Jet Quenching in Dense Matter
Jet Quenching in Dense Matter
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DOI:
10.1016/0370-2693(90)91409-5
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发表时间:
1990-07
影响因子:
4.4
通讯作者:
M. Gyulassy;M. Plümer
中科院分区:
文献类型:
--
作者:
M. Gyulassy;M. Plümer
The quenching of hard jets in ultrarelativistic nuclear collisions is estimated emphasizing its sensitivity to possible changes in the energy loss mechanism in a quark gluon plasma.We calculate the attenuation of hard jet production in ultra-relativistic nuclear collisions and consider its sensitivity to changes in the energy loss mechanisms, dE/dx, in dense matter. In particular, we consider the consequences of a possible sudden decrease of dE/dx near the quark-gluon plasma phase transition temperature. We find that such a change decreases the rate of quenching with increasing A and may under favorable conditions lead to one of the signatures of that transition. In any case, hard jets provide a powerful" external" probe of the transient dense matter produced in such reactions because their production rates are calculable with perturbative QCD [l] up to a slowly varying correction factor J {rv 2. The main difficulty is that those rates are very small and large soft and mini-jet background fluctuations [2, 3] may complicate their detection. Previous jet calculations [4, 5, 6] for nuclear collisions considered enhanced acoplanarity of jets as a probe of multiple scattering in dense matter. Unfortunately, as emphasized in [5, 6], increased acoplanarity is expected to occur in both confined and deconfined phases of dense matter. A reduction of dE/dx with increasing density would, on the other hand, be a novel effect that could only occur if there were a dramatic change in the nature of quark interactions at very high densities. While we cannot prove that such a decrease is necessarily associated with the QCD de confinement transition, we motivate that possibility by reviewing recent lattice" data" and by showing that radiative energy loss is suppressed for high energy jets. The jet attenuation factor is then calculated varying generously dE/dx and taking into account large uncertainties in the time-evolution of ultrarelativistic nuclear collisions.