Almost global large deviations principle for the KdV equation
Abstract
We study extreme wave formation for the Korteweg-de Vries equation on the torus with random initial data of average size ε. We establish a large deviations principle for the supremum of the solution over arbitrarily long polynomial timescales t ≤ ε−n for any fixed natural number n. This identifies the leading-order asymptotics of the probability of observing unusually large amplitudes. In this integrable setting, the dynamics evolves on invariant tori where Fourier moduli are almost conserved, ruling out mechanisms for extreme wave formation based on resonant energy exchange. As a result, large amplitudes can only arise through coherent structures or dispersive focusing, which corresponds to the quasi-synchronization of many phases. We show that the latter is dominant in the weakly nonlinear regime. Our approach combines a Birkhoff normal form analysis with probabilistic arguments, exploiting the stability of the integrable dynamics to control the probability of phase quasi-synchronization over long timescales.
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BibTeX
@misc{daquino2026almost,
title = {{Almost global large deviations principle for the KdV equation}},
author = {Riccardo Berforini d'Aquino and Ricardo Grande},
howpublished = {HAL},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2605.00484},
eprint = {2605.00484},
archivePrefix = {arXiv},
url = {https://hal.science/hal-05773748v1},
note = {CC BY},
}
RIS
TY - UNPB
TI - Almost global large deviations principle for the KdV equation
AU - Riccardo Berforini d'Aquino
AU - Ricardo Grande
PY - 2026
DA - 2026/10/01
PB - HAL
DO - 10.48550/arxiv.2605.00484
UR - https://hal.science/hal-05773748v1
AB - We study extreme wave formation for the Korteweg-de Vries equation on the torus with random initial data of average size ε. We establish a large deviations principle for the supremum of the solution over arbitrarily long polynomial timescales t ≤ ε^−n for any fixed natural number n. This identifies the leading-order asymptotics of the probability of observing unusually large amplitudes. In this integrable setting, the dynamics evolves on invariant tori where Fourier moduli are almost conserved, ruling out mechanisms for extreme wave formation based on resonant energy exchange. As a result, large amplitudes can only arise through coherent structures or dispersive focusing, which corresponds to the quasi-synchronization of many phases. We show that the latter is dominant in the weakly nonlinear regime. Our approach combines a Birkhoff normal form analysis with probabilistic arguments, exploiting the stability of the integrable dynamics to control the probability of phase quasi-synchronization over long timescales.
ER -