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Phys. Rev. Lett. 97, 036808 (2006) [4 pages]

Quantum Spin-Hall Effect and Topologically Invariant Chern Numbers

D. N. Sheng,1 Z. Y. Weng,2 L. Sheng,3 and F. D. M. Haldane4
1Department of Physics and Astronomy, California State University, Northridge, California 91330, USA
2Center for Advanced Study, Tsinghua University, Beijing 100084, China
3Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204, USA
4Department of Physics, Princeton University, Princeton, New Jersey 08544, USA

Received 6 March 2006; published 21 July 2006

We present a topological description of the quantum spin-Hall effect (QSHE) in a two-dimensional electron system on a honeycomb lattice with both intrinsic and Rashba spin-orbit couplings. We show that the topology of the band insulator can be characterized by a 2×2 matrix of first Chern integers. The nontrivial QSHE phase is identified by the nonzero diagonal matrix elements of the Chern number matrix (CNM). A spin Chern number is derived from the CNM, which is conserved in the presence of finite disorder scattering and spin nonconserving Rashba coupling. By using the Laughlin gedanken experiment, we numerically calculate the spin polarization and spin transfer rate of the conducting edge states and determine a phase diagram for the QSHE.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevLett.97.036808
DOI: 10.1103/PhysRevLett.97.036808
PACS: 73.43.Nq; 11.15.-q; 72.25.-b
  • 73.43.Nq
    Quantum phase transitions (quantum Hall effect)
  • 11.15.-q
    Gauge field theories
  • 72.25.-b
    Spin polarized transport
  • YEAR: 2006

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