Abstract

The hard contributions to the heavy quarkonium-nucleon cross sections are calculated based on the QCD factorization theorem and the nonrelativistic quarkonium model. We evaluate the nonperturbative part of these cross sections which dominates at sNN20\sqrt{s_{NN}}\approx 20 GeV at the Cern Super Proton Synchrotron (SPS) and becomes a correction at sNN6\sqrt{s_{NN}}\approx 6 TeV at the CERN Large Hadron Collider (LHC). \J production at the CERN SPS is well described by hard QCD, when the larger absorption cross sections of the χ\chi states predicted by QCD are taken into account. We predict an AA-dependent polarization of the χ\chi states. The expansion of small wave packets is discussed.Comment: 13 pages REVTEX, 1 table, 2 PostScript, corrected some typo

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