Classification of Interacting Topological Floquet Phases in One Dimension

Periodic driving of a quantum system can enable new topological phases with no analog in static systems. In this paper, we systematically classify one-dimensional topological and symmetry-protected topological (SPT) phases in interacting fermionic and bosonic quantum systems subject to periodic driv...

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Main Authors: Andrew C. Potter, Takahiro Morimoto, Ashvin Vishwanath
Format: Article
Language:English
Published: American Physical Society 2016-10-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.6.041001
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spelling doaj-81a9079c442a4f4e8d9af6fec25996202020-11-24T22:30:24ZengAmerican Physical SocietyPhysical Review X2160-33082016-10-016404100110.1103/PhysRevX.6.041001Classification of Interacting Topological Floquet Phases in One DimensionAndrew C. PotterTakahiro MorimotoAshvin VishwanathPeriodic driving of a quantum system can enable new topological phases with no analog in static systems. In this paper, we systematically classify one-dimensional topological and symmetry-protected topological (SPT) phases in interacting fermionic and bosonic quantum systems subject to periodic driving, which we dub Floquet SPTs (FSPTs). For physical realizations of interacting FSPTs, many-body localization by disorder is a crucial ingredient, required to obtain a stable phase that does not catastrophically heat to infinite temperature. We demonstrate that 1D bosonic and fermionic FSPT phases are classified by the same criteria as equilibrium phases but with an enlarged symmetry group G[over ˜], which now includes discrete time translation symmetry associated with the Floquet evolution. In particular, 1D bosonic FSPTs are classified by projective representations of the enlarged symmetry group H^{2}(G[over ˜],U(1)). We construct explicit lattice models for a variety of systems and then formalize the classification to demonstrate the completeness of this construction. We advocate that a prototypical Z_{2} bosonic FSPT may be realized by very simple Hamiltonians of the type currently available in existing cold atoms and trapped ion experiments.http://doi.org/10.1103/PhysRevX.6.041001
collection DOAJ
language English
format Article
sources DOAJ
author Andrew C. Potter
Takahiro Morimoto
Ashvin Vishwanath
spellingShingle Andrew C. Potter
Takahiro Morimoto
Ashvin Vishwanath
Classification of Interacting Topological Floquet Phases in One Dimension
Physical Review X
author_facet Andrew C. Potter
Takahiro Morimoto
Ashvin Vishwanath
author_sort Andrew C. Potter
title Classification of Interacting Topological Floquet Phases in One Dimension
title_short Classification of Interacting Topological Floquet Phases in One Dimension
title_full Classification of Interacting Topological Floquet Phases in One Dimension
title_fullStr Classification of Interacting Topological Floquet Phases in One Dimension
title_full_unstemmed Classification of Interacting Topological Floquet Phases in One Dimension
title_sort classification of interacting topological floquet phases in one dimension
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2016-10-01
description Periodic driving of a quantum system can enable new topological phases with no analog in static systems. In this paper, we systematically classify one-dimensional topological and symmetry-protected topological (SPT) phases in interacting fermionic and bosonic quantum systems subject to periodic driving, which we dub Floquet SPTs (FSPTs). For physical realizations of interacting FSPTs, many-body localization by disorder is a crucial ingredient, required to obtain a stable phase that does not catastrophically heat to infinite temperature. We demonstrate that 1D bosonic and fermionic FSPT phases are classified by the same criteria as equilibrium phases but with an enlarged symmetry group G[over ˜], which now includes discrete time translation symmetry associated with the Floquet evolution. In particular, 1D bosonic FSPTs are classified by projective representations of the enlarged symmetry group H^{2}(G[over ˜],U(1)). We construct explicit lattice models for a variety of systems and then formalize the classification to demonstrate the completeness of this construction. We advocate that a prototypical Z_{2} bosonic FSPT may be realized by very simple Hamiltonians of the type currently available in existing cold atoms and trapped ion experiments.
url http://doi.org/10.1103/PhysRevX.6.041001
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