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Superconductivity under pressure in a chromium-based kagome metal.
Liu, Yi; Liu, Zi-Yi; Bao, Jin-Ke; Yang, Peng-Tao; Ji, Liang-Wen; Wu, Si-Qi; Shen, Qin-Xin; Luo, Jun; Yang, Jie; Liu, Ji-Yong; Xu, Chen-Chao; Yang, Wu-Zhang; Chai, Wan-Li; Lu, Jia-Yi; Liu, Chang-Chao; Wang, Bo-Sen; Jiang, Hao; Tao, Qian; Ren, Zhi; Xu, Xiao-Feng; Cao, Chao; Xu, Zhu-An; Zhou, Rui; Cheng, Jin-Guang; Cao, Guang-Han.
Affiliation
  • Liu Y; School of Physics, Zhejiang University, Hangzhou, China.
  • Liu ZY; Department of Applied Physics, Key Laboratory of Quantum Precision Measurement of Zhejiang Province, Zhejiang University of Technology, Hangzhou, China.
  • Bao JK; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Yang PT; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Ji LW; School of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou, China.
  • Wu SQ; Department of Physics, Materials Genome Institute and Shanghai Key Laboratory of High Temperature Superconductors, Shanghai University, Shanghai, China.
  • Shen QX; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Luo J; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Yang J; School of Physics, Zhejiang University, Hangzhou, China.
  • Liu JY; School of Physics, Zhejiang University, Hangzhou, China.
  • Xu CC; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Yang WZ; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Chai WL; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Lu JY; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Liu CC; Department of Chemistry, Zhejiang University, Hangzhou, China.
  • Wang BS; School of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou, China.
  • Jiang H; School of Science, Westlake Institute for Advanced Study, Westlake University, Hangzhou, China.
  • Tao Q; School of Physics, Zhejiang University, Hangzhou, China.
  • Ren Z; School of Physics, Zhejiang University, Hangzhou, China.
  • Xu XF; School of Physics, Zhejiang University, Hangzhou, China.
  • Cao C; Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Xu ZA; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Zhou R; School of Physics and Optoelectronics, Xiangtan University, Xiangtan, China.
  • Cheng JG; School of Physics, Zhejiang University, Hangzhou, China.
  • Cao GH; School of Science, Westlake Institute for Advanced Study, Westlake University, Hangzhou, China.
Nature ; 632(8027): 1032-1037, 2024 Aug.
Article in En | MEDLINE | ID: mdl-39198671
ABSTRACT
Superconductivity in a highly correlated kagome system has been theoretically proposed for years (refs. 1-5), yet the experimental realization is hard to achieve6,7. The recently discovered vanadium-based kagome materials8, which exhibit both superconductivity9-11 and charge-density-wave orders12-14, are nonmagnetic8,9 and weakly correlated15,16. Thus these materials are unlikely to host the exotic superconductivity theoretically proposed. Here we report the discovery of a chromium-based kagome metal, CsCr3Sb5, which is contrastingly featured with strong electron correlations, frustrated magnetism and characteristic flat bands close to the Fermi level. Under ambient pressure, this kagome metal undergoes a concurrent structural and magnetic phase transition at 55 K, with a stripe-like 4a0 structural modulation. At high pressure, the phase transition evolves into two transitions, possibly associated with charge-density-wave and antiferromagnetic spin-density-wave orderings. These density-wave-like orders are gradually suppressed with pressure and, remarkably, a superconducting dome emerges at 3.65-8.0 GPa. The maximum of the superconducting transition temperature, Tcmax = 6.4 K, appears when the density-wave-like orders are completely suppressed at 4.2 GPa, and the normal state exhibits a non-Fermi-liquid behaviour, reminiscent of unconventional superconductivity and quantum criticality in iron-based superconductors17,18. Our work offers an unprecedented platform for investigating superconductivity in correlated kagome systems.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nature Year: 2024 Type: Article Affiliation country: China

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nature Year: 2024 Type: Article Affiliation country: China