Quantum coherence controls the nature of equilibration in coupled
chaotic systems
- URL: http://arxiv.org/abs/2204.07561v1
- Date: Fri, 15 Apr 2022 17:33:44 GMT
- Title: Quantum coherence controls the nature of equilibration in coupled
chaotic systems
- Authors: Jethin J. Pulikkottil, Arul Lakshminarayan, Shashi C. L. Srivastava,
Maximilian F. I. Kieler, Arnd B\"acker, Steven Tomsovic
- Abstract summary: Quantum coherence of the initial product states in the uncoupled eigenbasis can be viewed as a resource for equilibration and approach to thermalization.
Results are given for four distinct perturbation strength regimes, the ultra-weak, weak, intermediate, and strong regimes.
Maximally coherent initial states thermalize for any perturbation strength in spite of the fact that in the ultra-weak perturbative regime the underlying eigenstates of the system have a tensor product structure and are not at all thermal-like.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: A bipartite system whose subsystems are fully quantum chaotic and coupled by
a perturbative interaction with a tunable strength is a paradigmatic model for
investigating how isolated quantum systems relax towards an equilibrium. It is
found that quantum coherence of the initial product states in the uncoupled
eigenbasis can be viewed as a resource for equilibration and approach to
thermalization as manifested by the entanglement. Results are given for four
distinct perturbation strength regimes, the ultra-weak, weak, intermediate, and
strong regimes. For each, three types of initially unentangled states are
considered, coherent random-phase superpositions, random superpositions, and
eigenstate products. A universal time scale is identified involving the
interaction strength parameter. Maximally coherent initial states thermalize
for any perturbation strength in spite of the fact that in the ultra-weak
perturbative regime the underlying eigenstates of the system have a tensor
product structure and are not at all thermal-like; though the time taken to
thermalize tends to infinity as the interaction vanishes. In contrast to the
widespread linear behavior, in this regime the entanglement initially grows
quadratically in time.
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