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Centrality dependences of soft and hard components of p<sub>t</sub> distributions of negative pions in <sup>4</sup><font>He</font>+<sup>12</sup><font>C</font> collisions at 4.2A GeV/c

Khusniddin K. OlimovDepartment of Physics, COMSATS Institute of Information Technology, 44000 Islamabad, PakistanAkhtar IqbalDepartment of Physics, COMSATS Institute of Information Technology, 44000 Islamabad, PakistanS. L. LutpullaevPhysical-Technical Institute of Uzbek Academy of Sciences, 100084 Tashkent, UzbekistanSayyed A. HadiDepartment of Physics, Karakoram International University, Gilgit-Baltistan, PakistanВ. В. ГлаголевLaboratory of High Energies, Joint Institute for Nuclear Research, 141980 Dubna, RussiaB. S. YuldashevLaboratory of High Energies, Joint Institute for Nuclear Research, 141980 Dubna, RussiaMahnaz Q. HaseebDepartment of Physics, COMSATS Institute of Information Technology, 44000 Islamabad, Pakistan
ABI

Аннотация

The dependences of the shapes of transverse momentum distributions of the negative pions, produced in minimum bias 4 He + 12 C collisions at a momentum of 4.2 GeV/c per nucleon, on collision centrality and fitting range of p t were analyzed systematically. To study the change in slopes (temperatures) of the p t spectra of π - with changing collision centrality and fitting p t range, the p t spectra, extracted from the experimental data and quark–gluon string model (QGSM) calculations, were fitted by the one- and two-temperature Hagedorn and Boltzmann functions. Fitting of the experimental p t distributions of π - in both the whole p t and p t = 0.1–1.2 GeV/c intervals required the two-temperature functions for adequate description of spectra, in agreement with the previous findings for different sets of colliding nuclei and various energies. On the whole, the absolute values of the extracted temperatures were lower in case of fitting range p t = 0.1–0.7 GeV/c as compared to the fitting interval p t = 0.1–1.2 GeV/c. The one-temperature functions were sufficient for fitting satisfactorily the experimental p t distributions of the negative pions in range p t = 0.1–0.7 GeV/c. In contrast to the experimental temperatures, the extracted QGSM temperatures were not sensitive to collision centrality and fitting range of p t . The collision centrality dependences of the temperatures of soft (p t = 0.1–0.5 GeV/c) and hard (p t = 0.5–1.2 GeV/c) components of the experimental p t distributions of the negative pions in 4 He + 12 C collisions at 4.2A GeV/c were studied separately. The extracted temperatures of both soft and hard components of p t distributions of π - depended on geometry (size) and degree of overlap of colliding nuclei in peripheral, semicentral and central 4 He + 12 C collisions. The temperature of soft p t component of the negative pions was consistently larger in semicentral and central 4 He + 12 C collisions than that in peripheral interactions. The temperature of hard p t component of π - in 4 He + 12 C collisions decreased consistently with an increase in collision centrality. The physical interpretations of the observed centrality dependences of temperature (T) of soft and hard p t components of the negative pions in 4 He + 12 C collisions were given.

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