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Roton pair density wave in a strong-coupling kagome superconductor.
Chen, Hui; Yang, Haitao; Hu, Bin; Zhao, Zhen; Yuan, Jie; Xing, Yuqing; Qian, Guojian; Huang, Zihao; Li, Geng; Ye, Yuhan; Ma, Sheng; Ni, Shunli; Zhang, Hua; Yin, Qiangwei; Gong, Chunsheng; Tu, Zhijun; Lei, Hechang; Tan, Hengxin; Zhou, Sen; Shen, Chengmin; Dong, Xiaoli; Yan, Binghai; Wang, Ziqiang; Gao, Hong-Jun.
Afiliação
  • Chen H; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Yang H; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Hu B; CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Zhao Z; Songshan Lake Materials Laboratory, Dongguan, People's Republic of China.
  • Yuan J; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Xing Y; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Qian G; CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Huang Z; Songshan Lake Materials Laboratory, Dongguan, People's Republic of China.
  • Li G; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Ye Y; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Ma S; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Ni S; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Zhang H; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Yin Q; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Gong C; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Tu Z; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Lei H; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Tan H; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Zhou S; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Shen C; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Dong X; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Yan B; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Wang Z; CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing, People's Republic of China.
  • Gao HJ; Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China.
Nature ; 599(7884): 222-228, 2021 11.
Article em En | MEDLINE | ID: mdl-34587621
The transition metal kagome lattice materials host frustrated, correlated and topological quantum states of matter1-9. Recently, a new family of vanadium-based kagome metals, AV3Sb5 (A = K, Rb or Cs), with topological band structures has been discovered10,11. These layered compounds are nonmagnetic and undergo charge density wave transitions before developing superconductivity at low temperatures11-19. Here we report the observation of unconventional superconductivity and a pair density wave (PDW) in CsV3Sb5 using scanning tunnelling microscope/spectroscopy and Josephson scanning tunnelling spectroscopy. We find that CsV3Sb5 exhibits a V-shaped pairing gap Δ ~ 0.5 meV and is a strong-coupling superconductor (2Δ/kBTc ~ 5) that coexists with 4a0 unidirectional and 2a0 × 2a0 charge order. Remarkably, we discover a 3Q PDW accompanied by bidirectional 4a0/3 spatial modulations of the superconducting gap, coherence peak and gap depth in the tunnelling conductance. We term this novel quantum state a roton PDW associated with an underlying vortex-antivortex lattice that can account for the observed conductance modulations. Probing the electronic states in the vortex halo in an applied magnetic field, in strong field that suppresses superconductivity and in zero field above Tc, reveals that the PDW is a primary state responsible for an emergent pseudogap and intertwined electronic order. Our findings show striking analogies and distinctions to the phenomenology of high-Tc cuprate superconductors, and provide groundwork for understanding the microscopic origin of correlated electronic states and superconductivity in vanadium-based kagome metals.

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Qualitative_research Idioma: En Revista: Nature Ano de publicação: 2021 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Qualitative_research Idioma: En Revista: Nature Ano de publicação: 2021 Tipo de documento: Article