Mean field limits of interacting particle systems with positive stable jumps

This note is a companion article to the recent paper [Löcherbach, et al. Electronic J. Probab. (2025) in press]. We consider mean field systems of interacting particles. Each particle jumps with a jump rate depending on its position. When jumping, a macroscopic quantity is added to its own position. Moreover, simultaneously, all other particles of the system receive a small positive random kick which is distributed according to a one-sided α−stable law and scaled in N−1/α, where 0 < α < 1. In between successive jumps of the system, the particles follow a deterministic flow with drift depending on their position and on the empirical measure of the total system. In a more general framework where jump amplitudes and state space do not need to be non-negative, we have shown in [Löcherbach, et al. Electronic J. Probab. (2025) in press] that the mean field limit of this system is a McKean-Vlasov type process which is solution of a non-linear SDE, driven by an α−stable process. Moreover we have obtained in [Löcherbach, et al. Electronic J. Probab. (2025) in press] an upper bound for the strong rate of convergence with respect to some specific distance disregarding big jumps of the limit stable process. In the present note we consider the specific situation where all jump amplitudes are positive, and particles take values in ℝ+. We show that in this case it is possible to improve upon the error bounds obtained in [Löcherbach, et al. Electronic J. Probab. (2025) in press] by using an adhoc distance obtained after applying a concave space transform to the trajectories. The distance we propose here takes into account the big jumps of the limit α−stable subordinator.