scholarly journals On separate chemical freeze-outs of hadrons and light (anti)nuclei in high energy nuclear collisions

2019 ◽  
Vol 1390 ◽  
pp. 012038 ◽  
Author(s):  
K. A. Bugaev ◽  
B. E. Grinyuk ◽  
A. I. Ivanytskyi ◽  
V. V. Sagun ◽  
D. O. Savchenko ◽  
...  
2020 ◽  
Vol 1690 ◽  
pp. 012123
Author(s):  
K A Bugaev ◽  
O V Vitiuk ◽  
B E Grinyuk ◽  
N S Yakovenko ◽  
E S Zherebtsova ◽  
...  

2021 ◽  
Vol 57 (2) ◽  
Author(s):  
O. V. Vitiuk ◽  
K. A. Bugaev ◽  
E. S. Zherebtsova ◽  
D. B. Blaschke ◽  
L. V. Bravina ◽  
...  

AbstractThe recently developed hadron resonance gas model with multicomponent hard-core repulsion is used to address and resolve the long standing problem to describe the light nuclear cluster multiplicities including the hyper-triton measured by the STAR Collaboration, known as the hyper-triton chemical freeze-out puzzle. An improved description for the hadronic and light nuclear cluster data measured by STAR at the collision energy $$\sqrt{s_{NN}} =200$$ s NN = 200 GeV and by ALICE at $$\sqrt{s_{NN}} =2.76$$ s NN = 2.76 TeV is obtained. This is achieved by applying a new strategy of analyzing the light nuclear cluster data and by using the value for the hard-core radius of the (anti-)$$\varLambda $$ Λ hyperons found in earlier work. One of the most striking results of the present work is that for the most probable scenario of chemical freeze-out for the STAR energy the obtained parameters allow to simultaneously reproduce the values of the experimental ratios $$S_3$$ S 3 and $${\overline{S}}_3$$ S ¯ 3 which were not included in the fit.


2006 ◽  
Vol 151 (1) ◽  
pp. 363-366 ◽  
Author(s):  
M. Rybczyński ◽  
Z. Włodarczyk ◽  
O.V. Utyuzh ◽  
G. Wilk

2015 ◽  
Vol 30 (37) ◽  
pp. 1550205 ◽  
Author(s):  
Nirupam Dutta ◽  
Nicolas Borghini

According to the usual application of the sequential-suppression picture to the dynamics of heavy quarkonia in the hot medium formed in ultrarelativistic nuclear collisions, quark–antiquark pairs created in a given bound or unbound state remain in that same state as the medium evolves. We argue that this scenario implicitly assumes an adiabatic evolution of the quarkonia and we show that the validity of the adiabaticity assumption is questionable.


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