The rapidity distribution of the cascade inside deuteron in πd high energy collisions

1983 ◽  
Vol 19 (2) ◽  
pp. 155-158
Author(s):  
D. Kisielewska
2002 ◽  
Vol 80 (5) ◽  
pp. 533-540
Author(s):  
F -H Liu

The pseudorapidity (rapidity) distributions of particles produced in high-energy collisions are analyzed using the revised thermalized cylinder model. The calculated results are compared and found to be in agreement with the experimental data of pp collision and e+e– annihilation. PACS Nos.: 13.85-t, 13.75-n, 13.85Hd, 13.65+i


2014 ◽  
Vol 2014 ◽  
pp. 1-10 ◽  
Author(s):  
Fu-Hu Liu ◽  
Tian Tian ◽  
Jian-Xin Sun ◽  
Bao-Chun Li

Based on the (pseudo)rapidity distribution of final-state particles produced in proton-proton (pp) collisions at high energy, the probability distributions of momenta, longitudinal momenta, transverse momenta (transverse masses), energies, velocities, longitudinal velocities, transverse velocities, and emission angles of the considered particles are obtained in the framework of a multisource thermal model. The number density distributions of particles in coordinate and momentum spaces and related transverse planes, the particle dispersion plots in longitudinal and transverse coordinate spaces, and the particle dispersion plots in transverse momentum plane at the stage of freeze out in high energyppcollisions are also obtained.


2018 ◽  
Vol 171 ◽  
pp. 02005
Author(s):  
Helmut Satz

The relative multiplicities for hadron production in different high energy collisions are in general well described by an ideal gas of all hadronic resonances, except that under certain conditions, strange particle rates are systematically reduced. We show that the suppression factor γs, accounting for reduced strange particle rates in pp, pA and AA collisions at different collision energies, becomes a universal function when expressed in terms of the initial entropy density s0 or the initial temperature T of the produced thermal medium. It is found that γs increases from about 0.5 to 1.0 in a narrow temperature range around the quark-hadron transition temperature Tc ≃ 160 MeV. Strangeness suppression thus disappears with the onset of color deconfinement; subsequently, full equilibrium resonance gas behavior is attained.


2006 ◽  
Vol 73 (2) ◽  
Author(s):  
S. Eden ◽  
J. Tabet ◽  
K. Samraoui ◽  
S. Louc ◽  
B. Farizon ◽  
...  

1988 ◽  
Vol 7 (2) ◽  
pp. 125-129 ◽  
Author(s):  
A Bialas ◽  
K Fialkowski ◽  
R Peschanski

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