Excitation basis for (3+1)d topological phases

Abstract We consider an exactly solvable model in 3+1 dimensions, based on a finite group, which is a natural generalization of Kitaev’s quantum double model. The corresponding lattice Hamiltonian yields excitations located at torus-boundaries. By cutting open the three-torus, we obtain a manifold b...

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Main Author: Clement Delcamp
Format: Article
Language:English
Published: SpringerOpen 2017-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP12(2017)128
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spelling doaj-f3d53654fbae459aad6d269e1c20348f2020-11-25T02:29:15ZengSpringerOpenJournal of High Energy Physics1029-84792017-12-0120171213310.1007/JHEP12(2017)128Excitation basis for (3+1)d topological phasesClement Delcamp0Perimeter Institute for Theoretical PhysicsAbstract We consider an exactly solvable model in 3+1 dimensions, based on a finite group, which is a natural generalization of Kitaev’s quantum double model. The corresponding lattice Hamiltonian yields excitations located at torus-boundaries. By cutting open the three-torus, we obtain a manifold bounded by two tori which supports states satisfying a higher-dimensional version of Ocneanu’s tube algebra. This defines an algebraic structure extending the Drinfel’d double. Its irreducible representations, labeled by two fluxes and one charge, characterize the torus-excitations. The tensor product of such representations is introduced in order to construct a basis for (3+1)d gauge models which relies upon the fusion of the defect excitations. This basis is defined on manifolds of the form Σ×S1 $$ \varSigma \times {\mathbb{S}}_1 $$, with Σ a two-dimensional Riemann surface. As such, our construction is closely related to dimensional reduction from (3+1)d to (2+1)d topological orders.http://link.springer.com/article/10.1007/JHEP12(2017)128Topological States of MatterAnyonsGauge Symmetry
collection DOAJ
language English
format Article
sources DOAJ
author Clement Delcamp
spellingShingle Clement Delcamp
Excitation basis for (3+1)d topological phases
Journal of High Energy Physics
Topological States of Matter
Anyons
Gauge Symmetry
author_facet Clement Delcamp
author_sort Clement Delcamp
title Excitation basis for (3+1)d topological phases
title_short Excitation basis for (3+1)d topological phases
title_full Excitation basis for (3+1)d topological phases
title_fullStr Excitation basis for (3+1)d topological phases
title_full_unstemmed Excitation basis for (3+1)d topological phases
title_sort excitation basis for (3+1)d topological phases
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-12-01
description Abstract We consider an exactly solvable model in 3+1 dimensions, based on a finite group, which is a natural generalization of Kitaev’s quantum double model. The corresponding lattice Hamiltonian yields excitations located at torus-boundaries. By cutting open the three-torus, we obtain a manifold bounded by two tori which supports states satisfying a higher-dimensional version of Ocneanu’s tube algebra. This defines an algebraic structure extending the Drinfel’d double. Its irreducible representations, labeled by two fluxes and one charge, characterize the torus-excitations. The tensor product of such representations is introduced in order to construct a basis for (3+1)d gauge models which relies upon the fusion of the defect excitations. This basis is defined on manifolds of the form Σ×S1 $$ \varSigma \times {\mathbb{S}}_1 $$, with Σ a two-dimensional Riemann surface. As such, our construction is closely related to dimensional reduction from (3+1)d to (2+1)d topological orders.
topic Topological States of Matter
Anyons
Gauge Symmetry
url http://link.springer.com/article/10.1007/JHEP12(2017)128
work_keys_str_mv AT clementdelcamp excitationbasisfor31dtopologicalphases
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