Abstract

Mass generation of gauge fields can be universally described by topological couplings in gapped systems, such as the Abelian Higgs model in $(3+1)$ dimensions and the Maxwell-Chern-Simons theory in $(2+1)$ dimensions. These systems also exhibit the spontaneous breaking of higher-form $\mathbb{Z}_k$ symmetries and topological orders for level $k \geq 2$. In this paper, we consider topological mass generation in gapless systems. As a paradigmatic example, we study the axion electrodynamics with level $k$ in $(3+1)$ dimensions in background fields that hosts both gapped and gapless modes. We argue that the gapped mode is related to those in fully gapped systems in lower dimensions via dimensional reduction. We show that this system exhibits the spontaneous breaking of a higher-form $\mathbb{Z}_k$ symmetry despite the absence of the conventional topological order. In the case of the background magnetic field, we also derive the low-energy effective theory of the gapless mode with the quadratic dispersion relation and show that it satisfies the chiral anomaly matching.

Highlights

  • Understanding the origin of the mass is an important question in modern physics

  • It has been recently shown that photons can acquire a mass gap in (3 þ 1) dimensions even without the conventional Higgs mechanism: in the axion electrodynamics in the presence of background fields, such as a spatially varying axion field [2,3] or an external magnetic field [4,5], one of the helicity states of the photons acquires a mass gap, while the other is gapless with the quadratic dispersion relation

  • We argue that the helicity-dependent mass generation of photons in this theory is related to the topological mass generation in gapped systems in lower dimensions via dimensional reduction

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Summary

INTRODUCTION

Understanding the origin of the mass is an important question in modern physics. Among others, the Higgs mechanism provides a mechanism to explain the mass generation of gauge fields, such as the massive gauge bosons WÆ and Z0 mediating the weak interaction and massive photons in superconductivity. We can show that it exhibits the spontaneous breaking of a higher-form Zk symmetry similar to the gapped systems with topological order.2 This system satisfies the chiral anomaly matching by the gapless modes. We clarify the relation of the mass generation mechanism in this gapless system to those in gapped systems, the spontaneous breaking of a higher-form Zk symmetry, and how the chiral anomaly matching is satisfied at low energy. We take the level k to be positive for all the topological couplings without loss of generality

TOPOLOGICAL MASS GENERATION IN GAPPED SYSTEMS
Dual Stueckelberg action
Topological order and spontaneous breaking of higher-form Zk symmetries
Examples
Topological coupling with two one-form gauge fields
TOPOLOGICAL MASS GENERATION IN GAPLESS SYSTEMS
Background magnetic field
Spatially varying axion background
Higher-form symmetries without background fields
Symmetry transformations
Higher-form symmetries with background fields
Higher-form symmetry breaking
Low-energy effective theory and chiral anomaly matching
DISCUSSIONS

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