Abstract
This talk will be about the convergence of certain symmetric $N$-particle stochastic control problems towards their mean field limits. After a brief introduction to mean field control, we will mainly discuss the following question: how fast do the value functions $V^N$ for the $N$-particle problems converge towards the value function $U$ of the mean field problem? Or in terms of partial differential equations - how fast do the solutions of certain finite-dimensional Hamilton-Jacobi equations converge to the solution of a corresponding Hamilton-Jacobi equation set on the space of probability measures? If the data is smooth and convex, then $U$ is smooth, and the rate is $O(1/N)$. When the data is not convex, $U$ may fail to be smooth, and the answer is more subtle. On one hand, it has recently been shown (in a joint work of mine with Daudin and Delarue) that if the data is smooth but not convex, the optimal global rate is $O(1/\sqrt{N})$. On the other hand, a recent paper of Cardaliaguet and Souganidis identifies an open and dense set $\mathcal O$ of initial conditions (which we call the region of strong regularity, by analogy with some classical results on first order Hamilton-Jacobi equations) where $U$ is smooth, and it is natural to wonder whether the rate of convergence might be better inside of $\mathcal O$. In an ongoing joint work with Cardaliaguet, Mimikos-Stamatopoulos, and Souganidis, we show that this is indeed the case: the rate is $O(1/N)$ locally uniformly inside the set $\mathcal O$, so the convergence is indeed faster inside $\mathcal O$ than it is outside.