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Distinctive doping dependence of upper critical field in iron-based superconductor LaFeAsO1−xHx

Shiro Kawachi1,2,*, Jun-ichi Yamaura1,†, Yoshio Kuramoto3, Soshi Iimura1,4, Toshihiro Nomura5, Yoshimitsu Kohama5, Takashi Sasaki1, Masashi Tokunaga5, Youichi Murakami3 et al.

Hideo Hosono1,4

  • 1Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama, Kanagawa 226-8503, Japan
  • 2Graduate School of Science, University of Hyogo, Koto, Hyogo 678-1297, Japan
  • 3Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan
  • 4National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan
  • 5The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan

  • *kawachi@sci.u-hyogo.ac.jp
  • †Present address: The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan; jyamaura@issp.u-tokyo.ac.jp

Phys. Rev. B 108, L100503 – Published 11 September, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L100503

Abstract

High magnetic fields up to 105 T have been utilized in deriving the upper critical field Bc2 of LaFeAsO1−xHx throughout the wide temperature range below Tc. Resistivity measurements demonstrate that Bc2 behaves differently in samples with x=0.12 (SC1) from those with 0.32 (SC2). In SC1, the two-band model assuming s-wave pairing gives a good fitting with a repulsive intraband interaction and dominant interband coupling. In SC2, we have to assume an attractive intraband interaction with weak interband coupling, which in fact suggests a non-s-wave pairing in view of the strong Coulomb repulsion. These results support the possibility that SC1 and SC2 have different pairing symmetries.

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