  The present work establishes the mean-field limit of a N-particle system
towards a regularized variant of the relativistic Vlasov-Maxwell system,
following the work of Braun-Hepp [Comm. in Math. Phys. 56 (1977), 101-113] and
Dobrushin [Func. Anal. Appl. 13 (1979), 115-123] for the Vlasov-Poisson system.
The main ingredients in the analysis of this system are (a) a kinetic
formulation of the Maxwell equations in terms of a distribution of
electromagnetic potential in the momentum variable, (b) a regularization
procedure for which an analogue of the total energy - i.e. the kinetic energy
of the particles plus the energy of the electromagnetic field - is conserved
and (c) an analogue of Dobrushin's stability estimate for the
Monge-Kantorovich-Rubinstein distance between two solutions of the regularized
Vlasov-Poisson dynamics adapted to retarded potentials.
