Pseudorapidity (rapidity) distribution of shower particles in relativistic nucleus-nucleus collisions

1999 ◽  
Vol 112 (10) ◽  
pp. 1167-1179 ◽  
Author(s):  
F. H. Liu
2016 ◽  
Vol 25 (04) ◽  
pp. 1650025 ◽  
Author(s):  
Z. J. Jiang ◽  
J. Wang ◽  
Y. Huang

The charged particles produced in nucleus–nucleus collisions come from leading particles and those frozen out from the hot and dense matter created in collisions. The leading particles are conventionally supposed having Gaussian rapidity distributions normalized to the number of participants. The hot and dense matter is assumed to expand according to the unified hydrodynamics, a hydro model which unifies the features of Landau and Hwa–Bjorken model, and freeze out into charged particles from a time-like hypersurface with a proper time of [Formula: see text]. The rapidity distribution of this part of charged particles can be derived analytically. The combined contribution from both leading particles and unified hydrodynamics is then compared against the experimental data performed by BNL-RHIC-PHOBOS Collaboration in different centrality Cu–Cu collisions at [Formula: see text] and 62.4[Formula: see text]GeV, respectively. The model predictions are consistent with experimental measurements.


2003 ◽  
Vol 91 (18) ◽  
Author(s):  
Charalampos Anastasiou ◽  
Lance Dixon ◽  
Kirill Melnikov ◽  
Frank Petriello

2000 ◽  
Vol 15 (24) ◽  
pp. 1497-1501 ◽  
Author(s):  
FU-HU LIU

The negatively charged particle rapidity distribution in nucleus–nucleus collisions at high energy has been described by the thermalized cylinder picture. The calculated results are compared and found to be in agreement with the experimental data of the reactions 16 O + Au at 60A and 200A GeV, 32 S + Ag and S at 200A GeV, and 208 Pb + Pb at 158A GeV bombarding energies.


Author(s):  
Imtiyaz A. Najar ◽  
W. Bari

In this study, we have performed a detailed analysis of genuine pion correlations and fluctuations in terms of the normalized factorial comulant moments of second and third orders, [Formula: see text] and [Formula: see text], in case of [Formula: see text]O–AgBr interactions at [Formula: see text][Formula: see text]A and [Formula: see text][Formula: see text]A GeV/c. The experimental results are compared with the predictions of AMPT and UrQMD model simulated events. The UrQMD model reproduces the trends in experimental results but the strength of correlation is much smaller. However, the AMPT model does not also replicate all features of the experimental data. The genuine two-particle and three-particle correlations are found to become weaker with the increase in momentum of the projectile nucleus.


1987 ◽  
Vol 461 (1-2) ◽  
pp. 465-486 ◽  
Author(s):  
A. Sandoval ◽  
A. Bamberger ◽  
D. Bangert ◽  
J. Bartke ◽  
H. Bialkowska ◽  
...  

1999 ◽  
Vol 42 (8) ◽  
pp. 845-851 ◽  
Author(s):  
Xiaorong Wang ◽  
An Tai ◽  
Benhao Sa ◽  
Xu Cai

1979 ◽  
Vol 88 (1-2) ◽  
pp. 189-191 ◽  
Author(s):  
P.J. Jain ◽  
G. Das ◽  
B.T. Cheng ◽  
Y. Aliakbar

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