Universal Dynamical Response to Slow Driving in Chaotic Systems
Abstract
We propose a unified perspective on classical and quantum chaos based on the sensitivity of a system's stationary states to slow driving. We probe this sensitivity via the system's susceptibility to the average protocol speed, which we call the ``speed-Fisher information," and relate it to irreversible entropy production in the system. We show that chaotic dynamics manifests as a divergence of the speed-Fisher information with the protocol time, and that this response is controlled by the perturbation's low-frequency spectral weight. This approach to chaos applies to both classical and quantum Hamiltonian systems, and naturally extends to non-Hamiltonian classical flows. We illustrate this framework with simple classical and quantum examples, along with a non-Hamiltonian flow that qualitatively exhibits analogous low-frequency spectral behavior.
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BibTeX
@misc{karve2026universal,
title = {{Universal Dynamical Response to Slow Driving in Chaotic Systems}},
author = {Nachiket Karve and Nathan Rose and David Campbell and Anatoli Polkovnikov},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2606.23810},
eprint = {2606.23810},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2606.23810},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Universal Dynamical Response to Slow Driving in Chaotic Systems
AU - Nachiket Karve
AU - Nathan Rose
AU - David Campbell
AU - Anatoli Polkovnikov
PY - 2026
DA - 2026/09/28
PB - arXiv
DO - 10.48550/arxiv.2606.23810
UR - https://arxiv.org/abs/2606.23810
AB - We propose a unified perspective on classical and quantum chaos based on the sensitivity of a system's stationary states to slow driving. We probe this sensitivity via the system's susceptibility to the average protocol speed, which we call the ``speed-Fisher information," and relate it to irreversible entropy production in the system. We show that chaotic dynamics manifests as a divergence of the speed-Fisher information with the protocol time, and that this response is controlled by the perturbation's low-frequency spectral weight. This approach to chaos applies to both classical and quantum Hamiltonian systems, and naturally extends to non-Hamiltonian classical flows. We illustrate this framework with simple classical and quantum examples, along with a non-Hamiltonian flow that qualitatively exhibits analogous low-frequency spectral behavior.
ER -