Sharp local propagation of chaos for mean field particles with $W^{-1,\infty}$ kernels
Songbo Wang
TL;DR
This work addresses quantitative propagation of chaos for $N$ diffusive particles with singular mean-field interactions in the $W^{-1,fty}$ class. It develops two complementary hierarchical frameworks: an entropic hierarchy using relative entropy and Fisher information, and an $L^2$/Dirichlet-energy hierarchy, to compare $k$-particle marginals with the tensorized mean-field law. The entropic approach yields global-in-time sharp bounds $H^k_t \,=\, O\left( k^2/N^2 \right)$ (and exponential decay in the 2D viscous vortex regime under weak coupling), while the $L^2$ method provides short-time $D^k_t \,=\, O\left( k^2/N^2 \right)$ controls for fixed $k$ without smallness assumptions. The results extend Lacker to $W^{-1,\infty}$ interactions and provide a robust local PoC theory for singular kernels, including a detailed treatment of inner/outer interaction terms and a set of technical tools (transport inequalities, refined JW lemma, maximum principle). These contributions deepen understanding of mean-field limits in the presence of singular forces and offer new avenues for uniform-in-time results under structural conditions in 2D vortex-type models.
Abstract
We present two methods to obtain $O(1/N^2)$ local propagation of chaos bounds for $N$ diffusive particles in $W^{-1,\infty}$ mean field interaction. This extends the recent finding of Lacker [Probab. Math. Phys., 4(2):377-432, 2023] to the case of singular interactions. The first method is based on a hierarchy of relative entropies and Fisher informations, and applies to the 2D viscous vortex model in the high temperature regime. Time-uniform local chaos bounds are also shown in this case. In the second method, we work on a hierarchy of $L^2$ distances and Dirichlet energies, and derive the desired sharp estimates for the same model in short time without restrictions on the temperature.
