Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5

The nature of the superconductivity in the kagome metals AV3Sb5 (A = K, Rb, Cs) remains under debate. Here, using muon spin spectroscopy, the authors find that the superconductivity in RbV3Sb5 and KV3Sb5 evolves from nodal to nodeless with increasing pressure and the superconducting state breaks tim...

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Published in:Nature Communications
Main Authors: Z. Guguchia, C. Mielke, D. Das, R. Gupta, J.-X. Yin, H. Liu, Q. Yin, M. H. Christensen, Z. Tu, C. Gong, N. Shumiya, Md Shafayat Hossain, Ts. Gamsakhurdashvili, M. Elender, Pengcheng Dai, A. Amato, Y. Shi, H. C. Lei, R. M. Fernandes, M. Z. Hasan, H. Luetkens, R. Khasanov
Format: Article
Language:English
Published: Nature Portfolio 2023-01-01
Online Access:https://doi.org/10.1038/s41467-022-35718-z
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author Z. Guguchia
C. Mielke
D. Das
R. Gupta
J.-X. Yin
H. Liu
Q. Yin
M. H. Christensen
Z. Tu
C. Gong
N. Shumiya
Md Shafayat Hossain
Ts. Gamsakhurdashvili
M. Elender
Pengcheng Dai
A. Amato
Y. Shi
H. C. Lei
R. M. Fernandes
M. Z. Hasan
H. Luetkens
R. Khasanov
author_facet Z. Guguchia
C. Mielke
D. Das
R. Gupta
J.-X. Yin
H. Liu
Q. Yin
M. H. Christensen
Z. Tu
C. Gong
N. Shumiya
Md Shafayat Hossain
Ts. Gamsakhurdashvili
M. Elender
Pengcheng Dai
A. Amato
Y. Shi
H. C. Lei
R. M. Fernandes
M. Z. Hasan
H. Luetkens
R. Khasanov
author_sort Z. Guguchia
collection DOAJ
container_title Nature Communications
description The nature of the superconductivity in the kagome metals AV3Sb5 (A = K, Rb, Cs) remains under debate. Here, using muon spin spectroscopy, the authors find that the superconductivity in RbV3Sb5 and KV3Sb5 evolves from nodal to nodeless with increasing pressure and the superconducting state breaks time-reversal symmetry after suppression of the charge order.
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spelling doaj-art-e07255d879c94564bf426a2ab4dc30202025-08-19T21:13:56ZengNature PortfolioNature Communications2041-17232023-01-0114111010.1038/s41467-022-35718-zTunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5Z. Guguchia0C. Mielke1D. Das2R. Gupta3J.-X. Yin4H. Liu5Q. Yin6M. H. Christensen7Z. Tu8C. Gong9N. Shumiya10Md Shafayat Hossain11Ts. Gamsakhurdashvili12M. Elender13Pengcheng Dai14A. Amato15Y. Shi16H. C. Lei17R. M. Fernandes18M. Z. Hasan19H. Luetkens20R. Khasanov21Laboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteDepartment of Physics, Southern University of Science and TechnologyBeijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of SciencesDepartment of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of ChinaNiels Bohr Institute, University of CopenhagenDepartment of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of ChinaDepartment of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of ChinaLaboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton UniversityLaboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton UniversityLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteDepartment of Physics and Astronomy, Rice UniversityLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteBeijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of SciencesDepartment of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of ChinaSchool of Physics and Astronomy, University of MinnesotaLaboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton UniversityLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteLaboratory for Muon Spin Spectroscopy, Paul Scherrer InstituteThe nature of the superconductivity in the kagome metals AV3Sb5 (A = K, Rb, Cs) remains under debate. Here, using muon spin spectroscopy, the authors find that the superconductivity in RbV3Sb5 and KV3Sb5 evolves from nodal to nodeless with increasing pressure and the superconducting state breaks time-reversal symmetry after suppression of the charge order.https://doi.org/10.1038/s41467-022-35718-z
spellingShingle Z. Guguchia
C. Mielke
D. Das
R. Gupta
J.-X. Yin
H. Liu
Q. Yin
M. H. Christensen
Z. Tu
C. Gong
N. Shumiya
Md Shafayat Hossain
Ts. Gamsakhurdashvili
M. Elender
Pengcheng Dai
A. Amato
Y. Shi
H. C. Lei
R. M. Fernandes
M. Z. Hasan
H. Luetkens
R. Khasanov
Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title_full Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title_fullStr Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title_full_unstemmed Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title_short Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
title_sort tunable unconventional kagome superconductivity in charge ordered rbv3sb5 and kv3sb5
url https://doi.org/10.1038/s41467-022-35718-z
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