High baryon densities achievable in the fragmentation regions at RHIC and LHC

Abstract

We use the McLerran-Venugopalan model of the glasma energy-momentum tensor to compute the rapidity loss and excitation energy of the colliding nuclei in the fragmentation regions followed by a space-time picture to obtain their energy and baryon densities. At the top RHIC energy we find baryon densities up to 3 baryons/fm${}^3$, which is 20 times that of atomic nuclei. Assuming the formation of quark-gluon plasma, we find initial temperatures of 200 to 300 MeV and baryon chemical potentials of order 1 GeV. Assuming a roughly adiabatic expansion it would imply trajectories in the $T-\mu$ plane which would straddle a possible critical point.

arXiv comment4 pages, 6 figures, 1 table, Proceedings of Strangeness in Quark Matter 2016

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Cited by in corpus (1)

• Pseudorapidity distribution and decorrelation of anisotropic flow within CLVisc hydrodynamics