Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate

Abstract The rate of entropy production in a classical dynamical system is characterized by the Kolmogorov-Sinai entropy rate h KS given by the sum of all positive Lyapunov exponents of the system. We prove a quantum version of this result valid for bosonic systems with unstable quadratic Hamiltonia...

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Main Authors: Eugenio Bianchi, Lucas Hackl, Nelson Yokomizo
Format: Article
Language:English
Published: SpringerOpen 2018-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP03(2018)025
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spelling doaj-75726dcdc872481e8db885100a19f2fb2020-11-24T22:02:34ZengSpringerOpenJournal of High Energy Physics1029-84792018-03-012018317010.1007/JHEP03(2018)025Linear growth of the entanglement entropy and the Kolmogorov-Sinai rateEugenio Bianchi0Lucas Hackl1Nelson Yokomizo2Institute for Gravitation and the Cosmos & Department of Physics, The Pennsylvania State University, Davey LaboratoryInstitute for Gravitation and the Cosmos & Department of Physics, The Pennsylvania State University, Davey LaboratoryInstitute for Gravitation and the Cosmos & Department of Physics, The Pennsylvania State University, Davey LaboratoryAbstract The rate of entropy production in a classical dynamical system is characterized by the Kolmogorov-Sinai entropy rate h KS given by the sum of all positive Lyapunov exponents of the system. We prove a quantum version of this result valid for bosonic systems with unstable quadratic Hamiltonian. The derivation takes into account the case of time-dependent Hamiltonians with Floquet instabilities. We show that the entanglement entropy S A of a Gaussian state grows linearly for large times in unstable systems, with a rate Λ A ≤ h KS determined by the Lyapunov exponents and the choice of the subsystem A. We apply our results to the analysis of entanglement production in unstable quadratic potentials and due to periodic quantum quenches in many-body quantum systems. Our results are relevant for quantum field theory, for which we present three applications: a scalar field in a symmetry-breaking potential, parametric resonance during post-inflationary reheating and cosmological perturbations during inflation. Finally, we conjecture that the same rate Λ A appears in the entanglement growth of chaotic quantum systems prepared in a semiclassical state.http://link.springer.com/article/10.1007/JHEP03(2018)025Field Theories in Lower DimensionsLattice Quantum Field TheoryQuantum Dissipative Systems
collection DOAJ
language English
format Article
sources DOAJ
author Eugenio Bianchi
Lucas Hackl
Nelson Yokomizo
spellingShingle Eugenio Bianchi
Lucas Hackl
Nelson Yokomizo
Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
Journal of High Energy Physics
Field Theories in Lower Dimensions
Lattice Quantum Field Theory
Quantum Dissipative Systems
author_facet Eugenio Bianchi
Lucas Hackl
Nelson Yokomizo
author_sort Eugenio Bianchi
title Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
title_short Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
title_full Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
title_fullStr Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
title_full_unstemmed Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
title_sort linear growth of the entanglement entropy and the kolmogorov-sinai rate
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-03-01
description Abstract The rate of entropy production in a classical dynamical system is characterized by the Kolmogorov-Sinai entropy rate h KS given by the sum of all positive Lyapunov exponents of the system. We prove a quantum version of this result valid for bosonic systems with unstable quadratic Hamiltonian. The derivation takes into account the case of time-dependent Hamiltonians with Floquet instabilities. We show that the entanglement entropy S A of a Gaussian state grows linearly for large times in unstable systems, with a rate Λ A ≤ h KS determined by the Lyapunov exponents and the choice of the subsystem A. We apply our results to the analysis of entanglement production in unstable quadratic potentials and due to periodic quantum quenches in many-body quantum systems. Our results are relevant for quantum field theory, for which we present three applications: a scalar field in a symmetry-breaking potential, parametric resonance during post-inflationary reheating and cosmological perturbations during inflation. Finally, we conjecture that the same rate Λ A appears in the entanglement growth of chaotic quantum systems prepared in a semiclassical state.
topic Field Theories in Lower Dimensions
Lattice Quantum Field Theory
Quantum Dissipative Systems
url http://link.springer.com/article/10.1007/JHEP03(2018)025
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