Superconducting properties of sulfur-doped iron selenide

Mahmoud Abdel-Hafiez, Yuan-Yuan Zhang, Zi-Yu Cao, Chun-Gang Duan, G. Karapetrov, V. M. Pudalov, V. A. Vlasenko, A. V. Sadakov, D. A. Knyazev, T. A. Romanova, D. A. Chareev, O. S. Volkova, A. N. Vasiliev, and Xiao-Jia Chen
Phys. Rev. B 91, 165109 – Published 6 April 2015

Abstract

The recent discovery of high-temperature superconductivity in single-layer iron selenide has generated significant experimental interest for optimizing the superconducting properties of iron-based superconductors through the lattice modification. For simulating the similar effect by changing the chemical composition due to S doping, we investigate the superconducting properties of high-quality single crystals of FeSe1xSx (x=0, 0.04, 0.09, and 0.11) using magnetization, resistivity, the London penetration depth, and low temperature specific heat measurements. We show that the introduction of S to FeSe enhances the superconducting transition temperature Tc, anisotropy, upper critical field Hc2, and critical current density Jc. The upper critical field Hc2(T) and its anisotropy are strongly temperature dependent, indicating a multiband superconductivity in this system. Through the measurements and analysis of the London penetration depth λab(T) and specific heat, we show clear evidence for strong coupling two-gap s-wave superconductivity. The temperature dependence of λab(T) calculated from the lower critical field and electronic specific heat can be well described by using a two-band model with s-wave-like gaps. We find that a d wave and single-gap BCS theory under the weak-coupling approach cannot describe our experiments. The change of specific heat induced by the magnetic field can be understood only in terms of multiband superconductivity.

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  • Received 28 January 2015
  • Revised 20 March 2015

DOI:https://doi.org/10.1103/PhysRevB.91.165109

©2015 American Physical Society

Authors & Affiliations

Mahmoud Abdel-Hafiez1,2, Yuan-Yuan Zhang3, Zi-Yu Cao1,4, Chun-Gang Duan3, G. Karapetrov5, V. M. Pudalov6,7, V. A. Vlasenko6, A. V. Sadakov6, D. A. Knyazev6, T. A. Romanova6, D. A. Chareev8, O. S. Volkova9,10, A. N. Vasiliev9,10,11, and Xiao-Jia Chen1,*

  • 1Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China
  • 2Faculty of science, Physics department, Fayoum University, 63514-Fayoum, Egypt
  • 3Key Laboratory of Polar Materials and Devices, East China Normal University, Shanghai 200241, China
  • 4Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China
  • 5Department of Physics, Drexel University, Philadelphia, Pennsylvania 19104, USA
  • 6P. N. Lebedev Physical Institute, Russian Academy of Sciences, Moscow 119991, Russia
  • 7Moscow Institute of Physics and Technology, Moscow 141700, Russia
  • 8Institute of Experimental Mineralogy, Russian Academy of Sciences, 142432, Chernogolovka, Moscow District, Russia
  • 9Low Temperature Physics and Superconductivity Department, Physics Faculty, M.V. Lomonosov Moscow State University, 119991 Moscow, Russia
  • 10Theoretical Physics and Applied Mathematics Department, Ural Federal University, 620002 Ekaterinburg, Russia
  • 11National University of Science and Technology “MISiS,” Moscow 119049, Russia

  • *xjchen@hpstar.ac.cn

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Issue

Vol. 91, Iss. 16 — 15 April 2015

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