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We consider a system of components of bosons, each of which consists of particles, respectively. The bosons are in three dimensions with interactions via a generalized interaction potential which includes the Coulomb interaction. We set the initial condition to describe a mixture condensate, i.e., a tensor product of factorized states. We show that the difference between the many-body Schr"odinger evolution in the mean-field regime and the corresponding -particle dynamics due to a system of Hartree equation is where .

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