Defining classical and quantum chaos through adiabatic transformations

Fuente: arXiv
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Autori principali: Kim, Hyeongjin, Lim, Cedric, Matirko, Kirill, Polkovnikov, Anatoli, Flynn, Michael O.
Natura: Preprint
Pubblicazione: 2024
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author Kim, Hyeongjin
Lim, Cedric
Matirko, Kirill
Polkovnikov, Anatoli
Flynn, Michael O.
author_facet Kim, Hyeongjin
Lim, Cedric
Matirko, Kirill
Polkovnikov, Anatoli
Flynn, Michael O.
contents We propose a formalism which defines chaos in both quantum and classical systems in an equivalent manner by means of \textit{adiabatic transformations}. The complexity of adiabatic transformations which preserve classical time-averaged trajectories (quantum eigenstates) in response to Hamiltonian deformations serves as a measure of chaos. This complexity is quantified by the (properly regularized) fidelity susceptibility. Physically this measure quantifies long time instabilities of physical observables due to small changes in the Hamiltonian of the system. Our exposition clearly showcases the common structures underlying quantum and classical chaos and allows us to distinguish integrable, chaotic but non-thermalizing, and ergodic/mixing regimes. We apply the fidelity susceptibility to a model of two coupled spins and demonstrate that it successfully predicts the universal onset of chaos, both for finite spin $S$ and in the classical limit $S\to\infty$. Interestingly, we find that finite $S$ effects are anomalously large close to integrability.
format Preprint
id arxiv_https___arxiv_org_abs_2401_01927
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Defining classical and quantum chaos through adiabatic transformations
Kim, Hyeongjin
Lim, Cedric
Matirko, Kirill
Polkovnikov, Anatoli
Flynn, Michael O.
Statistical Mechanics
Chaotic Dynamics
Quantum Physics
We propose a formalism which defines chaos in both quantum and classical systems in an equivalent manner by means of \textit{adiabatic transformations}. The complexity of adiabatic transformations which preserve classical time-averaged trajectories (quantum eigenstates) in response to Hamiltonian deformations serves as a measure of chaos. This complexity is quantified by the (properly regularized) fidelity susceptibility. Physically this measure quantifies long time instabilities of physical observables due to small changes in the Hamiltonian of the system. Our exposition clearly showcases the common structures underlying quantum and classical chaos and allows us to distinguish integrable, chaotic but non-thermalizing, and ergodic/mixing regimes. We apply the fidelity susceptibility to a model of two coupled spins and demonstrate that it successfully predicts the universal onset of chaos, both for finite spin $S$ and in the classical limit $S\to\infty$. Interestingly, we find that finite $S$ effects are anomalously large close to integrability.
title Defining classical and quantum chaos through adiabatic transformations
topic Statistical Mechanics
Chaotic Dynamics
Quantum Physics
url https://arxiv.org/abs/2401.01927