Topological Orders with Global Gauge Anomalies
arXiv:1502.07752 · doi:10.1103/PhysRevB.92.054410
Abstract
By definition, the physics of the dimensional (dim) boundary of a dim symmetry protected topological (SPT) state cannot be realized as itself on a dim lattice. If the symmetry of the system is unitary, then a formal way to determine whether a dim theory must be a boundary or not, is to couple this theory to a gauge field (or to "gauge" its symmetry), and check if there is a gauge anomaly. In this paper we discuss the following question: can the boundary of a SPT state be driven into a fully gapped topological order which preserves all the symmetries? We argue that if the gauge anomaly of the boundary is "perturbative", then the boundary must remain gapless; while if the boundary only has global gauge anomaly but no perturbative anomaly, then it is possible to gap out the boundary by driving it into a topological state, when . We will demonstrate this conclusion with two examples: (1) the spin-1/2 chiral fermion with the well-known Witten's global anomaly, which is the boundary of a topological superconductor with SU(2) or U(1) symmetry; and (2) the boundary of a topological superconductor with the same symmetry. We show that these boundary systems can be driven into a fully gapped topological order with topological degeneracy, but this topological order cannot be future driven into a trivial confined phase that preserves all the symmetries due to some special properties of its topological defects.
12 pages
References in corpus (3)
- Three dimensional topological invariants for time reversal invariant Hamiltonians and the three dimensional quantum spin Hall effect
- Physics of three dimensional bosonic topological insulators: Surface Deconfined Criticality and Quantized Magnetoelectric Effect
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- Competing Orders and Anomalies