Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems

Entanglement in a pure state of a many-body system can be characterized by the R\'enyi entropies $S^{(\alpha)}=\ln\textrm{tr}(\rho^\alpha)/(1-\alpha)$ of the reduced density matrix $\rho$ of a subsystem. These entropies are, however, difficult to access experimentally and can typically be deter...

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Main Author: Maximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael Fleischhauer
Format: Article
Language:English
Published: SciPost 2020-06-01
Series:SciPost Physics
Online Access:https://scipost.org/SciPostPhys.8.6.083
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spelling doaj-f8e995627f0847cc9e39c2afae06c76c2020-11-25T03:02:39ZengSciPostSciPost Physics2542-46532020-06-018608310.21468/SciPostPhys.8.6.083Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systemsMaximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael FleischhauerEntanglement in a pure state of a many-body system can be characterized by the R\'enyi entropies $S^{(\alpha)}=\ln\textrm{tr}(\rho^\alpha)/(1-\alpha)$ of the reduced density matrix $\rho$ of a subsystem. These entropies are, however, difficult to access experimentally and can typically be determined for small systems only. Here we show that for free fermionic systems in a Gaussian state and with particle number conservation, $\ln S^{(2)}$ can be tightly bound---from above and below---by the much easier accessible R\'enyi number entropy $S^{(2)}_N=-\ln \sum_n p^2(n)$ which is a function of the probability distribution $p(n)$ of the total particle number in the considered subsystem only. A dynamical growth in entanglement, in particular, is therefore always accompanied by a growth---albeit logarithmically slower---of the number entropy. We illustrate this relation by presenting numerical results for quenches in non-interacting one-dimensional lattice models including disorder-free, Anderson-localized, and critical systems with off-diagonal disorder.https://scipost.org/SciPostPhys.8.6.083
collection DOAJ
language English
format Article
sources DOAJ
author Maximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael Fleischhauer
spellingShingle Maximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael Fleischhauer
Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
SciPost Physics
author_facet Maximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael Fleischhauer
author_sort Maximilian Kiefer-Emmanouilidis, Razmik Unanyan, Jesko Sirker, Michael Fleischhauer
title Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
title_short Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
title_full Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
title_fullStr Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
title_full_unstemmed Bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
title_sort bounds on the entanglement entropy by the number entropy in non-interacting fermionic systems
publisher SciPost
series SciPost Physics
issn 2542-4653
publishDate 2020-06-01
description Entanglement in a pure state of a many-body system can be characterized by the R\'enyi entropies $S^{(\alpha)}=\ln\textrm{tr}(\rho^\alpha)/(1-\alpha)$ of the reduced density matrix $\rho$ of a subsystem. These entropies are, however, difficult to access experimentally and can typically be determined for small systems only. Here we show that for free fermionic systems in a Gaussian state and with particle number conservation, $\ln S^{(2)}$ can be tightly bound---from above and below---by the much easier accessible R\'enyi number entropy $S^{(2)}_N=-\ln \sum_n p^2(n)$ which is a function of the probability distribution $p(n)$ of the total particle number in the considered subsystem only. A dynamical growth in entanglement, in particular, is therefore always accompanied by a growth---albeit logarithmically slower---of the number entropy. We illustrate this relation by presenting numerical results for quenches in non-interacting one-dimensional lattice models including disorder-free, Anderson-localized, and critical systems with off-diagonal disorder.
url https://scipost.org/SciPostPhys.8.6.083
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