Correlation estimates for Brownian particles with singular interactions
Mitia Duerinckx, Pierre-Emmanuel Jabin
TL;DR
The paper develops a linearized correlation framework for second-order Langevin particle systems with singular, potentially unbounded interactions in the mean-field regime. By introducing linear correlations H_{N,m} and a tractable BBGKY-type hierarchy, it obtains robust L^2-type bounds and weak convergence results for G_{N,m} under square-integrable kernels, and extends the analysis to the overdamped case. The authors establish a Bogolyubov correction with propagation of chaos at rate N^{−1}, characterize a Gaussian CLT for empirical measure fluctuations via a linearized Dean–Kawasaki SPDE, and, in the bounded-forces regime, derive globally valid, sharper estimates with optimal scaling. These results significantly extend correlation control to singular interaction regimes and provide a rigorous framework for mean-field corrections and fluctuations beyond bounded interactions.
Abstract
We study particle systems with singular pairwise interactions and non-vanishing diffusion in the mean-field scaling. A classical approach to describing corrections to mean-field behavior is through the analysis of correlation functions. For bounded interactions, the optimal estimates on correlations are well known: the $m$-particle correlation function is $G_{N,m}=O(N^{1-m})$ for all $m$. Such estimates, however, have remained out of reach for more singular interactions. In this work, we develop a new framework based on linearized correlation functions, which allows us to derive robust bounds for systems with merely square-integrable interaction kernels, providing the first systematic control of correlations in the singular setting. Although at first not optimal, our estimates can be partially refined a posteriori using the BBGKY hierarchy: in the case of bounded interactions, our method recovers the known optimal estimates with a simplified argument. As key applications, we establish the validity of the Bogolyubov correction to mean field and prove a central limit theorem for the empirical measure, extending these results beyond the bounded interaction regime for the first time.
