28 August 2022 to 2 September 2022
Science and Technology Campus, University of Parma
Europe/Rome timezone
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Two-component superconductivity in Sr$_2$RuO$_4$ studied by uniaxial and hydrostatic pressure $\mu$SR

O-7
29 Aug 2022, 15:00
20m
Science and Technology Campus, University of Parma

Science and Technology Campus, University of Parma

University of Parma, Italy
Oral Superconductivity Oral contributions

Speaker

Hans-Henning Klauss (TU Dresden)

Description

After two decades of research, the symmetry of the superconducting state in Sr$_2$RuO$_4$ is still under strong debate. The long time favoured spin-triplet px + i py state is ruled out by recent NMR experiments (1). However, in general time-reversal-symmetry breaking (TRSB) superconductivity indicates complex two-component order parameters. Probing Sr$_2$RuO$_4$ under uniaxial pressure offers the possibility to lift the degeneracy between such components (2). One key prediction for Sr$_2$RuO$_4$, a splitting of the superconducting and TRSB transitions under uniaxial pressure has not been observed so far.
Here, we report results of muon spin relaxation (μSR) measurements on Sr$_2$RuO$_4$ placed under uniaxial stress (3). We observed a large pressure-induced splitting between the onset temperatures of superconductivity (T$_c$) and TRSB (T$_{\mathrm{TRSB}}$). Moreover, at high stress beyond the van Hove singularity, a new spin density wave ordered phase is observed.
To distinguish between a symmetry protected chiral state (d+id) and non-chiral accidentally degenerated order parameters (d+ig, f+ig) we also report $\mu$SR studies under symmetry conserving hydrostatic pressure. In these experiment no splitting between T$_c$ and T$_{\mathrm{TRSB}}$ is observed (4).
In this talk we discuss the implications on the superconducting order parameter in Sr$_2$RuO$_4$.

(Left) Electronic phase diagram of Sr$_2$RuO$_4$  versus uniaxial pressure applied along the <100> direction (3). (Right) TRSB transition temperature versus superconducting transition temperature of Sr$_2$RuO$_4$ under hydrostatic and uniaxial pressure and La impurity doping (4).

*This work was supported by DFG (GR 4667, GRK 1621, and SFB 1143).
(1) A. Pustogow, et al., Nature 574, 72 (2019)
(2) C. Hicks, et al., Science 344, 283 (2014), M. E. Barber, et al., Phys. Rev. Lett. 120, 076602 (2018).
(3) V. Grinenko, S. Ghosh, et al.,  Nat. Phys. (2021)
(4) V. Grinenko, et al., Nat. Comm. (2021)

Primary authors

Dr Shreenanda Ghosh (Institute for Solid State and Materials Physics, Technische Universitat Dresden, Dresden, Germany ) Dr Vadim Grinenko (Institute for Solid State and Materials Physics, Technische Universitat Dresden, Dresden, Germany ) Mr Felix Brückner (Institute for Solid State and Materials Physics, Technische Universitat Dresden, Dresden, Germany ) Rajib Sarkar (TU Dresden) Dr Rustem Khasanov (Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland) J.‑C. Orain (Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut) Dr Artem Nikitin (PSI Villigen Switzerland) Mr Matthias Elender (PSI Villigen Switzerland) Dr Debarchan Das (PSI Viligen Switzerland) Dr Zurab Guguchia (Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland) Dr Hubertus Luetkens (Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland) Dr J. Park Mark Barber (MPI-CPfS Dresden) Dr Dmitry Sokolov (MPI-CPfS Dresden) Prof. Andrew Mackenzie (MPI-CPfS Dresden) Prof. Clifford Hicks (MPI-CPfS Dresden) Dr Jake Bobowski (MPI-CPfS Dresden) Dr Takuto Miyoshi (Kyoto University, Japan) Prof. Yoshiteru Maeno (Kyoto University, Japan) Dr Naoki Kikugawa (National Institute for Materials Science, Japan) Dr Bastian Zinkl (ETH Zürich) Prof. Manfred Sigrist (ETH Zürich) Hans-Henning Klauss (TU Dresden)

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