Measuring FPUT thermalization with Toda integrals

We assess the ergodic properties of the Fermi-Pasta-Ulam-Tsingou-α model for generic initial conditions using a Toda integral. It serves as an adiabatic invariant for the system and a suitable observable to measure its equilibrium time. Over this time scale, the onset of action diffusion results in ergodic temporal fluctuations. We compare this time scale with the inverse of the maximum Lyapunov exponent λ and its saturation time, which are systematically shorter. The Toda integral ergodization/equilibrium time is system size independent for long chains but show dramatic growth when the system size is smaller than a critical one, whose value depends on the energy density. We measure the dependence of energy density on the critical system size and relate this observation to the possible emergence of a Kolmogorov-Arnold-Moser regime. We numerically determine the critical energy density of this regime, finding that it approximately decays as 1/N2 with the number of particles N.

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Publication Details

Journal
Chaos An Interdisciplinary Journal of Nonlinear Science
Published
2025-11-01
DOI
https://doi.org/10.1063/5.0285451
Primary Topic
Quantum many-body systems
Type
article
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article

Measuring FPUT thermalization with Toda integrals

Helen Christodoulidi, Sergej Flach
Chaos An Interdisciplinary Journal of Nonlinear Science
Quantum many-body systems
article

Measuring FPUT thermalization with Toda integrals

Helen Christodoulidi, Sergej Flach
article en

Abstract

We assess the ergodic properties of the Fermi-Pasta-Ulam-Tsingou-α model for generic initial conditions using a Toda integral. It serves as an adiabatic invariant for the system and a suitable observable to measure its equilibrium time. Over this time scale, the onset of action diffusion results in ergodic temporal fluctuations. We compare this time scale with the inverse of the maximum Lyapunov exponent λ and its saturation time, which are systematically shorter. The Toda integral ergodization/equilibrium time is system size independent for long chains but show dramatic growth when the system size is smaller than a critical one, whose value depends on the energy density. We measure the dependence of energy density on the critical system size and relate this observation to the possible emergence of a Kolmogorov-Arnold-Moser regime. We numerically determine the critical energy density of this regime, finding that it approximately decays as 1/N2 with the number of particles N.

Chaos An Interdisciplinary Journal of Nonlinear ScienceVol. 35(11)
Institute for Basic Science (KR), University of Lincoln (GB)
Openalex Percentile: Top 72%
Quantum many-body systems
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