Abstract

Recently, it was realized that anomalies can be completely classified by topological orders, symmetry protected topological (SPT) orders, and symmetry enriched topological orders in one higher dimension. The anomalies that people used to study are invertible anomalies that correspond to invertible topological orders and/or symmetry protected topological orders in one higher dimension. In this paper, we introduce a notion of non-invertible anomaly, which describes the boundary of generic topological order. A key feature of non-invertible anomaly is that it has several partition functions. Under the mapping class group transformation of space-time, those partition functions transform in a certain way characterized by the data of the corresponding topological order in one higher dimension. In fact, the anomalous partition functions transform in the same way as the degenerate ground states of the corresponding topological order in one higher dimension. This general theory of non-invertible anomaly may have wide applications. As an example, we show that the irreducible gapless boundary of 2+1D double-semion (DS) topological order must have central charge $c=\bar c \geq \frac{25}{28}$.

Highlights

  • A classical field theory described by an action may have a gauge symmetry if the action is gauge invariant

  • The boundary of symmetry enriched topological order will corresponds to new types of gravitational anomaly with symmetry

  • We give the conformal field theory (CFT) characters and the partition functions induced by defect lines another physical interpretation, by viewing them as noninvertible anomaly

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Summary

INTRODUCTION

A classical field theory described by an action may have a gauge symmetry if the action is gauge invariant. The boundary of symmetry enriched topological order will corresponds to new types of gravitational anomaly with symmetry This point of view of anomaly plus Atiyah formulation of topological quantum field theory [16] allow us to develop a general theory of anomaly [7,8,9]. Eq (2) is a unified description for both gapped and gapless boundaries As another application, we point out that anomaly-free fermionic theories exactly correspond a subset of the bosonic theories with the noninvertible gravitational anomaly described by the bosonic Z2 topological order with emergent. A connection between the modular transformation of boundary partition functions and the S and T matrices that characterize the modular tensor category for the 2+1D bulk topological order was noticed Our paper generalizes those results and provides a more systematic discussion.

TOPOLOGICAL INVARIANT AND PROPERTIES OF BOUNDARY PARTITION FUNCTION
Topological partition function as topological invariant
Invertible and noninvertible topological orders
Properties of boundary partition function
Modular transformations of the partition function for an anomalous theory
NONINVERTIBLE GRAVITATIONAL ANOMALY AND “NONLOCALITY” OF HILBERT SPACE
Z2 topological order
Double-semion topological order
Semion topological order
Fibonacci topological order
VIII. SUMMARY
The minimal model CFT
Space-time lattice and branching structure
Discrete path integral
Path integral on space-time with natural boundary
Topological path integral
Topological path integral with world lines
Full Text
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