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Centrality evolution of transverse momentum spectra of primary charged particles produced in high-energy Pb+Pb collisions at the LHC

Khusniddin K. OlimovDepartment of Physics, New Uzbekistan University, Tashkent, UzbekistanI.A. LebedevInstitute of Physics and Technology, Satbayev University, Almaty, KazakhstanAnastasiya FedosimovaInstitute of Nuclear Physics of the Ministry of Energy of Kazakhstan, Almaty, KazakhstanF. H. LiuInstitute of Theoretical Physics, Shanxi University, Taiyuan 030006, P. R. ChinaAzizjon TokhirovPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2, Tashkent 100084, UzbekistanShokhida A. KhudoyberdievaPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2, Tashkent 100084, UzbekistanA. KurbanovDepartment of Natural Sciences, Jizzakh State Pedagogical University, Jizzakh, Uzbekistan
Modern Physics Letters Ajournal2026en
ABI

Аннотация

Evolution of the experimental mid(pseudo)rapidity [Formula: see text] distributions of primary charged particles with changing collision centrality, measured by the ALICE collaboration in the long [Formula: see text] range (up to [Formula: see text]) in [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV, has been analyzed using thermodynamically consistent Tsallis function with embedded transverse flow. The results have been compared with the earlier results coming from simultaneous analysis of short [Formula: see text] range (up to [Formula: see text]) of [Formula: see text] spectra of the charged pions and kaons, protons and antiprotons in [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV at the LHC. Transverse flow has been absent at low [Formula: see text] values and it starts emerging between collision centralities (40–50)% and (30–40)% in [Formula: see text] collisions at [Formula: see text] and between collision centralities (50–60)% and (40–50)% in [Formula: see text] collisions at [Formula: see text]. Kinetic freeze-out temperature, [Formula: see text], has decreased greatly between collision centralities (40–50)% and (30–40)% in [Formula: see text] collisions at [Formula: see text] and between collision centralities (50–60)% and (40–50)% in [Formula: see text] collisions at [Formula: see text]. We have estimated border value of collision centrality for crossover phase transition from the dense hadronic state to that of QGP state (or mixed state of QGP and hadrons) to be [Formula: see text] and [Formula: see text] in [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV, respectively. Non-extensivity parameter q has decreased systematically with increasing [Formula: see text] and [Formula: see text] (with an increase in collision centrality) in both [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV. This denotes systematic increase in degree of system thermalization with increasing centrality of [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV at the LHC, in agreement with similar result of previous works. Strong negative correlation has been obtained between parameter q and [Formula: see text] as well as between parameter q and [Formula: see text] with Pearson correlation coefficient [Formula: see text] in both [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV. Kinetic freeze-out temperature parameter, [Formula: see text], has proved to be strongly anticorrelated with average transverse flow velocity, [Formula: see text], with [Formula: see text] in both [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV, in agreement with analogous result of earlier works. The obtained results have been compared with those extracted in minimum bias [Formula: see text] and [Formula: see text] collisions at [Formula: see text] and 5.02[Formula: see text]TeV.

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