Sharp propagation of chaos in Rényi divergence
Matthew S. Zhang
TL;DR
The paper proves sharp stationary propagation of chaos in $q$-Rényi divergence for interacting diffusion systems under strong isoperimetric conditions and very weak interaction, obtaining $\mathsf{R}_q(\mu^{[k]} \|\pi^{\otimes k}) \lesssim \widetilde{O}\Bigl(\frac{d k^3 q^2}{N^2}\Bigr)$ for large $N$. Building on the hierarchical framework of Lacker (2023), the authors develop a Renyi-specific analysis that leverages a sub-Gaussian score bound and a Lipschitz recursion for conditional measures to control the Rényi Fisher information and related terms. The results extend prior KL-based propagation of chaos to Rényi divergences, with corollaries giving change-of-measure and sampling guarantees and providing evidence for tight $N^{-2}$ rates (at least for moderate $k$). The work relies on strong isoperimetric (LSI/Talagrand) conditions and a notion of very weak interaction, and it outlines potential extensions to dynamics and broader energy functionals, highlighting practical implications for precise tail control and finite-particle approximations.
Abstract
We establish sharp rates for propagation of chaos in Rényi divergences for interacting diffusion systems at stationarity. Building upon the entropic hierarchy established in Lacker (2023), we show that under strong isoperimetry and weak interaction conditions, one can achieve $\mathsf R_q(μ^1 \,\lVert\, π) = \widetilde O(\frac{d q^2}{N^2})$ bounds on the $q$-Rényi divergence.
