Multiple particle production in proton-proton collisions at energies available at the Large Hadron Collider

On Antiproton Production in 158 GeV/cProton-Carbon Collisions and Nuclear Temperature of Interacting System

“…Combined with the previous works [15,16,[21][22][23][24][25][26][27] analyzed by the multisource thermal model, we guess the energy behavior of some parameters of the model here. For a given projectile-target impacting system, the rapidity shifts of the cylinders increase slowly with the logarithmic center-of-mass energy and do not depend obviously on the centrality.…”

“…Besides, the transverse mass spectra of protons, pions, kaons, Lambdas, and Antilambdas produced in Au-Au collisions at 2A, 4A, 6A, and 8A GeV and Pb-Pb collisions at 20A, 30A, 40A, 80A, and 158A GeV were studied [23]. The pseudorapidity distributions of charged particles produced in -collisions at 0.053, 0.2, 0.54, 0.546, 0.63, 0.9, and 1.8 TeV; the pseudorapidity and multiplicity distributions of charged particles produced in -collisions at 0.9, 2.36, and 7 GeV; and the pseudorapidity distributions of charged particles produced in Pb-Pb collisions at 2.76A TeV were studied too [24][25][26][27]. We would like to say that the multisource thermal model used in the present work describes different particles produced in different collisions at different energies.…”