Strangeness enhancement and strangeness suppression in nuclear collisions at 200 GeV/N

1992 ◽  
Vol 55 (3) ◽  
pp. 491-495 ◽  
Author(s):  
Helena Biaŀkowska ◽  
Marek Gaździcki ◽  
Waldemar Retyk ◽  
Ewa Skrzypczak
1991 ◽  
Vol 525 ◽  
pp. 221-226 ◽  
Author(s):  
R. Stock ◽  
J. Baechler ◽  
J. Bartke ◽  
H. Bialkowska ◽  
R. Bock ◽  
...  

2022 ◽  
Vol 258 ◽  
pp. 05010
Author(s):  
Mariia Mitrankova ◽  
Alexander Berdnikov ◽  
Yaroslav Berdnikov ◽  
Dmitry Kotov ◽  
Iurii Mitrankov

The measurements of light hadron production in small collision systems (such as p+Al, p+Au, d+Au, 3He+Au) may allow to explore the quarkgluon plasma formation and to determine the main hadronization mechanism in the considered collisions. Such research has become particularly crucial with the observation of the light hadrons collective behavior in p/d/3He+Au collisions at √SNN = 200 GeV and in p+Al collisions at the same energy at forward and backward rapidities. Among the large variety of light hadrons, ϕ meson is of particular interest since its production is sensitive to the presence of the quark-gluon plasma. The paper presents the comparison of the obtained experimental results on ϕ meson production to different light hadron production in p+Al and 3He+Au at √SNN = 200 GeV at midrapidity. The comparisons of ϕ meson production in p+Al, p+Au, d+Au, and 3He+Au collisions at √SNN = 200 GeV at midrapidity to theoretical models predictions (PYTHIA model and default and string melting versions of the AMPT model) are also provided. The results suggest that the QGP can be formed in p/d/3He+Au collisions, but the volume and lifetime of the produced medium might be insufficient for observation of strangeness enhancement effect. Conceivably, the main hadronization mechanism of ϕ meson production in p+Al collisions is fragmentation, while in p/d/3He+Au collisions this process occurs via coalescence.


2018 ◽  
Vol 172 ◽  
pp. 04004
Author(s):  
Cesar L. da Silva

The use of probes containing heavy quarks is one of the pillars for the study of medium formed in high energy nuclear collisions. The conceptual ideas formulated more than two decades ago, such as quark mass hierarchy of the energy that the probe lose in the media and color screening of bound heavy quarkonia states, have being challenged by the measurements performed at RHIC and LHC. A summary of the most recent experimental observations involving charm and bottom quarks in pp, pA, and AA collisions from collisions energies extending from √sNN =200 GeV to 8 TeV is presented. This manuscript also discuss possibilities of new measurements which can be at reach with increased statistics and detector upgrades.


2020 ◽  
Vol 240 ◽  
pp. 07006
Author(s):  
Kian Hwee Lim ◽  
Aik Hui Chan ◽  
Choo Hiap Oh

A phenomenological model describing the transverse energy distribution (ET) of nuclear collisions is first studied in detail by fitting it on ET data for O-Pb collisions at √sNN = 200 GeV per nucleon obtained from the NA35 collaboration. Next, the model is used to fit the ET data for Pb-Pb collisions at LHC energies of √sNN = 2.76 TeV per nucleon obtained from the ATLAS collaboration. From the fits, we determine an upper bound for the energy density for Pb-Pb collisions at LHC energies of √sNN = 2.76 TeV per nucleon.


2012 ◽  
Vol 108 (7) ◽  
Author(s):  
G. Agakishiev ◽  
M. M. Aggarwal ◽  
Z. Ahammed ◽  
A. V. Alakhverdyants ◽  
I. Alekseev ◽  
...  

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