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Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5.
Guguchia, Z; Mielke, C; Das, D; Gupta, R; Yin, J-X; Liu, H; Yin, Q; Christensen, M H; Tu, Z; Gong, C; Shumiya, N; Hossain, Md Shafayat; Gamsakhurdashvili, Ts; Elender, M; Dai, Pengcheng; Amato, A; Shi, Y; Lei, H C; Fernandes, R M; Hasan, M Z; Luetkens, H; Khasanov, R.
Affiliation
  • Guguchia Z; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland. zurab.guguchia@psi.ch.
  • Mielke C; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Das D; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Gupta R; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Yin JX; Department of Physics, Southern University of Science and Technology, Shenzhen, Guangdong, 518055, China.
  • Liu H; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China.
  • Yin Q; University of Chinese Academy of Sciences, 100049, Beijing, China.
  • Christensen MH; Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China, 100872, Beijing, China.
  • Tu Z; Niels Bohr Institute, University of Copenhagen, Copenhagen, 2100, Denmark.
  • Gong C; Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China, 100872, Beijing, China.
  • Shumiya N; Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China, 100872, Beijing, China.
  • Hossain MS; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, 08544, USA.
  • Gamsakhurdashvili T; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, 08544, USA.
  • Elender M; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Dai P; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Amato A; Department of Physics and Astronomy, Rice University, Houston, TX, 77005, USA.
  • Shi Y; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232, Villigen PSI, Switzerland.
  • Lei HC; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, 100190, Beijing, China.
  • Fernandes RM; University of Chinese Academy of Sciences, 100049, Beijing, China.
  • Hasan MZ; Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China, 100872, Beijing, China.
  • Luetkens H; School of Physics and Astronomy, University of Minnesota, Minneapolis, MN, 55455, USA.
  • Khasanov R; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, 08544, USA.
Nat Commun ; 14(1): 153, 2023 Jan 11.
Article in En | MEDLINE | ID: mdl-36631467
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 and ultra-low temperature muon spin spectroscopy to uncover the unconventional nature of superconductivity in RbV3Sb5 and KV3Sb5. At ambient pressure, we observed time-reversal symmetry breaking charge order below [Formula see text] 110 K in RbV3Sb5 with an additional transition at [Formula see text] 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 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, 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.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nat Commun Journal subject: BIOLOGIA / CIENCIA Year: 2023 Document type: Article Affiliation country:

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nat Commun Journal subject: BIOLOGIA / CIENCIA Year: 2023 Document type: Article Affiliation country: