Abstract

Braiding phases among topological excitations are key data for physically characterizing topological orders. In this paper, we provide a field-theoretical approach towards a complete list of mutually compatible braiding phases of topological orders in (3+1)D spacetime. More concretely, considering a discrete gauge group as input data, topological excitations in this paper are bosonic \particles carrying gauge charges and loops carrying gauge fluxes. Among these excitations, there are three classes of root braiding processes: particle-loop braidings (i.e., the familiar Aharonov-Bohm phase of winding an electric charge around a thin magnetic solenoid), multi-loop braidings [Phys. Rev. Lett. 113, 080403 (2014)], and particle-loop-loop braidings [i.e., Borromean Rings braiding in Phys. Rev. Lett. 121, 061601 (2018)]. A naive way to exhaust all topological orders is to arbitrarily combine these root braiding processes. Surprisingly, we find that there exist illegitimate combinations in which certain braiding phases cannot coexist, i.e., are mutually incompatible. Thus, the resulting topological orders are illegitimate and must be excluded. It is not obvious to identify these illegitimate combinations. But with the help of the powerful (3+1)D topological quantum field theories (TQFTs), we find that illegitimate combinations violate gauge invariance. In this way, we are able to obtain all sets of mutually compatible braiding phases and all legitimate topological orders. To illustrate, we work out all details when gauge groups are $\mathbb{Z}_{N_1},\mathbb{Z}_{N_1}\times\mathbb{Z}_{N_2},\mathbb{Z}_{N_1}\times\mathbb{Z}_{N_2}\times\mathbb{Z}_{N_3}$, and $\mathbb{Z}_{N_1}\times\mathbb{Z}_{N_2}\times\mathbb{Z}_{N_3}\times\mathbb{Z}_{N_4}$. Finally, we concisely discuss compatible braidings and TQFTs in (4+1)D spacetime.

Highlights

  • The order parameter, which is designed for characterizing orders, is one of fundamental concepts of many-body physics

  • Topological orders [1,2,3,4] in gapped systems are characterized by intrinsically nonlocal order parameters, such as adiabatic quantum phases accumulated by braiding topological excitations [5]

  • In this paper, when a gauge group is given, we investigate the compatibility between all three classes of root braiding processes in (3 + 1)D spacetime, i.e., particle-loop braidings, multiloop braidings, and Borromean rings (BR) braidings

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Summary

INTRODUCTION

The order parameter, which is designed for characterizing orders, is one of fundamental concepts of many-body physics. Within each gauge subgroup, e.g., ZNi , Ht2Nhπioerpmefoliidsn2kaπiswwfeohlrle-mndeethdfienbeHydoapnpfaelrlitenicmklieen-nglotaionrpyvapbrairarantiidtciilnseg’osnpterha.3ajesHceteorrey,Hi tγh=eei and an elementary loop mi This braiding phase always exists since it physically encodes the cyclic group structure of ZNi. For the whole gauge group, the root braiding phases of the first class form a set { Hi }G with i = 1, · · · , n. I.e., the particle-loop-loop braiding or BR braiding [45], an elementary particle carrying unit gauge charge of ZNk gauge subgroup moves around two loops (denoted by mi, m2j ) that, respectively, carry unit gauge fluxes of ZNi and ZNj , such that the particle’s trajectory γek and the two loops together form aBR link, or general Brunnian link.

The corresponding
REVIEW ON ROOT BRAIDING PROCESSES AND GAUGE TRANSFORMATIONS
Particle-loop braiding and BdA term
D BD Aei
Borromean rings braiding and AAB term
COMPATIBLE BRAIDING PROCESSES
Results for general gauge groups
INCOMPATIBLE BRAIDING PROCESSES
Incompatibility
A1 d A2
CONCLUSION
A3 d A3
Ni Y idAi
Derivation of incompatibility between A1A2A3A4 and A1A2B4
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