Abstract
We consider the J/Ψ propagation in the mixed phase of the quark-gluon plasma and the hot gas of pions. The distortion of the J/Ψ is due solely to inelastic scatterings with the hadron fraction, and no (formation) time is assumed for a [Formula: see text] pair to form a J/Ψ, here. Both the longitudinal and transverse expansions of the matter are taken into account. Also the case of the gas with ρ mesons being included is briefly reported.
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