Quantized Anomalous Hall Effect in Magnetic Topological Insulators

By R. Yu, Wei Zhang, Haijun Zhang, Shoucheng Zhang, X. Dai, Z. Fang. Science, 2010

1,876 citations recorded by the source corpus.

Quantum Anomalous Hall Effect In addition to the Hall effect, which appears as a voltage change in conductors in response to an external magnetic field, ferromagnets exhibit the anomalous Hall effect, which is often proportional to their magnetization and independent of the presence of the magnetic field. This effect, first observed more than a century ago, has not been realized in its quantized form. Yu et al. (p. 61, published online 3 June) propose a realization of a quantum anomalous Hall system by magnetically doping thin films of three-dimensional topological insulators and calculate the effects of various dopants and film thicknesses. The resulting insulators are predicted to have long-range ferromagnetic order, potentially joining dilute magnetic semiconductors as candidates for spintronic applications. Magnetically doped topological insulators are predicted to be ferromagnetic and exhibit the quantum anomalous Hall effect. The anomalous Hall effect is a fundamental transport process in solids arising from the spin-orbit coupling. In a quantum anomalous Hall insulator, spontaneous magnetic moments and spin-orbit coupling combine to give rise to a topologically nontrivial electronic structure, leading to the quantized Hall effect without an external magnetic field. Based on first-principles calculations, we predict that the tetradymite semiconductors Bi2Te3, Bi2Se3, and Sb2Te3 form magnetically ordered insulators when doped with transition metal elements (Cr or Fe), in contrast to conventional dilute magnetic semiconductors where free carriers are necessary to mediate the magnetic coupling. In two-dimensional thin films, this magnetic order gives rise to a topological electronic structure characterized by a finite Chern number, with the Hall conductance quantized in units of e2/h (where e is the charge of an electron and h is Planck’s constant).

Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics, Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/d7821c00788d420148b2174d714d3501534065df

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In Atomic and Molecular Physics, and Optics

  1. Ashvin Vishwanath
  2. D. Vanderbilt
  3. Hsin Lin
  4. Arun Bansil
  5. Shoucheng Zhang
  6. Tanmoy Das
  7. X. Dai
  8. Z. Fang

In Condensed Matter Physics

  1. Shoucheng Zhang
  2. X. Dai
  3. Z. Fang
  4. H. Weng
  5. Zhong Wang
  6. Xiao-Liang Qi
  7. Hsin Lin
  8. Arun Bansil

In Materials Chemistry

  1. Shoucheng Zhang
  2. Ashvin Vishwanath
  3. Hsin Lin
  4. Arun Bansil
  5. D. Vanderbilt
  6. Allan H. MacDonald
  7. Xiao-Liang Qi
  8. Z. Fang

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