Abstract

We revisit the problem of boundary excitations at a topological boundary or junction defects between topological boundaries in nonchiral bosonic topological orders in 2+1 dimensions. Based on physical considerations, we derive a formula that relates the fusion rules of the boundary excitations and the "half-linking" number between condensed anyons and confined boundary excitations. This formula is a direct analogue of the Verlinde formula. We also demonstrate how these half-linking numbers can be computed in explicit Abelian and non-Abelian examples. As a fundamental property of topological orders and their allowed boundaries, this should also find applications in the search for suitable platforms realizing quantum computing devices.

Highlights

  • We revisit the problem of boundary excitations at a topological boundary or junction defects between topological boundaries in nonchiral bosonic topological orders in 2 þ 1 dimensions

  • These objects are intimately related to topological defect lines in conformal field theories (CFT’s), which have been extensively studied e.g., in [6,7,8,9,10,11,12]

  • Topological orders have found applications in quantum computing, given their robustness against decoherence, and it has been proposed in the literature that topological defects might be a more convenient candidate to realize universal computing [13]

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Summary

Introduction

We revisit the problem of boundary excitations at a topological boundary or junction defects between topological boundaries in nonchiral bosonic topological orders in 2 þ 1 dimensions. Gapped boundaries can be described by anyon condensation [1,3,15,16,17,18,19,20,21,22]. For a given nonchiral bulk phase B in 2 þ 1 dimensions, there could be multiple different gapped boundaries, each characterized by a distinct pattern of anyon condensation.

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