{ "id": "nucl-th/9609025", "version": "v1", "published": "1996-09-10T14:36:26.000Z", "updated": "1996-09-10T14:36:26.000Z", "title": "$J/Ψ$ suppression in nuclear collisions at SPS energies", "authors": [ "W. Cassing", "C. M. Ko" ], "comment": "9 pages, LaTeX, plus 4 postscript figures, submitted to Phys. Lett. B", "journal": "Phys.Lett. B396 (1997) 39-44", "doi": "10.1016/S0370-2693(97)00115-9", "categories": [ "nucl-th" ], "abstract": "We have carried out a first calculation of $J/\\Psi$ production from nuclear collisions within the covariant transport approach HSD, which has been very successful in describing both hadronic and electromagnetic observables from heavy-ion collisions at intermediate and high energies. The production of $J/\\Psi$'s is based on the Lund string fragmentation model, while its interactions with hadrons are included by conventional cascade-type two-body collisions. Adopting 6 mb for the $J/\\Psi$-baryon cross sections and 3 mb for the $J/\\Psi$-meson cross sections above the $D\\bar{D}$ threshold, we find that data on $J/\\Psi$ suppression from both proton-nucleus and nucleus-nucleus collisions (including Pb + Pb) can be explained without assuming the formation of a quark-gluon plasma in these collisions. Our microscopic studies thus confirm the suggestion of Gavin et al. that $J/\\Psi$ suppression observed in nuclear collisions is largely due to absorption by comovers, i.e., the produced mesons.", "revisions": [ { "version": "v1", "updated": "1996-09-10T14:36:26.000Z" } ], "analyses": { "subjects": [ "25.75.+r", "24.10.Jv" ], "keywords": [ "nuclear collisions", "sps energies", "suppression", "covariant transport approach hsd", "conventional cascade-type two-body collisions" ], "tags": [ "journal article" ], "publication": { "journal": "Physics Letters B", "year": 1997, "month": "Feb", "volume": 396, "pages": 39 }, "note": { "typesetting": "LaTeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "inspire": 423150, "adsabs": "1997PhLB..396...39C" } } }