Propagation of chaos for multi-species moderately interacting particle systems up to Newtonian singularity
José Antonio Carrillo, Shuchen Guo, Alexandra Holzinger
TL;DR
This work delivers a rigorous, quantitative propagation-of-chaos result for multi-species moderately interacting particle systems with Coulomb/Newtonian singularities, deriving the limiting aggregation-diffusion PDEs without additional particle-level cutoffs. The authors integrate a two-step limiting strategy: a mean-field/relative-entropy transition from the particle system to an intermediate regularised PDE, followed by a PDE-error estimate to the singular limiting system, aided by a stopping-time argument to prove convergence in probability. The main contributions include an algebraic-in-$N$ strong $L^1$ convergence rate, a coupled relative-entropy/$L^2$-distance framework between intermediate and limiting PDEs, and a global well-posedness theory for the multi-species aggregation-diffusion system under small initial data. The results bridge microscopic stochastic dynamics with singular cross-diffusion PDEs applicable to physics, biology, and social dynamics, and lay groundwork for subsequent fluctuation analysis and higher-regularity improvements.
Abstract
We derive a class of multi-species aggregation-diffusion systems from stochastic interacting particle systems via relative entropy method with quantitative bounds. We show an algebraic $L^1$-convergence result using moderately interacting particle systems approximating attractive/repulsive singular potentials up to Newtonian/Coulomb singularities without additional cut-off on the particle level. The first step is to make use of the relative entropy between the joint distribution of the particle system and an approximated limiting aggregation-diffusion system. A crucial argument in the proof is to show convergence in probability by a stopping time argument. The second step is to obtain a quantitative convergence rate to the limiting aggregation-diffusion system from the approximated PDE system. This is shown by evaluating a combination of relative entropy and $L^2$-distance.
