The extent to which geometrical effects contribute to the production and su
ppression of the J/psi and q (q) over bar minijet pairs in general is inves
tigated for high-energy heavy-ion collisions at SPS,RHIC, and LHC energies.
For the energy range under investigation, the geometrical effects referred
to are shadowing and antishadowing, respectively. Due to those effects, th
e parton distributions in nuclei deviate from the naive extrapolation from
the free nucleon result: f(A)not equal Af(N). The strength of the shadowing
/antishadowing effect increases with the mass number. Therefore it is inter
esting to see the difference between cross sections for,e.g., S+U vs Pb+Pb
at SPS. The recent NA50 results for the survival probability of produced J/
psi's has attracted great attention and are often interpreted as a signatur
e of a quark gluon plasma. This paper will present a fresh look on hard QCD
effects for the charmonium production level. It is shown that the apparent
suppression of J/psi's must also be linked to the production process. Due
to the uncertainty in the shadowing of gluons the suppression of charmonium
states might not give reliable information on a created plasma phase at th
e collider energies now available. The consequences of shadowing effects fo
r the x(F) distribution of J/psi's at root s=20 GeV, root s=200 GeV, and ro
ot s=6 TeV are calculated for some relevant combinations of nuclei, as well
as the p(T) distribution of minijets at midrapidity for N-f=4 in the final
state. [S0556-2813(99)04205-3].