type temperature dependence at TTc, but increases linearly with magnetic field at T=1.5 K. A detailed analysis demonstrates that both λL(T) and ρsTDO(T), measured in the Meissner state using the TDO method, are well described by a two-gap γ model with gap sizes of Δ1(0)=1.31kBTc and Δ2(0)=1.80kBTc, and weak interband coupling. In contrast, ρsμSR(T), derived from the μSR data, can be fitted by a single-gap BCS model with a gap close to Δ2(0). We conclude that LaPt4Ge12 is a marginal two-gap superconductor and the small gap Δ1 seems to be suppressed by a small magnetic field applied in the μSR experiments. In comparison, the 4f electrons in PrPt4Ge12 may enhance the interband coupling and, therefore, give rise to more robust multiband superconductivity.

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  • Received 23 April 2015

DOI:https://doi.org/10.1103/PhysRevB.92.220503

©2015 American Physical Society

Authors & Affiliations

J. L. Zhang1,2, G. M. Pang1, L. Jiao1, M. Nicklas3,*, Y. Chen1, Z. F. Weng1, M. Smidman1, W. Schnelle3, A. Leithe-Jasper3, A. Maisuradze4,5, C. Baines4, R. Khasanov4, A. Amato4, F. Steglich1,3, R. Gumeniuk3,6, and H. Q. Yuan1,7,†

  • 1Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China
  • 2High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China
  • 3Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Straße 40, D-01187 Dresden, Germany
  • 4Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 5Physik-Institut der Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
  • 6Institut für Experimentelle Physik, TU Bergakademie Freiberg, Leipziger Straße 23, D-09596 Freiberg, Germany
  • 7Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China

  • *nicklas@cpfs.mpg.de
  • hqyuan@zju.edu.cn

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Issue

Vol. 92, Iss. 22 — 1 December 2015

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