dorsal/arxiv
View SchemaTight bounds on recurrence time in closed quantum systems
| Authors | Marcin Kotowski, Michał Oszmaniec |
|---|---|
| Categories | |
| ArXiv ID | 2601.10409vv1 |
| URL | https://arxiv.org/abs/2601.10409 |
| License | http://creativecommons.org/licenses/by/4.0/ |
Abstract
The evolution of an isolated quantum system inevitably exhibits recurrence: the state returns to the vicinity of its initial condition after finite time. Despite its fundamental nature, a rigorous quantitative understanding of recurrence has been lacking. We establish upper bounds on the recurrence time, $t_{\mathrm{rec}} \lesssim t_{\mathrm{exit}}(\epsilon)(1/\epsilon)^d$, where $d$ is the Hilbert-space dimension, $\epsilon$ the neighborhood size, and $t_{\mathrm{exit}}(\epsilon)$ the escape time from this neighborhood. For pure states evolving under a Hamiltonian $H$, estimating $t_{\mathrm{exit}}$ is equivalent to an inverse quantum speed limit problem: finding upper bounds on the time a time-evolved state $\psi_t$ needs to depart from the $\epsilon$-vicinity of the initial state $\psi_0$. We provide a partial solution, showing that under mild assumptions $t_{\mathrm{exit}}(\epsilon) \approx \epsilon /\sqrt{ \Delta(H^2)}$, with $\Delta(H^2)$ the Hamiltonian variance in $\psi_0$. We show that our upper bound on $t_{\mathrm{rec}}$ is generically saturated for random Hamiltonians. Finally, we analyze the impact of coherence of the initial state in the eigenbasis of $H$ on recurrence behavior.
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"abstract": "The evolution of an isolated quantum system inevitably exhibits recurrence: the state returns to the vicinity of its initial condition after finite time. Despite its fundamental nature, a rigorous quantitative understanding of recurrence has been lacking. We establish upper bounds on the recurrence time, $t_{\\mathrm{rec}} \\lesssim t_{\\mathrm{exit}}(\\epsilon)(1/\\epsilon)^d$, where $d$ is the Hilbert-space dimension, $\\epsilon$ the neighborhood size, and $t_{\\mathrm{exit}}(\\epsilon)$ the escape time from this neighborhood. For pure states evolving under a Hamiltonian $H$, estimating $t_{\\mathrm{exit}}$ is equivalent to an inverse quantum speed limit problem: finding upper bounds on the time a time-evolved state $\\psi_t$ needs to depart from the $\\epsilon$-vicinity of the initial state $\\psi_0$. We provide a partial solution, showing that under mild assumptions $t_{\\mathrm{exit}}(\\epsilon) \\approx \\epsilon /\\sqrt{ \\Delta(H^2)}$, with $\\Delta(H^2)$ the Hamiltonian variance in $\\psi_0$. We show that our upper bound on $t_{\\mathrm{rec}}$ is generically saturated for random Hamiltonians. Finally, we analyze the impact of coherence of the initial state in the eigenbasis of $H$ on recurrence behavior.",
"arxiv_id": "2601.10409",
"authors": [
"Marcin Kotowski",
"Micha\u0142 Oszmaniec"
],
"categories": [
"quant-ph"
],
"license": "http://creativecommons.org/licenses/by/4.0/",
"title": "Tight bounds on recurrence time in closed quantum systems",
"url": "https://arxiv.org/abs/2601.10409",
"version": "v1"
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