Abstract

In three dimensions, gapped phases can support "fractonic" quasiparticle excitations, which are either completely immobile or can only move within a low-dimensional submanifold, a peculiar topological phenomenon going beyond the conventional framework of topological quantum field theory. In this work we explore fractonic topological phases using three-dimensional coupled wire constructions, which have proven to be a successful tool to realize and characterize topological phases in two dimensions. We find that both gapped and gapless phases with fractonic excitations can emerge from the models. In the gapped case, we argue that fractonic excitations are mobile along the wire direction, but their mobility in the transverse plane is generally reduced. We show that the excitations in general have infinite-order fusion structure, distinct from previously known gapped fracton models. Like the 2D coupled wire constructions, many models exhibit gapless (or even chiral) surface states, which can be described by infinite-component Luttinger liquids. However, the universality class of the surface theory strongly depends on the surface orientation, thus revealing a new type of bulk-boundary correspondence unique to fracton phases.

Highlights

  • It is a common belief that gapped phases of quantum manybody systems can be described by topological quantum field theories (TQFT)

  • In searching for the unified structure underlying fracton order, it was realized that certain fracton models can be built from coupling stacks of two-dimensional (2D) topological phases [9,10]

  • A simple stack of layers of 2D gapped states already exhibits some of the characteristics of fracton topological order, e.g., size-dependent ground-state degeneracy (GSD), quasiparticles with reduced mobility

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Summary

INTRODUCTION

It is a common belief that gapped phases of quantum manybody systems can be described by topological quantum field theories (TQFT). A simple stack of layers of 2D gapped states already exhibits some of the characteristics of fracton topological order, e.g., size-dependent GSD, quasiparticles with reduced mobility (i.e., they can only move in planes). This observation has inspired more general constructions of fracton topological order [11,12,13,14,15,16,17], as well as shedding light on the precise meaning of frac-. We find that the construction can give rise to both gapped and gapless phases In both cases, there can exist gapped fractonic excitations. IV an example with each wire hosting a two-component Luttinger liquid is considered These “CSS” models are shown to be gapped, with all quasiparticles being lineon.

COUPLED-WIRE CONSTRUCTION
Energy spectrum and excitations
Ground-state degeneracy
Surface states
Polynomial representation
CHIRAL PLAQUETTE MODELS
Surface theory
Mobility along x
Planon phase I
Planon phase II
Gapless fracton phase
Gapless planon phase
CSS MODELS
DISCUSSIONS
Mode expansion of bosonic fields
Bogoliubov transformation for bosons
Spectrum of the chiral plaquette models
Now we use the definition that for each power product
Cleaning to a minimal box containing the excitation patches
Diagonal pair creation operators
Horizontal and vertical strips
L-shaped operators
Full Text
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