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We investigate the contribution of the charm-anticharrm () asymmetry of the proton eigenstate obtained from QCD lattice gauge to the asymmetry of and mesons produced in collisions at large Feynman variables . It is shown that an important tool for the establishing the intrinsic charm (IC) content of the proton is the charm hadron-antihadron asymmetry formed in collisions. Predictions for the asymmetry as function of for different IC probabilities are presented. We show that the interference of the intrinsic Fock state with the standard contribution from the PQCD evolution leads to a large asymmetry at large Feynman .

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