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Phys. Rev. Lett. 103, 146401 (2009) [4 pages]

Observation of Time-Reversal-Protected Single-Dirac-Cone Topological-Insulator States in Bi2Te3 and Sb2Te3

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D. Hsieh1, Y. Xia1, D. Qian1, L. Wray1, F. Meier2,3, J. H. Dil2,3, J. Osterwalder3, L. Patthey2, A. V. Fedorov4, H. Lin5, A. Bansil5, D. Grauer6, Y. S. Hor6, R. J. Cava6, and M. Z. Hasan1,*
1Joseph Henry Laboratories of Physics, Princeton University, Princeton, New Jersey 08544, USA
2Swiss Light Source, Paul Scherrer Institute, CH-5232, Villigen, Switzerland
3Physik-Institut, Universität Zürich-Irchel, 8057 Zürich, Switzerland
4Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
5Department of Physics, Northeastern University, Boston, Massachusetts 02115, USA
6Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA

Received 18 June 2009; published 28 September 2009

We show that the strongly spin-orbit coupled materials Bi2Te3 and Sb2Te3 and their derivatives belong to the Z2 topological-insulator class. Using a combination of first-principles theoretical calculations and photoemission spectroscopy, we directly show that Bi2Te3 is a large spin-orbit-induced indirect bulk band gap (δ∼150  meV) semiconductor whose surface is characterized by a single topological spin-Dirac cone. The electronic structure of self-doped Sb2Te3 exhibits similar Z2 topological properties. We demonstrate that the dynamics of spin-Dirac fermions can be controlled through systematic Mn doping, making these materials classes potentially suitable for topological device applications.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.103.146401
DOI:
10.1103/PhysRevLett.103.146401
PACS:
71.20.−b, 71.10.Pm, 73.20.At, 73.23.−b

*mzhasan@Princeton.edu