Entropic Chaos of Mixed Mean-Field Jump Processes
Tau Shean Lim, Shuoning Zhang
TL;DR
The paper develops a comprehensive entropy-based framework for mixed mean-field jump processes, including PDMPs, to prove entropic propagation of chaos as the number of particles grows. It introduces an abstract generator $\mathcal{L}(\mu)=\mathcal{K}+\mathcal{A}(\mu)$ with nonlinear mean-field dependence, and establishes well-posedness of mean-field evolution alongside explicit $O(1/N)$ relative-entropy bounds between the $N$-particle law and the mean-field product law. The core is a generalized concentration inequality (via a second-order bound) that closes the entropy method under first- and second-order bounded-difference conditions on the mean-field kernel, enabling quantitative propagation of chaos. The results apply to both PDMP-type and jump-driven mean-field dynamics, include averaged-in-N analyses, and provide explicit conditions under which entropic chaos and L1-chaos hold, with illustrative multi-body and $\mathbb{R}^k$-parametrized kernels.
Abstract
This paper studies a class of mixed mean-field jump processes on an abstract state space $Π$, together with their associated $N$-particle systems. The dynamics consist of the superposition of an independent Markovian component and a bounded mean-field jump interaction; in particular, piecewise deterministic Markov processes (PDMPs) with mean-field interactions are covered by this framework. Under a second-order bounded difference condition on the mean-field jump kernel, we establish entropic propagation of chaos as $N \to \infty$. In particular, we obtain an explicit qualitative bound on the relative entropy between the law of the $N$-particle system and the product measure induced by the mean-field limit. The proof relies on the second-order concentration inequality introduced in Götze and Sambale, 2020.
