Abstract
AbstractWe introduce a novel approach based on elastic and inelastic scattering rates to extract the hyper-surface of the chemical freeze-out from a hadronic transport model in the energy range from E$$_\mathrm {lab}=1.23$$
lab
=
1.23
AGeV to $$\sqrt{s_\mathrm {NN}}=62.4$$
s
NN
=
62.4
GeV. For this study, the Ultra-relativistic Quantum Molecular Dynamics (UrQMD) model combined with a coarse-graining method is employed. The chemical freeze-out distribution is reconstructed from the pions through several decay and re-formation chains involving resonances and taking into account inelastic, pseudo-elastic and string excitation reactions. The extracted average temperature and baryon chemical potential are then compared to statistical model analysis. Finally we investigate various freeze-out criteria suggested in the literature. We confirm within this microscopic dynamical simulation, that the chemical freeze-out at all energies coincides with $$\langle E\rangle /\langle N\rangle \approx 1$$
⟨
E
⟩
/
⟨
N
⟩
≈
1
GeV, while other criteria, like $$s/T^3=7$$
s
/
T
3
=
7
and $$n_\mathrm {B}+n_{\bar{\mathrm {B}}}\approx 0.12$$
n
B
+
n
B
¯
≈
0.12
fm$$^{-3}$$
-
3
are limited to higher collision energies.
Funder
Helmholtz Forschungsakademie Hessen
Deutscher Akademischer Austauschdienst
Academy of Finland
COST Action
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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