Evidence for charmonium generation at the phase boundary in ultra-relativistic nuclear coll.pdf
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Evidence for charmonium generation at the phase boundary in ultra-relativistic nuclear coll
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Evidence for charmonium generation at the
phase boundary in ultra-relativistic nuclear
collisions
A. Andronic a, P. Braun-Munzinger a,b, K. Redlich c, J. Stachel d
aGesellschaft fu?r Schwerionenforschung, GSI, D-64291 Darmstadt, Germany
bTechnical University Darmstadt, D-64289 Darmstadt, Germany
cInstitute of Theoretical Physics, University of Wroc law, PL-50204 Wroc law,
Poland
dPhysikalisches Institut der Universita?t Heidelberg, D-69120 Heidelberg, Germany
Abstract
We investigate the transition from suppression to enhancement of J/ψ mesons
produced in ultra-relativistic nuclear collisions in the framework of the statisti-
cal hadronization model. The calculations are confronted with the most recent data
from the RHIC accelerator. This comparison yields first direct evidence for genera-
tion of J/ψ mesons at the phase boundary. Based on the success of this approach
we make specific predictions for LHC energy.
Twenty years ago the J/ψ meson was proposed [1] as a crucial observable for the di-
agnosis of the Quark-Gluon Plasma (QGP) produced in ultra-relativistic nucleus-nucleus
collisions. Since then this probe has been the focus of intense experimental and theoretical
efforts. In the course of these, it was recently realized [2] that even complete J/ψ melting
in the QGP via Debye screening [1] could lead to large J/ψ yields due to production
at the phase boundary (hadronization). Predictions using the corresponding statistical
hadronization model (SHM) [2,3] met with initial success when compared to data. In a
different approach, based on the kinetic model [4], the J/ψ production is described via dy-
namical melting and (re)generation over the whole temporal evolution of the QGP [5,6,7].
Transport model calculations [8,9] were also performed. We note that, in general, the gen-
eration can only take place effectively if the charm quarks reach thermal (not chemical)
equilibrium and are free to trav
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