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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Online Access: | http://link.springer.com/article/10.1007/JHEP12(2017)128 |
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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 |
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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 |
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AT clementdelcamp excitationbasisfor31dtopologicalphases |
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1724834326701408256 |