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Importance of charge fluctuations for the topological phase in SmB(6).
Min, Chul-Hee; Lutz, P; Fiedler, S; Kang, B Y; Cho, B K; Kim, H-D; Bentmann, H; Reinert, F.
Afiliação
  • Min CH; Universität Würzburg, Experimentelle Physik VII, 97074 Würzburg, Germany and Karlsruhe Institut für Technologie KIT, Gemeinschaftslabor für Nanoanalytik, 76021 Karlsruhe, Germany.
  • Lutz P; Universität Würzburg, Experimentelle Physik VII, 97074 Würzburg, Germany.
  • Fiedler S; Universität Würzburg, Experimentelle Physik VII, 97074 Würzburg, Germany and Karlsruhe Institut für Technologie KIT, Gemeinschaftslabor für Nanoanalytik, 76021 Karlsruhe, Germany.
  • Kang BY; School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Republic of Korea.
  • Cho BK; School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Republic of Korea.
  • Kim HD; Center for Correlated Electron Systems, Institute for Basic Science (IBS), Seoul 151-747, Republic of Korea and Department of Physics and Astronomy, Seoul National University, Seoul 151-747, Republic of Korea.
  • Bentmann H; Universität Würzburg, Experimentelle Physik VII, 97074 Würzburg, Germany and Karlsruhe Institut für Technologie KIT, Gemeinschaftslabor für Nanoanalytik, 76021 Karlsruhe, Germany.
  • Reinert F; Universität Würzburg, Experimentelle Physik VII, 97074 Würzburg, Germany and Karlsruhe Institut für Technologie KIT, Gemeinschaftslabor für Nanoanalytik, 76021 Karlsruhe, Germany.
Phys Rev Lett ; 112(22): 226402, 2014 Jun 06.
Article em En | MEDLINE | ID: mdl-24949780
Typical Kondo insulators (KIs) can have a nontrivial Z_{2} topology because the energy gap opens at the Fermi energy (E_{F}) by a hybridization between odd- and even-parity bands. SmB_{6} deviates from such KI behavior, and it has been unclear how the insulating phase occurs. Here, we demonstrate that charge fluctuations are the origin of the topological insulating phase in SmB_{6}. Our angle-resolved photoemission spectroscopy results reveal that with decreasing temperature the bottom of the d-f hybridized band at the X[over ¯] point, which is predicted to have odd parity and is required for a topological phase, gradually shifts from below to above E_{F}. We conclude that SmB_{6} is a charge-fluctuating topological insulator.
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Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2014 Tipo de documento: Article País de afiliação: Alemanha
Buscar no Google
Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2014 Tipo de documento: Article País de afiliação: Alemanha