In the recent 3, Cesbron and Herda study a Vlasov–Fokker–Planck (VFP) equation with non-symmetric interaction, introduced in physics to model the distribution of electrons in a synchrotron particle accelerator. We make four remarks in view of their work: first, it is noticed in 3 that the free energy classically considered for the (symmetric) VFP equation is not a Lyapunov function in the non-symmetric case, and we will show however that this is still the case for a suitable definition of the free energy (with no explicit expression in general). Second, when the interaction is sufficiently small (in W 1,∞ ), it is proven in 3 that the equation has a unique stationary solution which is locally attractive; in this spirit, we will see that, when the interaction force is Lipschitz with a sufficiently small constant, the convergence is global. Third, we also briefly discuss the mean-field interacting particle system corresponding to the VFP equation which, interestingly, is a non-equilibrium Langevin process. Finally, we will see that, in the small interaction regime, a suitable (explicit) non-linear Fisher information is contracted at constant rate, similarly to the situation of Wasserstein gradient flows for convex functionals (although here the dynamics is not a gradient flow).
Pierre Monmarché (Mon,) studied this question.