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Evidence of a room-temperature quantum spin Hall edge state in a higher-order topological insulator.
Shumiya, Nana; Hossain, Md Shafayat; Yin, Jia-Xin; Wang, Zhiwei; Litskevich, Maksim; Yoon, Chiho; Li, Yongkai; Yang, Ying; Jiang, Yu-Xiao; Cheng, Guangming; Lin, Yen-Chuan; Zhang, Qi; Cheng, Zi-Jia; Cochran, Tyler A; Multer, Daniel; Yang, Xian P; Casas, Brian; Chang, Tay-Rong; Neupert, Titus; Yuan, Zhujun; Jia, Shuang; Lin, Hsin; Yao, Nan; Balicas, Luis; Zhang, Fan; Yao, Yugui; Hasan, M Zahid.
Afiliação
  • Shumiya N; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Hossain MS; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA. mdsh@princeton.edu.
  • Yin JX; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA. jiaxiny@princeton.edu.
  • Wang Z; Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, China.
  • Litskevich M; Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing Institute of Technology, Beijing, China.
  • Yoon C; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Li Y; Department of Physics, University of Texas at Dallas, Richardson, TX, USA.
  • Yang Y; Department of Physics and Astronomy, Seoul National University, Seoul, Korea.
  • Jiang YX; Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, China.
  • Cheng G; Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing Institute of Technology, Beijing, China.
  • Lin YC; Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing Institute of Technology, Beijing, China.
  • Zhang Q; Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing Institute of Technology, Beijing, China.
  • Cheng ZJ; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Cochran TA; Princeton Institute for Science and Technology of Materials, Princeton University, Princeton, NJ, USA.
  • Multer D; Department of Physics, National Taiwan University, Taipei, Taiwan.
  • Yang XP; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Casas B; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Chang TR; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Neupert T; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Yuan Z; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Jia S; National High Magnetic Field Laboratory, Tallahassee, FL, USA.
  • Lin H; Department of Physics, National Cheng Kung University, Tainan, Taiwan.
  • Yao N; Center for Quantum Frontiers of Research and Technology (QFort), Tainan, Taiwan.
  • Balicas L; Physics Division, National Center for Theoretical Sciences, Taipei, Taiwan.
  • Zhang F; Department of Physics, University of Zürich, Zürich, Switzerland.
  • Yao Y; International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
  • Hasan MZ; CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing, China.
Nat Mater ; 21(10): 1111-1115, 2022 Oct.
Article em En | MEDLINE | ID: mdl-35835819
Room-temperature realization of macroscopic quantum phases is one of the major pursuits in fundamental physics1,2. The quantum spin Hall phase3-6 is a topological quantum phase that features a two-dimensional insulating bulk and a helical edge state. Here we use vector magnetic field and variable temperature based scanning tunnelling microscopy to provide micro-spectroscopic evidence for a room-temperature quantum spin Hall edge state on the surface of the higher-order topological insulator Bi4Br4. We find that the atomically resolved lattice exhibits a large insulating gap of over 200 meV, and an atomically sharp monolayer step edge hosts an in-gap gapless state, suggesting topological bulk-boundary correspondence. An external magnetic field can gap the edge state, consistent with the time-reversal symmetry protection inherent in the underlying band topology. We further identify the geometrical hybridization of such edge states, which not only supports the Z2 topology of the quantum spin Hall state but also visualizes the building blocks of the higher-order topological insulator phase. Our results further encourage the exploration of high-temperature transport quantization of the putative topological phase reported here.

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Prognostic_studies Idioma: En Ano de publicação: 2022 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Prognostic_studies Idioma: En Ano de publicação: 2022 Tipo de documento: Article