Bloch theorem in the presence of an additional conserved charge

The Bloch theorem is a general theorem restricting the persistent current associated with a conserved U(1) charge in a ground state or in a thermal equilibrium. It gives an upper bound of the magnitude of the current density, which is inversely proportional to the system size. In a recent paper, Els...

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Main Author: Haruki Watanabe
Format: Article
Language:English
Published: American Physical Society 2022-01-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.4.013043
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author Haruki Watanabe
author_facet Haruki Watanabe
author_sort Haruki Watanabe
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description The Bloch theorem is a general theorem restricting the persistent current associated with a conserved U(1) charge in a ground state or in a thermal equilibrium. It gives an upper bound of the magnitude of the current density, which is inversely proportional to the system size. In a recent paper, Else and Senthil applied the argument for the Bloch theorem to a generalized Gibbs ensemble, assuming the presence of an additional conserved charge, and predicted a nonzero current density in the nonthermal steady state [Else and Senthil, Phys. Rev. B 104, 205132 (2021)2469-995010.1103/PhysRevB.104.205132]. In this paper, we provide a complementary derivation based on the canonical ensemble, given that the additional charge is strictly conserved within the system by itself. Furthermore, using the example where the additional conserved charge is the momentum operator, we discuss that the persistent current tends to vanish when the system is in contact with an external momentum reservoir in the comoving frame of the reservoir.
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spelling doaj.art-458fe530132045a9af82c55125fbaa762024-04-12T17:17:19ZengAmerican Physical SocietyPhysical Review Research2643-15642022-01-014101304310.1103/PhysRevResearch.4.013043Bloch theorem in the presence of an additional conserved chargeHaruki WatanabeThe Bloch theorem is a general theorem restricting the persistent current associated with a conserved U(1) charge in a ground state or in a thermal equilibrium. It gives an upper bound of the magnitude of the current density, which is inversely proportional to the system size. In a recent paper, Else and Senthil applied the argument for the Bloch theorem to a generalized Gibbs ensemble, assuming the presence of an additional conserved charge, and predicted a nonzero current density in the nonthermal steady state [Else and Senthil, Phys. Rev. B 104, 205132 (2021)2469-995010.1103/PhysRevB.104.205132]. In this paper, we provide a complementary derivation based on the canonical ensemble, given that the additional charge is strictly conserved within the system by itself. Furthermore, using the example where the additional conserved charge is the momentum operator, we discuss that the persistent current tends to vanish when the system is in contact with an external momentum reservoir in the comoving frame of the reservoir.http://doi.org/10.1103/PhysRevResearch.4.013043
spellingShingle Haruki Watanabe
Bloch theorem in the presence of an additional conserved charge
Physical Review Research
title Bloch theorem in the presence of an additional conserved charge
title_full Bloch theorem in the presence of an additional conserved charge
title_fullStr Bloch theorem in the presence of an additional conserved charge
title_full_unstemmed Bloch theorem in the presence of an additional conserved charge
title_short Bloch theorem in the presence of an additional conserved charge
title_sort bloch theorem in the presence of an additional conserved charge
url http://doi.org/10.1103/PhysRevResearch.4.013043
work_keys_str_mv AT harukiwatanabe blochtheoreminthepresenceofanadditionalconservedcharge