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Observation of flat band, Dirac nodal lines and topological surface states in Kagome superconductor CsTi3Bi5.
Yang, Jiangang; Yi, Xinwei; Zhao, Zhen; Xie, Yuyang; Miao, Taimin; Luo, Hailan; Chen, Hao; Liang, Bo; Zhu, Wenpei; Ye, Yuhan; You, Jing-Yang; Gu, Bo; Zhang, Shenjin; Zhang, Fengfeng; Yang, Feng; Wang, Zhimin; Peng, Qinjun; Mao, Hanqing; Liu, Guodong; Xu, Zuyan; Chen, Hui; Yang, Haitao; Su, Gang; Gao, Hongjun; Zhao, Lin; Zhou, X J.
Afiliación
  • Yang J; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Yi X; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Zhao Z; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Xie Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Miao T; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Luo H; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Chen H; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Liang B; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhu W; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Ye Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • You JY; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Gu B; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhang S; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Zhang F; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Yang F; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Wang Z; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Peng Q; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Mao H; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Liu G; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Xu Z; Department of Physics, Faculty of Science, National University of Singapore, Singapore, 117551, Singapore.
  • Chen H; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • Yang H; CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing, 100190, China.
  • Su G; Kavli Institute of Theoretical Sciences, University of Chinese Academy of Sciences, Beijing, 100190, China.
  • Gao H; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhao L; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhou XJ; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, China.
Nat Commun ; 14(1): 4089, 2023 Jul 10.
Article en En | MEDLINE | ID: mdl-37429852
ABSTRACT
Kagome lattices of various transition metals are versatile platforms for achieving anomalous Hall effects, unconventional charge-density wave orders and quantum spin liquid phenomena due to the strong correlations, spin-orbit coupling and/or magnetic interactions involved in such a lattice. Here, we use laser-based angle-resolved photoemission spectroscopy in combination with density functional theory calculations to investigate the electronic structure of the newly discovered kagome superconductor CsTi3Bi5, which is isostructural to the AV3Sb5 (A = K, Rb or Cs) kagome superconductor family and possesses a two-dimensional kagome network of titanium. We directly observe a striking flat band derived from the local destructive interference of Bloch wave functions within the kagome lattice. In agreement with calculations, we identify type-II and type-III Dirac nodal lines and their momentum distribution in CsTi3Bi5 from the measured electronic structures. In addition, around the Brillouin zone centre, [Formula see text] nontrivial topological surface states are also observed due to band inversion mediated by strong spin-orbit coupling.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2023 Tipo del documento: Article País de afiliación: China

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2023 Tipo del documento: Article País de afiliación: China
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