Parameter-free determination of actual temperature at chemical freeze-out in nuclear interactions

1995 ◽  
Author(s):  
A. D. Panagiotou ◽  
G. Mavromanolakis ◽  
J. Tzoulis
Author(s):  
Jamie M. Stafford ◽  
Paolo Alba ◽  
Rene Bellwied ◽  
Valentina Mantovani-Sarti ◽  
Jacquelyn Noronha-Hostler ◽  
...  
Keyword(s):  

2015 ◽  
Vol 97 ◽  
pp. 00019
Author(s):  
V. Mantovani Sarti ◽  
P. Alba ◽  
W. Alberico ◽  
R. Bellwied ◽  
M. Bluhm ◽  
...  

2015 ◽  
Vol 60 (3) ◽  
pp. 181-200 ◽  
Author(s):  
K.A. Bugaev ◽  
◽  
A.I. Ivanytskyi ◽  
D.R. Oliinychenko ◽  
E.G. Nikonov ◽  
...  

2011 ◽  
Vol 8 (8) ◽  
pp. 811-817 ◽  
Author(s):  
D. B. Blaschke ◽  
J. Berdermann ◽  
J. Cleymans ◽  
K. Redlich

Author(s):  
V. Vovchenko ◽  
M. I. Gorenstein ◽  
L. M. Satarov ◽  
H. Stöcker
Keyword(s):  

2020 ◽  
Vol 56 (10) ◽  
Author(s):  
Tom Reichert ◽  
Gabriele Inghirami ◽  
Marcus Bleicher

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.


Open Physics ◽  
2012 ◽  
Vol 10 (6) ◽  
Author(s):  
Frithjof Karsch

AbstractFreeze-out conditions in Heavy Ion Collisions are generally determined by comparing experimental results for ratios of particle yields with theoretical predictions based on applications of the Hadron Resonance Gas model. We discuss here how this model dependent determination of freeze-out parameters may eventually be replaced by theoretical predictions based on equilibrium QCD thermodynamics.


Sign in / Sign up

Export Citation Format

Share Document