Abstract

We consider the semi-relativistic system of NN gravitating Bosons with gravitation constant GG. The time evolution of the system is described by the relativistic dispersion law, and we assume the mean-field scaling of the interaction where NN \to \infty and G0G \to 0 while GN=λGN = \lambda fixed. In the super-critical regime of large λ\lambda, we introduce the regularized interaction where the cutoff vanishes as NN \to \infty. We show that the difference between the many-body semi-relativistic Schr\"{o}dinger dynamics and the corresponding semi-relativistic Hartree dynamics is at most of order N1N^{-1} for all λ\lambda, i.e., the result covers the sub-critical regime and the super-critical regime. The NN dependence of the bound is optimal.Comment: 29 page

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