{ "id": "nucl-th/0308006", "version": "v3", "published": "2003-08-01T19:54:06.000Z", "updated": "2004-09-23T08:22:50.000Z", "title": "Pentaquark baryon production at the Relativistic Heavy Ion Collider", "authors": [ "Lie-Wen Chen", "V. Greco", "C. M. Ko", "S. H. Lee", "W. Liu" ], "comment": "6 pages, 2 figures, revised version, to appear in PLB", "journal": "Phys.Lett. B601 (2004) 34-40", "doi": "10.1016/j.physletb.2004.09.027", "categories": [ "nucl-th", "hep-ex", "hep-ph", "nucl-ex" ], "abstract": "Production of pentaquark $\\Theta^+$ baryons in central relativistic heavy ion collisions is studied in a kinetic model. Assuming that a quark-gluon plasma is produced in the collisions, we first determine the number of $\\Theta^+$ produced from the quark-gluon plasma using a parton coalescence model, and then take into consideration its production and absorption in subsequent hadronic matter via the reactions $KN\\leftrightarrow\\Theta$, $KN\\leftrightarrow\\pi\\Theta$, and $\\piN\\leftrightarrow\\bar K\\Theta$. We find that although the final $\\Theta^+$ number is affected by hadronic interactions, it remains sensitive to the initial number of $\\Theta^+$ produced from the quark-gluon plasma, particularly in the case of a small $\\Theta^+$ width as imposed by the $K^+N$ and $K^+d$ scattering data. Because of small baryon chemical potential in the hot dense matter produced in these collisions, the number of produced anti-$\\Theta$ is only slightly smaller than that of $\\Theta^+$.", "revisions": [ { "version": "v3", "updated": "2004-09-23T08:22:50.000Z" } ], "analyses": { "subjects": [ "25.75.Nq", "25.75.Dw", "25.75.-q" ], "keywords": [ "relativistic heavy ion collider", "pentaquark baryon production", "quark-gluon plasma", "central relativistic heavy ion collisions", "hot dense matter" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 6, "language": "en", "license": "arXiv", "status": "editable", "inspire": 624811 } } }