Abstract
The experimental ratio of ψ to J/ψ is approximately a constant in pA collisions, but decreases as the transverse energy increases in nucleus-nucleus collisions. These peculiar features can be explained as arising from approximately the same cc¯-baryon absorption cross section for ψ and J/ψ but greater disruption probabilities for ψ than for J/ψ due to the interaction of the cc¯ system with soft particles produced in baryon-baryon collisions.