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Manipulation of the time-reversal symmetry breaking superconductivity in Sr<sub>2</sub>RuO<sub>4</sub> by uniaxial stress

ORAL

Abstract


The symmetry of the unconventional superconducting state of Sr2RuO4 continues to be under strong debate [1]. In general, time-reversal-symmetry breaking (TRSB) superconductivity indicates two-component order parameters. Probing Sr2RuO4 under uniaxial stress offers the possibility to lift the degeneracy between such components. One key prediction for Sr2RuO4, a splitting of the superconducting and TRSB transitions under uniaxial stress has not been observed so far. We report measurements of zero-field muon spin relaxation (μSR) on samples under uniaxial stresses of up to ∼1.05 GPa. We observe a stress-induced splitting between the onset temperatures of superconductivity and TRSB, consistent with qualitative expectations for a chiral order parameter. In addition, we report the appearance of a bulk magnetic order under the uniaxial stress of ∼1.0 GPa [2]. A custom pressure cell was developed to perform μSR under uniaxial stress[3].

References:
[1] Kivelson et al. npj Qua Mat. 5, 43 (2020).
[2] V. Grinenko*, S. Ghosh* et al., https://www.nature.com/articles/s41567-021-01182-7#Abs1.'
[3] S. Ghosh et al., Rev. Sci. Inst. 91, 103902 (2020).
**This work was supported by DFG (GR 4667, GRK 1621, SFB 1143).

Presenters

  • Shreenanda Ghosh

    Institute for Solid State and Materials Physics, Technical University of Dresden, Germany

Authors

  • Shreenanda Ghosh

    Institute for Solid State and Materials Physics, Technical University of Dresden, Germany

  • Vadim Grinenko

    Institute for Solid State and Materials Physics, Technische Universitat Dresden, Institute for Solid State and Materials Physics, Technical University of Dresden, Germany

  • Rajib Sarkar

    Institute for Solid State and Materials Physics, Technical University of Dresden, Germany

  • Felix Bruckner

    Institute for Solid State and Materials Physics, Technische Universitat Dresden, Institute for Solid State and Materials Physics, Technical University of Dresden, Germany

  • Jean-Christophe Orain

    Paul Scherrer Institute, Bulk MUSR group, LMU 5232 Villigen PSI, Switzerland, Laboratory for Muon spin spectroscopy, Paul Scherrer Institute, Villigen, Switzerland

  • Artem Nikitin

    Laboratory for Muon spin spectroscopy, Paul Scherrer Institute, Villigen, Switzerland

  • Joonbum Park

    Max Planck Institute for Chemical Physics of Solids, Dresden, Germany

  • Mark E Barber

    Max Planck Institute for Chemical Physics of Solids, Dresden, Germany

  • Naoki Kikugawa

    National Institute for Materials Science, Tsukuba, Japan, National Institute for Material Science, Tsukuba Japan, National Institute for Materials Science, National Institute for Material Science, Japan

  • Jake Bobowski

    Department of Physics, Graduate School of Science, Kyoto University, Kyoto, Japan

  • Dmitry Sokolov

    Max Planck Institute for Chemical Physics of Solids, Dresden, Germany, Max Planck Institute for Chemical Physics of Solids, Max Planck Institute for the Chemical Physics of Solids

  • YOSHITERU Maeno

    Department of Physics, Graduate School of Science, Kyoto University, Kyoto, Japan

  • Andrew P. Mackenzie

    Max Planck Institute for Chemical Physics of Solids, Dresden, Germany

  • Hubertus Luetkens

    Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, Laboratory for Muon spin spectroscopy, Paul Scherrer Institute, Villigen, Switzerland

  • Clifford W Hicks

    Max Planck Institute for Chemical Physics of Solids, Dresden, Germany, Max Planck Institute for Chemical Physics of Solids, Chemical Physics of Solids, Max Planck Institute, Max Planck Institute for the Chemical Physics of Solids

  • Hans-Henning Klauss

    Institute for Solid State and Materials Physics, Technische Universitat Dresden, Institute for Solid State and Materials Physics, Technical University of Dresden, Germany