Your browser doesn't support javascript.
loading
Topological chiral crystals with helicoid-arc quantum states.
Sanchez, Daniel S; Belopolski, Ilya; Cochran, Tyler A; Xu, Xitong; Yin, Jia-Xin; Chang, Guoqing; Xie, Weiwei; Manna, Kaustuv; Süß, Vicky; Huang, Cheng-Yi; Alidoust, Nasser; Multer, Daniel; Zhang, Songtian S; Shumiya, Nana; Wang, Xirui; Wang, Guang-Qiang; Chang, Tay-Rong; Felser, Claudia; Xu, Su-Yang; Jia, Shuang; Lin, Hsin; Hasan, M Zahid.
Afiliação
  • Sanchez DS; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Belopolski I; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Cochran TA; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Xu X; International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
  • Yin JX; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Chang G; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Xie W; Department of Chemistry, Louisiana State University, Baton Rouge, LA, USA.
  • Manna K; Max Planck Institute for Chemical Physics of Solids, Dresden, Germany.
  • Süß V; Max Planck Institute for Chemical Physics of Solids, Dresden, Germany.
  • Huang CY; Institute of Physics, Academia Sinica, Taipei, Taiwan.
  • Alidoust N; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Multer D; Rigetti Quantum Computing, Berkeley, CA, USA.
  • Zhang SS; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Shumiya N; Department of Chemistry, Princeton University, Princeton, NJ, USA.
  • Wang X; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Wang GQ; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Chang TR; International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
  • Felser C; International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
  • Xu SY; Department of Physics, National Cheng Kung University, Tainan, Taiwan.
  • Jia S; Max Planck Institute for Chemical Physics of Solids, Dresden, Germany.
  • Lin H; Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton University, Princeton, NJ, USA.
  • Hasan MZ; International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
Nature ; 567(7749): 500-505, 2019 03.
Article em En | MEDLINE | ID: mdl-30894753
ABSTRACT
The quantum behaviour of electrons in materials is the foundation of modern electronics and information technology1-11, and quantum materials with topological electronic and optical properties are essential for realizing quantized electronic responses that can be used for next generation technology. Here we report the first observation of topological quantum properties of chiral crystals6,7 in the RhSi family. We find that this material class hosts a quantum phase of matter that exhibits nearly ideal topological surface properties originating from the crystals' structural chirality. Electrons on the surface of these crystals show a highly unusual helicoid fermionic structure that spirals around two high-symmetry momenta, indicating electronic topological chirality. The existence of bulk multiply degenerate band fermions is guaranteed by the crystal symmetries; however, to determine the topological invariant or charge in these chiral crystals, it is essential to identify and study the helicoid topology of the arc states. The helicoid arcs that we observe on the surface characterize the topological charges of ±2, which arise from bulk higher-spin chiral fermions. These topological conductors exhibit giant Fermi arcs of maximum length (π), which are orders of magnitude larger than those found in known chiral Weyl fermion semimetals5,8-11. Our results demonstrate an electronic topological state of matter on structurally chiral crystals featuring helicoid-arc quantum states. Such exotic multifold chiral fermion semimetal states could be used to detect a quantized photogalvanic optical response, the chiral magnetic effect and other optoelectronic phenomena predicted for this class of materials6.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: Nature Ano de publicação: 2019 Tipo de documento: Article País de afiliação: Estados Unidos

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: Nature Ano de publicação: 2019 Tipo de documento: Article País de afiliação: Estados Unidos