TY - JOUR
T1 - How much strangeness production is there in ultrarelativistic nucleus-nucleus collisions?
AU - Kapusta, J.
AU - Mekjian, A.
PY - 1986
Y1 - 1986
N2 - Strangeness production has been proposed as a signal for the formation of a quark-gluon plasma in ultrarelativistic nucleus-nucleus collisions. We address this problem in the framework of Bjorkens model for the longitudinal hydrodynamic expansion of baryon-free matter. Different scenarios are considered for the assumed first-order phase transition from QCD plasma into hadrons, including a slow transition via the Maxwell construction of coexisting phases, and a rapid transition from supercooling followed by reheating. The rate equations for strange-quark and kaon abundances are solved numerically. With the most likely set of parameters, the K-/- ratio is about three times larger than in p»p collisions at the same energy. This results primarily from the large rate constant in the hadron phase and from the long time spent in this phase. Thus, the K-/- ratio may not be a direct signal for the formation of quark-gluon plasma; however, it may be an indirect signal, since the system would not live nearly as long if the quark-gluon plasma had not been formed initially.
AB - Strangeness production has been proposed as a signal for the formation of a quark-gluon plasma in ultrarelativistic nucleus-nucleus collisions. We address this problem in the framework of Bjorkens model for the longitudinal hydrodynamic expansion of baryon-free matter. Different scenarios are considered for the assumed first-order phase transition from QCD plasma into hadrons, including a slow transition via the Maxwell construction of coexisting phases, and a rapid transition from supercooling followed by reheating. The rate equations for strange-quark and kaon abundances are solved numerically. With the most likely set of parameters, the K-/- ratio is about three times larger than in p»p collisions at the same energy. This results primarily from the large rate constant in the hadron phase and from the long time spent in this phase. Thus, the K-/- ratio may not be a direct signal for the formation of quark-gluon plasma; however, it may be an indirect signal, since the system would not live nearly as long if the quark-gluon plasma had not been formed initially.
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U2 - 10.1103/PhysRevD.33.1304
DO - 10.1103/PhysRevD.33.1304
M3 - Article
AN - SCOPUS:6644227763
SN - 1550-7998
VL - 33
SP - 1304
EP - 1313
JO - Physical review D: Particles and fields
JF - Physical review D: Particles and fields
IS - 5
ER -