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Maximizing T c by tuning nematicity and magnetism in FeSe1−x S x superconductors

Author

Listed:
  • K. Matsuura

    (University of Tokyo)

  • Y. Mizukami

    (University of Tokyo)

  • Y. Arai

    (University of Tokyo)

  • Y. Sugimura

    (University of Tokyo)

  • N. Maejima

    (Synchrotron Radiation Research Center, National Institutes for Quantum and Radiological Science and Technology)

  • A. Machida

    (Synchrotron Radiation Research Center, National Institutes for Quantum and Radiological Science and Technology)

  • T. Watanuki

    (Synchrotron Radiation Research Center, National Institutes for Quantum and Radiological Science and Technology)

  • T. Fukuda

    (Materials Sciences Research Center, Japan Atomic Energy Agency (SPring-8/JAEA))

  • T. Yajima

    (The University of Tokyo)

  • Z. Hiroi

    (The University of Tokyo)

  • K. Y. Yip

    (The Chinese University of Hong Kong)

  • Y. C. Chan

    (The Chinese University of Hong Kong)

  • Q. Niu

    (The Chinese University of Hong Kong)

  • S. Hosoi

    (University of Tokyo)

  • K. Ishida

    (University of Tokyo)

  • K. Mukasa

    (University of Tokyo)

  • S. Kasahara

    (Kyoto University)

  • J.-G. Cheng

    (Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences)

  • S. K. Goh

    (The Chinese University of Hong Kong)

  • Y. Matsuda

    (Kyoto University)

  • Y. Uwatoko

    (The University of Tokyo)

  • T. Shibauchi

    (University of Tokyo)

Abstract

A fundamental issue concerning iron-based superconductivity is the roles of electronic nematicity and magnetism in realising high transition temperature (T c). To address this issue, FeSe is a key material, as it exhibits a unique pressure phase diagram involving non-magnetic nematic and pressure-induced antiferromagnetic ordered phases. However, as these two phases in FeSe have considerable overlap, how each order affects superconductivity remains perplexing. Here we construct the three-dimensional electronic phase diagram, temperature (T) against pressure (P) and isovalent S-substitution (x), for FeSe1−x S x . By simultaneously tuning chemical and physical pressures, against which the chalcogen height shows a contrasting variation, we achieve a complete separation of nematic and antiferromagnetic phases. In between, an extended non-magnetic tetragonal phase emerges, where T c shows a striking enhancement. The completed phase diagram uncovers that high-T c superconductivity lies near both ends of the dome-shaped antiferromagnetic phase, whereas T c remains low near the nematic critical point.

Suggested Citation

  • K. Matsuura & Y. Mizukami & Y. Arai & Y. Sugimura & N. Maejima & A. Machida & T. Watanuki & T. Fukuda & T. Yajima & Z. Hiroi & K. Y. Yip & Y. C. Chan & Q. Niu & S. Hosoi & K. Ishida & K. Mukasa & S. K, 2017. "Maximizing T c by tuning nematicity and magnetism in FeSe1−x S x superconductors," Nature Communications, Nature, vol. 8(1), pages 1-6, December.
  • Handle: RePEc:nat:natcom:v:8:y:2017:i:1:d:10.1038_s41467-017-01277-x
    DOI: 10.1038/s41467-017-01277-x
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