  In this article we show, in a concise manner, a result of uniform in time
propagation of chaos for non exchangeable systems of particles interacting
according to a random graph. Provided the interaction is Lipschitz continuous,
the restoring force satisfies a general one-sided Lipschitz condition (thus
allowing for non-convex confining potential) and the graph is dense enough, we
use a coupling method suggested by Eberle known as reflection coupling to
obtain uniform in time mean-field limit with bounds that depend explicitly on
the graph structure.
