Many-body delocalisation as symmetry breaking

We present a framework in which the transition between a many-body localised (MBL) phase and an ergodic one is symmetry breaking. We consider random Floquet spin chains, expressing their averaged spectral form factor (SFF) as a function of time in terms of a transfer matrix that acts in the space di...

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প্রধান লেখক: Garratt, SJ, Chalker, JT
বিন্যাস: Journal article
ভাষা:English
প্রকাশিত: American Physical Society 2021
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author Garratt, SJ
Chalker, JT
author_facet Garratt, SJ
Chalker, JT
author_sort Garratt, SJ
collection OXFORD
description We present a framework in which the transition between a many-body localised (MBL) phase and an ergodic one is symmetry breaking. We consider random Floquet spin chains, expressing their averaged spectral form factor (SFF) as a function of time in terms of a transfer matrix that acts in the space direction. The SFF is determined by the leading eigenvalues of this transfer matrix. In the MBL phase the leading eigenvalue is unique, as in a symmetry-unbroken phase, while in the ergodic phase and at late times the leading eigenvalues are asymptotically degenerate, as in a system with degenerate symmetry-breaking phases. We identify the broken symmetry of the transfer matrix, introduce a local order parameter for the transition, and show that the associated correlation functions are long-ranged only in the ergodic phase.
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spelling oxford-uuid:f1cdde3e-89a8-425c-89fc-053c4f0625cb2022-03-27T11:58:50ZMany-body delocalisation as symmetry breakingJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:f1cdde3e-89a8-425c-89fc-053c4f0625cbEnglishSymplectic ElementsAmerican Physical Society2021Garratt, SJChalker, JTWe present a framework in which the transition between a many-body localised (MBL) phase and an ergodic one is symmetry breaking. We consider random Floquet spin chains, expressing their averaged spectral form factor (SFF) as a function of time in terms of a transfer matrix that acts in the space direction. The SFF is determined by the leading eigenvalues of this transfer matrix. In the MBL phase the leading eigenvalue is unique, as in a symmetry-unbroken phase, while in the ergodic phase and at late times the leading eigenvalues are asymptotically degenerate, as in a system with degenerate symmetry-breaking phases. We identify the broken symmetry of the transfer matrix, introduce a local order parameter for the transition, and show that the associated correlation functions are long-ranged only in the ergodic phase.
spellingShingle Garratt, SJ
Chalker, JT
Many-body delocalisation as symmetry breaking
title Many-body delocalisation as symmetry breaking
title_full Many-body delocalisation as symmetry breaking
title_fullStr Many-body delocalisation as symmetry breaking
title_full_unstemmed Many-body delocalisation as symmetry breaking
title_short Many-body delocalisation as symmetry breaking
title_sort many body delocalisation as symmetry breaking
work_keys_str_mv AT garrattsj manybodydelocalisationassymmetrybreaking
AT chalkerjt manybodydelocalisationassymmetrybreaking