Abstract

We revisit ’t Hooft anomalies in (1+1)dd non-spin quantum field theory, starting from the consistency and locality conditions, and find that consistent U(1) and gravitational anomalies cannot always be canceled by properly quantized (2+1)dd classical Chern-Simons actions. On the one hand, we prove that certain exotic anomalies can only be realized by non-reflection-positive or non-compact theories; on the other hand, without insisting on reflection-positivity, the exotic anomalies present a caveat to the inflow paradigm. For the mixed U(1) gravitational anomaly, we propose an inflow mechanism involving a mixed U(1)\times×SO(2) classical Chern-Simons action with a boundary condition that matches the SO(2) gauge field with the (1+1)dd spin connection. Furthermore, we show that this mixed anomaly gives rise to an isotopy anomaly of U(1) topological defect lines. The isotopy anomaly can be canceled by an extrinsic curvature improvement term, but at the cost of creating a periodicity anomaly. We survey the holomorphic bcbc ghost system which realizes all the exotic consistent anomalies, and end with comments on a subtlety regarding the anomalies of finite subgroups of U(1).

Highlights

  • A more modern perspective on ’t Hooft anomalies is the inflow paradigm: a D-dimensional anomalous quantum field theory (QFT) should be viewed as the boundary theory of a (D + 1)-dimensional bulk classical action, called a symmetry protected topological phase or an invertible field theory, such that the coupled system exhibits no anomaly [14,15,16,17,18,19,20,21,22,23,24,25,26,27,28]

  • For the mixed gravitational anomaly at hand, we show that this improvement is not possible, and only the consistent anomaly exists

  • The quantization conditions turned out to be weaker than those predicted by the inflow of properly quantized classical Chern-Simons actions

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Summary

Introduction

An ’t Hooft anomaly is a controlled breaking of symmetries in quantum field theory (QFT). A more modern perspective on ’t Hooft anomalies is the inflow paradigm: a D-dimensional anomalous QFT should be viewed as the boundary theory of a (D + 1)-dimensional bulk classical action, called a symmetry protected topological phase or an invertible field theory, such that the coupled system exhibits no anomaly [14,15,16,17,18,19,20,21,22,23,24,25,26,27,28]. We propose a relativistic inflow that matches the boundary (1+1)d spin connection with a bulk SO(2) gauge field Another slightly bizarre feature of the mixed gravitational anomaly is the non-existence of an improved stress tensor with covariant anomalous conservation. Appendix B proves that the consistent mixed gravitational anomaly does not have a covariant counterpart

Consistency and locality
Pure anomalies
Perturbative pure anomalies
Global gravitational anomaly
Topological defects and isotopy anomaly
Periodicity anomaly
Holomorphic bc ghost system
Concluding remarks
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