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Title: Fractional Topological Insulators in Three Dimensions

Journal Article · · Physical Review Letters
;  [1];  [2];  [3]
  1. Department of Physics, Stanford University, Stanford, California 94305 (United States)
  2. Microsoft Research, Station Q, Elings Hall, University of California, Santa Barbara, California 93106 (United States)
  3. Department of Physics, University of Washington, Seattle, Washington 98195-1560 (United States)

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{sub 3}, and a 'halved' fractional quantum Hall effect on the surface with Hall conductance of the form {sigma}{sub H}=(p/q)(e{sup 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{sub 3} and allows fractional values consistent with T invariance.

OSTI ID:
21554467
Journal Information:
Physical Review Letters, Vol. 105, Issue 24; Other Information: DOI: 10.1103/PhysRevLett.105.246809; (c) 2010 American Institute of Physics; ISSN 0031-9007
Country of Publication:
United States
Language:
English