Realizing anomalous anyonic symmetries at the surfaces of 3d gauge theories
Lukasz Fidkowski, Ashvin Vishwanath

TL;DR
This paper demonstrates how anomalous anyonic symmetries, previously thought to be unphysical in 2D, can be realized as surface states of 3D topological phases, expanding the understanding of symmetry-enriched topological phases.
Contribution
It provides a physical realization of anomalous anyonic symmetry actions as surface theories of 3D long-range entangled phases, resolving a longstanding puzzle.
Findings
Identified anomalous symmetry actions that cannot be realized in 2D.
Established a correspondence between these anomalies and 3D bulk phases.
Expanded the classification of symmetry-enriched topological phases.
Abstract
The hallmark of a 2 dimensional topologically ordered phase is the existence of deconfined `anyon' excitations that have exotic braiding and exchange statistics, different from those of ordinary bosons or fermions. As opposed to conventional Landau-Ginzburg-Wilson phases, which are classified on the basis of the spontaneous breaking of an underlying symmetry, topologically ordered phases, such as those occurring in the fractional quantum Hall effect, are absolutely stable, not requiring any such symmetry. Recently, though, it has been realized that symmetries, which may still be present in such systems, can give rise to a host of new, distinct, many-body phases, all of which share the same underlying topological order. A useful approach to classifying SETs is to determine all possible such symmetry actions on the anyons that are algebraically consistent with the anyons' statistics.…
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