Abstract

In this paper, we classify EF topological orders for 3+1D bosonic systems where some emergent pointlike excitations are fermions. (1) We argue that all 3+1D bosonic topological orders have gappable boundary. (2) All the pointlike excitations in EF topological orders are described by the representations of $G_f=Z_2^f\leftthreetimes_{e_2} G_b$ -- a $Z_2^f$ central extension of a finite group $G_b$ characterized by $e_2\in H^2(G_b,Z_2)$. (3) We find that the EF topological orders are classified by 2+1D anomalous topological orders $\mathcal{A}_b^3$ on their unique canonical boundary. Here $\mathcal{A}_b^3$ is a unitary fusion 2-category with simple objects labeled by $\hat G_b=Z_2^m\leftthreetimes G_b$. $\mathcal{A}_b^3$ also has one invertible fermionic 1-morphism for each object as well as quantum-dimension-$\sqrt 2$ 1-morphisms that connect two objects $g$ and $gm$, where $g\in \hat G_b$ and $m$ is the generator of $Z_2^m$. (4) When $\hat G_b$ is the trivial $Z_2^m$ extension, the EF topological orders are called EF1 topological orders, which is classified by simple data $(G_b,e_2,n_3,\nu_4)$. (5) When $\hat G_b$ is a non-trivial $Z_2^m$ extension, the EF topological orders are called EF2 topological orders, where some intersections of three stringlike excitations must carry Majorana zero modes. (6) Every EF2 topological order with $G_f=Z_2^f\leftthreetimes G_b$ can be associated with a EF1 topological order with $G_f=Z_2^f\leftthreetimes \hat G_b$. (7) We find that all EF topological orders correspond to gauged 3+1D fermionic symmetry protected topological (SPT) orders with a finite unitary symmetry group. (8) We further propose that the general classification of 3+1D topological orders with finite unitary symmetries for bosonic and fermionic systems can be obtained by gauging or partially gauging the finite symmetry group of 3+1D SPT phases of bosonic and fermionic systems.

Highlights

  • The study of topological phases of matter has become a very active field in condensed-matter physics

  • The 2 þ 1D topological order is mathematically described by fusion categories, whose objects correspond to pointlike excitations, and morphisms correspond to physical processes, such as braiding

  • (7) We find that all EF topological orders correspond to gauged 3 þ 1D fermionic symmetry-protected topological (SPT) orders with a finite unitary symmetry group

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Summary

INTRODUCTION

The study of topological phases of matter has become a very active field in condensed-matter physics. We classify 3 þ 1D topological orders whose emergent pointlike excitations are bosons and fermions, which are called EF topological orders. [37] and in this paper classify all 3 þ 1D topological orders in bosonic systems, since there are only two kinds of statistics for pointlike excitations in 3 þ 1D: Bose statistics and Fermi statistics. Since the remote detection is done by braiding, the self-consistency of fusion and braiding plus the remote detectability can totally fix the structure of pointlike and stringlike excitations Those structures, in turn, classify the 3 þ 1D EF topological orders

A list of the results obtained in this paper
Emergence of a group Gf
Unique canonical gapped boundary described by a unitary fusion 2-category
Emergence of Majorana zero modes
A map from EF topological orders to EF1 topological orders
The line of arguments
Dimension reduction of generic topological orders
Condensing all the bosonic pointlike excitations
All simple boundary strings and boundary particles have quantum dimension 1
Fusion of domain-wall strings recovers the group
Unitary fusion 2-category with a single invertible fermionic 1-morphism
The canonical domain wall
The canonical boundary
Define string type using local or nonlocal unitary transformations?
New string type from pSC chain
Zf2 topological order cannot be an EF2 topological order
Partial characterization of EF 2-categories
Majorana zero modes at triple-string junctions
Two necessary conditions for EF2 topological order
Two physical models
Tannaka duality I
Tannaka duality II
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