Abstract

Fracton models, a collection of exotic gapped lattice Hamiltonians recently discovered in three spatial dimensions, contain some 'topological' features: they support fractional bulk excitations (dubbed fractons), and a ground state degeneracy that is robust to local perturbations. However, because previous fracton models have only been defined and analyzed on a cubic lattice with periodic boundary conditions, it is unclear to what extent a notion of topology is applicable. In this paper, we demonstrate that the X-cube model, a prototypical type-I fracton model, can be defined on general three-dimensional manifolds. Our construction revolves around the notion of a singular compact total foliation of the spatial manifold, which constructs a lattice from intersecting stacks of parallel surfaces called leaves. We find that the ground state degeneracy depends on the topology of the leaves and the pattern of leaf intersections. We further show that such a dependence can be understood from a renormalization group transformation for the X-cube model, wherein the system size can be changed by adding or removing 2D layers of topological states. Our results lead to an improved definition of fracton phase and bring to the fore the topological nature of fracton orders.

Highlights

  • Characterization and classification of quantum phases of matter is a fundamental problem of physics

  • We investigate the nature of the underlying physics in these fracton models: topological, geometric, or something else

  • Since a foliation of a three-manifold is regarded as a topological structure, we suggest that the X-cube model can be considered to be a new kind of generalized topological order

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Summary

INTRODUCTION

Characterization and classification of quantum phases of matter is a fundamental problem of physics. An intriguing class of gapped Hamiltonians referred to as fracton models in this paper have been proposed as potential new topological phases of matter [1,2,3,4,5,6,7,8,9,10,11,12]. These models appear in three spatial dimensions and have ground states exhibiting long-range entanglement. VII, we show that these results can be generalized to the ZN version of the X-cube model

REVIEW OF THE X-CUBE MODEL ON THE THREE-TORUS
X-CUBE MODEL ON GENERIC LATTICES
Intersecting leaves
X-CUBE MODEL ON GENERAL MANIFOLDS VIA TOTAL FOLIATION
Three-sphere
Half-twist manifold
Klein bottle times S1
Genus g surface times S1
ENTANGLEMENT RENORMALIZATION FOR THE X-CUBE MODEL
RG transformation
Ground-state degeneracy
Relation to the Haah code
Entanglement structure
TYPE-I FRACTON PHASES
ZN GENERALIZATION OF THE X-CUBE MODEL
VIII. DISCUSSION

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