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Characteristics of secondary particles associated with the leading protons in n12C and p12C collisions at 3.37GeV incident energy

Kosim OlimovPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, UzbekistanK. G. GulamovPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, UzbekistanV. V. LugovoiPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, UzbekistanS. L. LutpullaevPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, UzbekistanR.N. BekmirzaevJizzakh State Pedagogical Institute, Jizzakh 130100, UzbekistanAlisher K. OlimovPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, UzbekistanAzizjon A. JonzakovJizzakh State Pedagogical Institute, Jizzakh 130100, UzbekistanKhusniddin K. OlimovPhysical-Technical Institute of Uzbekistan Academy of Sciences, Chingiz Aytmatov Street 2B, 100084 Tashkent, Uzbekistan
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Abstract

The new experimental data on characteristics of the secondary particles associated with the leading protons in inelastic interactions of projectile neutrons and protons with target carbon nuclei at incident momentum 4.2[Formula: see text]GeV/c (corresponds to incident kinetic energy 3.37[Formula: see text]GeV) have been presented. The dependencies of the average multiplicities of the charged pions and accompanying protons on longitudinal as well as transverse momenta of the leading protons in [Formula: see text]C and [Formula: see text]C collisions at 4.2[Formula: see text]GeV/c have been investigated. The experimental dependencies have been compared systematically with the Monte Carlo calculations using the modified FRITIOF model. On the whole, the kinematical characteristics of the leading protons in [Formula: see text]C and [Formula: see text]C collisions have proved to be practically the same, even though they are formed as a result of different processes. From a systematic comparison of the experimental data with the model calculations, we could conclude that for a realistic description of the studied experimental dependencies it is probably necessary to take into account the interaction of strings for the case when fragmentation of strings occurs not outside of the nucleus (as it is assumed in the model), but inside and, possibly, on the boundary of the nucleus in the modified FRITIOF model.

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