Antiferromagnetic topological insulators

By Roger S. K. Mong, A. Essin, J. Moore. 2010

439 citations recorded by the source corpus.

We consider antiferromagnets breaking both time-reversal $(\ensuremath{\Theta})$ and a primitive-lattice translational symmetry $({T}_{1/2})$ of a crystal but preserving the combination $S=\ensuremath{\Theta}{T}_{1/2}$. The $S$ symmetry leads to a ${\mathbb{Z}}_{2}$ topological classification of insulators, separating the ordinary insulator phase from the ``antiferromagnetic topological insulator'' phase. This state is similar to the ``strong'' topological insulator with time-reversal symmetry and shares with it such properties as a quantized magnetoelectric effect. However, for certain surfaces the surface states are intrinsically gapped with a half-quantum Hall effect $[{\ensuremath{\sigma}}_{xy}={e}^{2}/(2h)]$, which may aid experimental confirmation of $\ensuremath{\theta}=\ensuremath{\pi}$ quantized magnetoelectric coupling. Step edges on such a surface support gapless, chiral quantum wires. In closing we discuss GdBiPt as a possible example of this topological class.

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

View Paper: https://www.semanticscholar.org/paper/8a9a35ddb0dd3350d6402298b0f82d1132b94688

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In Atomic and Molecular Physics, and Optics

  1. D. Vanderbilt
  2. Hsin Lin
  3. Arun Bansil
  4. Tanmoy Das
  5. Liang Fu
  6. Bogdan Andrei Bernevig
  7. Shoucheng Zhang
  8. H. Weng

In Condensed Matter Physics

  1. Liang Fu
  2. Hsin Lin
  3. Arun Bansil
  4. Tanmoy Das
  5. Shoucheng Zhang
  6. D. Vanderbilt
  7. Bogdan Andrei Bernevig
  8. H. Weng

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