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Rigorous Derivation of the Wave Kinetic Equation for $\beta$-FPUT System

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arxiv 2506.02948 v2 pith:GDR6QTUE submitted 2025-06-03 math.AP math-phmath.MP

classification math.APmath-phmath.MP
keywords kineticbetaepsilonequationfputgammasystemwave
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abstract

Wave kinetic theory has been suggested as a way to understand the longtime statistical behavior of the Fermi-Pasta-Ulam-Tsingou (FPUT) system, with the aim of determining the thermalization time scale. The latter has been a major problem since the model was introduced in the 1950s. In this thesis we establish the wave kinetic equation for a reduced evolution equation obtained from the $\beta$-FPUT system by removing the non-resonant terms. We work in the kinetic limit $N\to \infty$ and $\beta\to 0$ under the scaling laws $\beta=N^{-\gamma}$ with $0<\gamma<1$. The result holds up to the sub-kinetic time scale $T=N^{-\epsilon}\min\bigl(N,N^{5\gamma/4}\bigr)=N^{-\epsilon}T_{\mathrm{kin}}^{5/8}$ for $\epsilon\ll 1$, where $T_{\mathrm{kin}}$ represents the kinetic (thermalization) timescale. The novelties of this work include the treatment of non-polynomial dispersion relations, and the introduction of a robust phase renormalization argument to cancel dangerous divergent interactions.

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  1. Sharp decay thresholds in weighted $L^\infty$ for wave kinetic equations with power-law dispersion

    math.AP 2026-07 conditional novelty 6.0 of 10

    Four-wave kinetic equations with dispersion |p|^a and kernel growth |p|^{2β} in 3D are locally well-posed in weighted L∞ exactly above the decay threshold s_c = 4β + 3 − a/2, with ill-posedness below.

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