Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions

Abstract Matrix Product States (MPSs) provide a powerful framework to study and classify gapped quantum phases — symmetry-protected topological (SPT) phases in particular — defined in one dimensional lattices. On the other hand, it is natural to expect that gapped quantum phases in the limit of zero...

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Main Authors: Ken Shiozaki, Shinsei Ryu
Format: Article
Language:English
Published: SpringerOpen 2017-04-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP04(2017)100
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spelling doaj-cfddb7f6bda247b982efc05ce2f216122020-11-25T00:27:51ZengSpringerOpenJournal of High Energy Physics1029-84792017-04-012017414710.1007/JHEP04(2017)100Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensionsKen Shiozaki0Shinsei Ryu1Department of Physics, University of Illinois at Urbana ChampaignJames Franck Institute and Kadanoff Center for Theoretical Physics, University of ChicagoAbstract Matrix Product States (MPSs) provide a powerful framework to study and classify gapped quantum phases — symmetry-protected topological (SPT) phases in particular — defined in one dimensional lattices. On the other hand, it is natural to expect that gapped quantum phases in the limit of zero correlation length are described by topological quantum field theories (TFTs or TQFTs). In this paper, for (1+1)-dimensional bosonic SPT phases protected by symmetry G, we bridge their descriptions in terms of MPSs, and those in terms of G-equivariant TFTs. In particular, for various topological invariants (SPT invariants) constructed previously using MPSs, we provide derivations from the point of view of (1+1) TFTs. We also discuss the connection between boundary degrees of freedom, which appear when one introduces a physical boundary in SPT phases, and “open” TFTs, which are TFTs defined on spacetimes with boundaries.http://link.springer.com/article/10.1007/JHEP04(2017)100Topological Field TheoriesTopological States of MatterGlobal SymmetriesLattice Quantum Field Theory
collection DOAJ
language English
format Article
sources DOAJ
author Ken Shiozaki
Shinsei Ryu
spellingShingle Ken Shiozaki
Shinsei Ryu
Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
Journal of High Energy Physics
Topological Field Theories
Topological States of Matter
Global Symmetries
Lattice Quantum Field Theory
author_facet Ken Shiozaki
Shinsei Ryu
author_sort Ken Shiozaki
title Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
title_short Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
title_full Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
title_fullStr Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
title_full_unstemmed Matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
title_sort matrix product states and equivariant topological field theories for bosonic symmetry-protected topological phases in (1+1) dimensions
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-04-01
description Abstract Matrix Product States (MPSs) provide a powerful framework to study and classify gapped quantum phases — symmetry-protected topological (SPT) phases in particular — defined in one dimensional lattices. On the other hand, it is natural to expect that gapped quantum phases in the limit of zero correlation length are described by topological quantum field theories (TFTs or TQFTs). In this paper, for (1+1)-dimensional bosonic SPT phases protected by symmetry G, we bridge their descriptions in terms of MPSs, and those in terms of G-equivariant TFTs. In particular, for various topological invariants (SPT invariants) constructed previously using MPSs, we provide derivations from the point of view of (1+1) TFTs. We also discuss the connection between boundary degrees of freedom, which appear when one introduces a physical boundary in SPT phases, and “open” TFTs, which are TFTs defined on spacetimes with boundaries.
topic Topological Field Theories
Topological States of Matter
Global Symmetries
Lattice Quantum Field Theory
url http://link.springer.com/article/10.1007/JHEP04(2017)100
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