Publisher's Note: Blast-wave model with two freeze-out temperatures for hadrons produced in relativistic heavy-ion collisions [Phys. Rev. C84, 064905 (2011)]

2011 ◽  
Vol 84 (6) ◽  
Author(s):  
Suk Choi ◽  
Kang Seog Lee
2020 ◽  
Vol 35 (14) ◽  
pp. 2050115 ◽  
Author(s):  
Khusniddin K. Olimov ◽  
Shakhnoza Z. Kanokova ◽  
Kosim Olimov ◽  
Kadyr G. Gulamov ◽  
Bekhzod S. Yuldashev ◽  
...  

The experimental invariant transverse momentum [Formula: see text] spectra of the charged pions and kaons, protons and antiprotons, produced at midrapidity in central (0–10%) Au[Formula: see text]Au collisions at [Formula: see text], central (0–10%) Cu[Formula: see text]Cu collisions at [Formula: see text], central (0–10%) Au[Formula: see text]Au collisions at [Formula: see text], and central (0–5%) Pb[Formula: see text]Pb collisions at [Formula: see text], measured by BRAHMS, STAR and ALICE collaborations, were analyzed using three different transverse expansion (blast-wave) models: Siemens–Rasmussen blast-wave model, Simple transverse flow model, and Simplified (hydro-inspired) blast-wave model of Schnedermann et al. Combined (simultaneous) minimum [Formula: see text] fits of the experimental invariant [Formula: see text] spectra of the charged pions and kaons, protons and antiprotons with the above three model functions were conducted, using the identical selected optimal fitting ranges in [Formula: see text] in each studied collision system, and the values of the average transverse expansion velocity [Formula: see text] and global kinetic freeze-out temperature [Formula: see text] and their dependencies on the collision system [Formula: see text] and [Formula: see text] were extracted. The combined (simultaneous) fits using Hagedorn formula with the (embedded) simple transverse flow describe well the experimental invariant [Formula: see text] spectra of the charged pions, kaons, protons and antiprotons in the whole measured range in region [Formula: see text] in the analyzed central heavy ion collisions at RHIC and LHC, reproducing qualitatively well all the established dependencies of the parameters [Formula: see text] and [Formula: see text] on the collision system [Formula: see text] and [Formula: see text]. The obtained results were compared with those of the previous analyses of high energy heavy ion collisions.


1995 ◽  
Vol 354 (3-4) ◽  
pp. 196-201 ◽  
Author(s):  
L.V. Bravina ◽  
I.N. Mishustin ◽  
N.S. Amelin ◽  
J.P. Bondorf ◽  
L.P. Csernai

2007 ◽  
Vol 16 (07n08) ◽  
pp. 1890-1895 ◽  
Author(s):  
V. K. MAGAS ◽  
L. P. CSERNAI ◽  
E. MOLNAR

The freeze out of the expanding systems, created in relativistic heavy ion collisions, will be discussed. We combine kinetic freeze out equations with Bjorken type system expansion into a unified model. Such a model is a more physical generalization of the earlier simplified non-expanding freeze out models. We shall see that the basic freeze out features, pointed out in the earlier works, are not smeared out by the expansion.


1999 ◽  
Vol 60 (4) ◽  
Author(s):  
L. V. Bravina ◽  
I. N. Mishustin ◽  
J. P. Bondorf ◽  
Amand Faessler ◽  
E. E. Zabrodin

2019 ◽  
Author(s):  
Larissa Bravina ◽  
Y. Kvasiuk ◽  
D. Sachenko ◽  
S Y. Sivoklokov ◽  
O. Vitiuk ◽  
...  

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