Heavy resonance production in high energy nuclear collisions
| dc.creator | Seibert, David | |
| dc.creator | Fai, George | |
| dc.date | 1994-07-07 | |
| dc.date.accessioned | 2026-07-07T11:15:13Z | |
| dc.date.available | 2026-07-07T11:15:13Z | |
| dc.description | We estimate freezeout conditions for $s$, $c$, and $b$ quarks in high energy nuclear collisions. Freezeout is due either to loss of thermal contact, or to particles ``wandering'' out of the region of hot matter. We then develop a thermal recombination model in which both single-particle (quark and antiquark) and two-particle (quark-antiquark) densities are conserved. Conservation of two-particle densities is necessary because quarks and antiquarks are always produced in coincidence, so that the local two-particle density can be much larger than the product of the single-particle densities. We use the freezeout conditions and recombination model to discuss heavy resonance production at zero baryon density in high energy nuclear collisions. | |
| dc.description | revtex, 15 pages, no figures, KSUCNR-009-94 | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9407014 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9407014 | |
| dc.identifier | Phys.Rev.C50:2532-2539,1994 | |
| dc.identifier | doi:10.1103/PhysRevC.50.2532 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/192323 | |
| dc.subject | Nuclear Theory | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Heavy resonance production in high energy nuclear collisions | |
| dc.type | text |