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Tunable unconventional kagome superconductivity in charge ordered RbV<sub>3</sub>Sb<sub>5</sub> and KV<sub>3</sub>Sb<sub>5</sub>

ORAL

Abstract

Unconventional superconductors often feature competing orders, small superfluid density, and nodal electronic pairing. While unusual superconductivity has been proposed in the kagome metals AV3Sb5, key spectroscopic evidence has remained elusive. Here we utilize pressure-tuned (up to 2.25 GPa) and ultra-low temperature (down to 18 mK) muon spin spectroscopy to uncover the unconventional nature of superconductivity in RbV3Sb5 and KV3Sb5. At ambient pressure, we detect a two-step enhancement of the width of the internal magnetic field distribution sensed by the muon ensemble in RbV3Sb5, indicative of time-reversal symmetry breaking charge order below T1' = 110 K with an additional transition at T2' = 50 K. Remarkably, the superconducting state displays a nodal energy gap and a reduced superfluid density, which can be attributed to the competition with the novel charge order. Upon applying pressure, the charge-order transitions are suppressed, the superfluid density increases, and the superconducting state progressively evolves from nodal to nodeless. Once optimal superconductivity is achieved, after either full or partial suppression of charge order, we find a superconducting pairing state that is not only fully gapped, but also spontaneously breaks time-reversal symmetry. Our results point to unprecedented tunable nodal kagome superconductivity competing with time-reversal symmetry-breaking charge order and offer unique insights into the nature of the pairing state.

Publication: Z. Guguchia et. al., arXiv:2202.07713 (2022).

Presenters

  • Zurab Guguchia

    Paul Scherrer Institute, Paul Scherrer Institut

Authors

  • Zurab Guguchia

    Paul Scherrer Institute, Paul Scherrer Institut

  • Charles Mielke

    University of Zurich

  • Debarchan Das

    Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen, PSI, Switzerland, LMU, Paul Scherrer Institute, Switzerland

  • Ritu Gupta

    Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen, PSI, Switzerland

  • Jiaxin Yin

    Princeton University

  • Hongxiong Liu

    Institute of Physics, Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences, Beijing, China, Chinese Academy of Sciences

  • Qiangwei Yin

    Renmin University of China, Renmin University of China, Beijing, China

  • Morten Holm Christensen

    Niels Bohr Institute, University of Copenhagen, University of Minnesota

  • Zhijun Tu

    Renmin University of China, Renmin University of China, Beijing, China

  • Chunsheng Gong

    Renmin University of China, Renmin University of China, Beijing, China

  • Nana Shumiya

    Princeton University

  • Tsotne Gamsakhurdashvili

    Paul Scherrer Institute

  • Mathias Elender

    Paul Scherrer Institute, Paul Scherrer Institute, Switzerland

  • Pengcheng Dai

    Rice University

  • Alex Amato

    Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen, PSI, Switzerland

  • Youguo Shi

    Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences, Beijing, China, Chinese Academy of Sciences

  • Hechang Lei

    Renmin University of China, Renmin University of China, Beijing, China, Princeton University

  • Rafael M Fernandes

    University of Minnesota

  • M. Zahid M Hasan

    Princeton University

  • Hubertus Luetkens

    Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen, PSI, Switzerland

  • Rustem Khasanov

    Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen, PSI, Switzerland