The multiplicity of particle production from hadron-hadron and nucleus-nucleus interaction

Abstract

The particle production in hadron-nucleon (h-N), hadron-nucleus (h-A) and nucleus-nucleus (A-A

Shower and Slow Particle Productions in Nucleus-Nucleus Collisions at High Energy

“…Others concern the thermal characteristics of final-state particles and fragments. One of these thermal models is the multisource thermal model, proposed to explain the multiplicity and angular distributions, based on the assumption that many emission sources are assumed to be formed in the interactions [19][20][21][22][23][24][25][26][27][28][29][30]. The aim of the present research is to check the model validity for describing the basic characteristics of particle production in the interactions of nuclei with emulsion at 4.1-4.5 A GeV/c, mainly beams of 4.1 A GeV/c 22 Ne and 4.5 A GeV/c ( 4 He, 12 C, 16 O, and 28 Si) from Dubna Synchrophasotron.…”