THE HADRONIZATION OF A QUARK-GLUON PLASMA

We consider two scenarios for the expansion of a quark-gluon plasma. I f the evolution is slow enough, the system can remain in equilibrium t hroughout its entire history up to the freeze-out of a hadron gas; for a very rapid expansion, it may break up into hadrons before or at the confinement transition, without ever going through an equilibrium had ron phase. We compare hadron production rates in the two approaches an d show that for a hadronisation temperature T congruent-to 200 MeV and baryonic chemical potential mu(B) less than or similar to 500 MeV, th eir predictions essentially coincide. Present data on strange particle production lead to values in this range and hence cannot provide a di stinction between the two scenarios. Pion, nucleon and non-strange mes on production seem to require a considerably lower freeze-out temperat ure and baryonic chemical potential. In the hadron gas picture, this i s in accord with the difference in mean free path of the different had rons in the medium; it suggests a sequential freeze-out, in which stra nge hadrons stop interacting earlier than non-strange hadrons. In the quark-gluon plasma break-up, the hadronic final state fails to provide the high entropy per baryon observed in non-strange hadron production . The break-up moreover leads to a decrease of the entropy per baryon; hence it must be conceptually modified before it can be considered as a viable hadronisation mechanism.