Fractional topological insulators in three dimensions

Details Fractional topological insulators in three dimensions Fractional topological insulators in three dimensions

2010-04-21

arxiv.org/abs/1004.3628v3

Phys. Rev. Lett. 105, 246809 (2010)

Physics

Condensed Matter

Strongly Correlated Electrons

4+epsilon pages, 1 figure; accepted for publication in Phys. Rev. Lett

Scientific paper

10.1103/PhysRevLett.105.246809

Topological insulators can be generally defined by a topological field theory with an axion angle theta of 0 or pi. In this work, we introduce the concept of fractional topological insulator defined by a fractional axion angle and show that it can be consistent with time reversal (T) invariance if ground state degeneracies are present. The fractional axion angle can be measured experimentally by the quantized fractional bulk magnetoelectric polarization P_3, and a `halved' fractional quantum Hall effect on the surface with Hall conductance of the form (p/q)(e^2/2h) with p,q odd. In the simplest of these states the electron behaves as a bound state of three fractionally charged `quarks' coupled to a deconfined non-Abelian SU(3) `color' gauge field, where the fractional charge of the quarks changes the quantization condition of P_3 and allows fractional values consistent with T-invariance.

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