Linear growth of the entanglement entropy and the Kolmogorov-Sinai rate
A bstract 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 Hamiltoni...
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Published in: | The journal of high energy physics Vol. 2018; no. 3; pp. 1 - 70 |
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Main Authors: | , , |
Format: | Journal Article |
Language: | English |
Published: |
Berlin/Heidelberg
Springer Berlin Heidelberg
01-03-2018
Springer Nature B.V SpringerOpen |
Subjects: | |
Online Access: | Get full text |
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Summary: | A
bstract
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. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP03(2018)025 |