Abstract
In this paper, we propose a generalization of the -duality of four-dimensional quantum electrodynamics () to with fractionally charged excitations, the fractional -duality. Such can be obtained by gauging the symmetry of a topologically ordered state with fractional charges. When time-reversal symmetry is imposed, the axion angle () can take a nontrivial but still time-reversal-invariant value (). Here, specifies the minimal electric charge carried by bulk excitations. Such states with time-reversal and global symmetry (fermion number conservation) are fractional topological insulators (FTIs). We propose a topological quantum field theory description, which microscopically justifies the fractional -duality. Then, we consider stacking operations (i.e., a direct sum of Hamiltonians) among FTIs. We find that there are two topologically distinct classes of FTIs: type I and type II. Type I () can be obtained by directly stacking a noninteracting topological insulator and a fractionalized gapped fermionic state with minimal charge and vanishing . But type II () cannot be realized through any stacking. Finally, we study the surface topological order of fractional topological insulators.
- Received 26 January 2017
- Revised 24 April 2017
DOI:https://doi.org/10.1103/PhysRevB.96.085125
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