1D Many-body localized Floquet systems II: Symmetry-Broken phases
Recent work suggests that a sharp definition of `phase of matter' can be given for periodically driven `Floquet' quantum systems exhibiting many-body localization. In this work we propose a classification of the phases of interacting Floquet localized systems with (completely) spontaneousl...
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| Published in | arXiv.org |
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| Main Authors | , |
| Format | Paper Journal Article |
| Language | English |
| Published |
Ithaca
Cornell University Library, arXiv.org
24.11.2016
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| ISSN | 2331-8422 |
| DOI | 10.48550/arxiv.1602.06949 |
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| Abstract | Recent work suggests that a sharp definition of `phase of matter' can be given for periodically driven `Floquet' quantum systems exhibiting many-body localization. In this work we propose a classification of the phases of interacting Floquet localized systems with (completely) spontaneously broken symmetries -- we focus on the one dimensional case, but our results appear to generalize to higher dimensions. We find that the different Floquet phases correspond to elements of \(Z(G)\), the centre of the symmetry group in question. In a previous paper we offered a companion classification of unbroken, i.e., paramagnetic phases. |
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| AbstractList | Phys. Rev. B 93, 245146 (2016) Recent work suggests that a sharp definition of `phase of matter' can be
given for periodically driven `Floquet' quantum systems exhibiting many-body
localization. In this work we propose a classification of the phases of
interacting Floquet localized systems with (completely) spontaneously broken
symmetries -- we focus on the one dimensional case, but our results appear to
generalize to higher dimensions. We find that the different Floquet phases
correspond to elements of $Z(G)$, the centre of the symmetry group in question.
In a previous paper we offered a companion classification of unbroken, i.e.,
paramagnetic phases. Recent work suggests that a sharp definition of `phase of matter' can be given for periodically driven `Floquet' quantum systems exhibiting many-body localization. In this work we propose a classification of the phases of interacting Floquet localized systems with (completely) spontaneously broken symmetries -- we focus on the one dimensional case, but our results appear to generalize to higher dimensions. We find that the different Floquet phases correspond to elements of \(Z(G)\), the centre of the symmetry group in question. In a previous paper we offered a companion classification of unbroken, i.e., paramagnetic phases. |
| Author | von Keyserlingk, C W Sondhi, S L |
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| BackLink | https://doi.org/10.1103/PhysRevB.93.245146$$DView published paper (Access to full text may be restricted) https://doi.org/10.48550/arXiv.1602.06949$$DView paper in arXiv |
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| DOI | 10.48550/arxiv.1602.06949 |
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| Snippet | Recent work suggests that a sharp definition of `phase of matter' can be given for periodically driven `Floquet' quantum systems exhibiting many-body... Phys. Rev. B 93, 245146 (2016) Recent work suggests that a sharp definition of `phase of matter' can be given for periodically driven `Floquet' quantum systems... |
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| SubjectTerms | Classification Many body interactions Phases Physics - Disordered Systems and Neural Networks Physics - Strongly Correlated Electrons Symmetry |
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| Title | 1D Many-body localized Floquet systems II: Symmetry-Broken phases |
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