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Orbital-selective spin texture and its manipulation in a topological insulator.
Xie, Zhuojin; He, Shaolong; Chen, Chaoyu; Feng, Ya; Yi, Hemian; Liang, Aiji; Zhao, Lin; Mou, Daixiang; He, Junfeng; Peng, Yingying; Liu, Xu; Liu, Yan; Liu, Guodong; Dong, Xiaoli; Yu, Li; Zhang, Jun; Zhang, Shenjin; Wang, Zhimin; Zhang, Fengfeng; Yang, Feng; Peng, Qinjun; Wang, Xiaoyang; Chen, Chuangtian; Xu, Zuyan; Zhou, X J.
Afiliação
  • Xie Z; 1] Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China [2].
  • He S; 1] Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China [2].
  • Chen C; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Feng Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Yi H; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Liang A; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhao L; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Mou D; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • He J; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Peng Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Liu X; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Liu Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Liu G; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Dong X; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Yu L; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhang J; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhang S; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Wang Z; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhang F; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Yang F; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Peng Q; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Wang X; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Chen C; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Xu Z; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhou XJ; 1] Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China [2] Collaborative Innovation Center of Quantum Matter, Beijing 100871, China.
Nat Commun ; 5: 3382, 2014 Feb 28.
Article em En | MEDLINE | ID: mdl-24584220
ABSTRACT
Topological insulators represent a new quantum state of matter that are insulating in the bulk but metallic on the edge or surface. In the Dirac surface state, it is well-established that the electron spin is locked with the crystal momentum. Here we report a new phenomenon of the spin texture locking with the orbital texture in a topological insulator Bi2Se3. We observe light-polarization-dependent spin texture of both the upper and lower Dirac cones that constitutes strong evidence of the orbital-dependent spin texture in Bi2Se3. The different spin texture detected in variable polarization geometry is the manifestation of the spin-orbital texture in the initial state combined with the photoemission matrix element effects. Our observations provide a new orbital degree of freedom and a new way of light manipulation in controlling the spin structure of the topological insulators that are important for their future applications in spin-related technologies.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Nat Commun Assunto da revista: BIOLOGIA / CIENCIA Ano de publicação: 2014 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Nat Commun Assunto da revista: BIOLOGIA / CIENCIA Ano de publicação: 2014 Tipo de documento: Article