1992
DOI: 10.1016/0550-3213(92)90005-v
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The role of the entropy in an expanding hadronic gas

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Cited by 156 publications
(174 citation statements)
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“…[20] and corresponds to a parametrization of a lattice QCD calculation, at high temperatures, smoothly connected to a parametrization of the hadron resonance gas at lower temperatures. At temperatures below T ch = 0.16 GeV, this equation of state follows a partial chemical equilibrium prescription, which assumes that ratios of particle multiplicity remain fixed for all T < T ch [17,21].…”
Section: B Relativistic Dissipative Fluid Dynamicsmentioning
confidence: 99%
“…[20] and corresponds to a parametrization of a lattice QCD calculation, at high temperatures, smoothly connected to a parametrization of the hadron resonance gas at lower temperatures. At temperatures below T ch = 0.16 GeV, this equation of state follows a partial chemical equilibrium prescription, which assumes that ratios of particle multiplicity remain fixed for all T < T ch [17,21].…”
Section: B Relativistic Dissipative Fluid Dynamicsmentioning
confidence: 99%
“…Chemical potentials of the resonance species are determined in accord with the model of partially chemically frozen gas [12]. It assumes that after the chemical freeze-out [13] the effective numbers of particles decaying weakly (and thus slowly) stay fixed while the strong (and therefore fast) interactions stay in equilibrium.…”
Section: The Freeze-out State In Central Collisionsmentioning
confidence: 99%
“…However, it has been discussed whether this is really an appropriate description. Some authors have argued that an over-dense pionic system is created in the initial stage of the collision and that the fireball remains out of equilibrium due to the long relaxation time [31,32]. In other models μ π becomes finite after the number of pions is fixed at the chemical freeze-out but the system further cools and extends [10,33].…”
Section: The Coarse-graining Approachmentioning
confidence: 99%