THE HADRONIZATION OF A QUARK-GLUON PLASMA

被引:65
作者
CLEYMANS, J
REDLICH, K
SATZ, H
SUHONEN, E
机构
[1] UNIV BIELEFELD,FAK PHYS,W-4800 BIELEFELD 1,GERMANY
[2] WROCLAW UNIV,INST THEORET PHYS,PL-50205 WROCLAW,POLAND
[3] CERN,DIV THEORY,CH-1211 GENEVA 23,SWITZERLAND
[4] UNIV OULU,DEPT THEORET PHYS,SF-90570 OULU,FINLAND
来源
ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS | 1993年 / 58卷 / 02期
关键词
D O I
10.1007/BF01560356
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We consider two scenarios for the expansion of a quark-gluon plasma. If the evolution is slow enough, the system can remain in equilibrium throughout 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 hadron phase. We compare hadron production rates in the two approaches and show that for a hadronisation temperature T congruent-to 200 MeV and baryonic chemical potential mu(B) less than or similar to 500 MeV, their predictions essentially coincide. Present data on strange particle production lead to values in this range and hence cannot provide a distinction between the two scenarios. Pion, nucleon and non-strange meson production seem to require a considerably lower freeze-out temperature and baryonic chemical potential. In the hadron gas picture, this is in accord with the difference in mean free path of the different hadrons in the medium; it suggests a sequential freeze-out, in which strange 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.
引用
收藏
页码:347 / 355
页数:9
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