Abstract

We discuss an isomorphism between the possible anomalies of $(d+1)$-dimensional quantum field theories with $\mathbb{Z}_{2}$ unitary global symmetry, and those of $d$-dimensional quantum field theories with time-reversal symmetry $\mathsf{T}$. This correspondence is an instance of symmetry defect decoration. The worldvolume of a $\mathbb{Z}_{2}$ symmetry defect is naturally invariant under $\mathsf{T},$ and bulk $\mathbb{Z}_{2}$ anomalies descend to $\mathsf{T}$ anomalies on these defects. We illustrate this correspondence in detail for $(1+1)d$ bosonic systems where the bulk $\mathbb{Z}_{2}$ anomaly leads to a Kramers degeneracy in the symmetry defect Hilbert space, and exhibit examples. We also discuss $(1+1)d$ fermion systems protected by $\mathbb{Z}_{2}$ global symmetry where interactions lead to a $\mathbb{Z}_{8}$ classification of anomalies. Under the correspondence, this is directly related to the $\mathbb{Z}_{8}$ classification of $(0+1)d$ fermions protected by $\mathsf{T}$. Finally, we consider $(3+1)d$ bosonic systems with $\mathbb{Z}_{2}$ symmetry where the possible anomalies are classified by $\mathbb{Z}_{2}\times \mathbb{Z}_{2}$. We construct topological field theories realizing these anomalies and show that their associated symmetry defects support anyons that can be either fermions or Kramers doublets.

Highlights

  • Global symmetries and anomalies are crucial tools in the analysis of quantum field theory

  • Since anomalies of d dimensional theories are determined by inflow from (d þ 1)-dimensional symmetry-protected topological phases (SPTs), our discussion can be interpreted as a connection between SPTs

  • The precise mathematical relationship behind (1.1) is sometimes referred to as a Smith isomorphism [9,10], which we review in Appendix

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Summary

INTRODUCTION

Global symmetries and anomalies are crucial tools in the analysis of quantum field theory. A rich class of phenomena are associated with systems with discrete global symmetry In this case the associated anomalies are finite order and can be carried by gapped or gapless systems. A precise understanding of the physics of anomalies is a central tool in many recent developments including the theory of topological insulators. Since anomalies of d dimensional theories are determined by inflow from (d þ 1)-dimensional symmetry-protected topological phases (SPTs), our discussion can be interpreted as a connection between SPTs. there is an isomorphism: Z2 anomalies in d dimensions. We illustrate this correspondence in a simple class of models described by ð1 þ 1Þd bosonic quantum field theories (QFTs) with Z2 global symmetry. We discuss the extension to ð1 þ 1Þd fermionic systems and give an example application in ð3 þ 1Þd bosonic systems

Z2 symmetry defects and time-reversal symmetry
Generalization to spin systems
Further extensions
Symmetry lines and the defect Hilbert space
Orientation-reversal anomaly on the symmetry line
Symmetry lines on curved surfaces
Orientation-reversal anomaly for Z2 lines
KRAMERS DOUBLETS IN THE
T2 CFT with no time-reversal symmetry
Ising model
Twisted compactification
Discrete gauge theory construction
Full Text
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