Mean string field theory: Landau-Ginzburg theory for 1-form symmetries
Nabil Iqbal, John McGreevy
SciPost Phys. 13, 114 (2022) · published 22 November 2022
- doi: 10.21468/SciPostPhys.13.5.114
- Submissions/Reports
Abstract
By analogy with the Landau-Ginzburg theory of ordinary zero-form symmetries, we introduce and develop a Landau-Ginzburg theory of one-form global symmetries, which we call mean string field theory. The basic dynamical variable is a string field -- defined on the space of closed loops -- that can be used to describe the creation, annihilation, and condensation of effective strings. Like its zero-form cousin, the mean string field theory provides a useful picture of the phase diagram of broken and unbroken phases. We provide a transparent derivation of the area law for charged line operators in the unbroken phase and describe the dynamics of gapless Goldstone modes in the broken phase. The framework also provides a theory of topological defects of the broken phase and a description of the phase transition that should be valid above an upper critical dimension, which we discuss. We also discuss general consequences of emergent one-form symmetries at zero and finite temperature.
Cited by 24
Authors / Affiliations: mappings to Contributors and Organizations
See all Organizations.- 1 Nabil Iqbal,
- 2 John McGreevy