1985
DOI: 10.1007/bf01556607
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Multiplicity, momentum and angular characteristics of π− mesons forpC,dC, αC and CC interactions at 4.2 GeV/c per nucleon

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Cited by 46 publications
(16 citation statements)
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“…78]. Combining these experimental findings, one may conclude that the expected deviations for the pion energy Agakishiyev et al [60] distribution shape between pp and the light nuclear interactions that are relevant in astrophysics should not be larger than 30-40 % for collisions with T p ≤ 100 A GeV. Thus, for simplicity I assume here that nucleus-nucleus and nucleon-nucleon collisions with 1 ≤ T p ≤ 100 A GeV have identical pion spectral shape.…”
Section: B Differential Cross Section Dσπ/deπmentioning
confidence: 81%
“…78]. Combining these experimental findings, one may conclude that the expected deviations for the pion energy Agakishiyev et al [60] distribution shape between pp and the light nuclear interactions that are relevant in astrophysics should not be larger than 30-40 % for collisions with T p ≤ 100 A GeV. Thus, for simplicity I assume here that nucleus-nucleus and nucleon-nucleon collisions with 1 ≤ T p ≤ 100 A GeV have identical pion spectral shape.…”
Section: B Differential Cross Section Dσπ/deπmentioning
confidence: 81%
“…As we have mentioned above that all the experimental data have been compared with ones coming from the Dubna version of the cascade model [22]. The model was described in somewhere else [21,23], based on Monte-Carlo simulation, used to explain the common prospects of nucleus-nucleus and hadron-nucleus collisions at relativistic energies.…”
Section: Cascade Evaporation Model (Cem)mentioning
confidence: 99%
“…The x-distribution of the charged particles with maximum values of the x in an event is also considered. All the experimental data were compared with ones coming from the Dubna version of the cascade model and were fitted using the exponential function y=ax+b (a and b are free parameters of fitting) [22].…”
Section: Introductionmentioning
confidence: 99%
“…The 2-m propane bubble chamber was placed in a magnetic field of strength 1.5 T [22,[30][31][32][33][34][35][36]. Three tantalum 181 Ta foils also were placed in the experimental setup of the chamber.…”
Section: The Experimentsmentioning
confidence: 99%
“…The bubble chamber then was irradiated with beams of 2 H and 12 C nuclei accelerated to a momentum of 4.2 GeV/c per nucleon at the Dubna synchrophasotron. The deuterons and 12 C nuclei were made to interact with the carbon nuclei and protons of the propane molecules and the tantalum 181 Ta foils placed in the propane bubble chamber [22,[34][35][36]. Methods of selection of inelastic d + 12 C, 12 C + 12 C, and 12 C + 181 Ta collision events in this experiment were explained in detail in Refs.…”
Section: The Experimentsmentioning
confidence: 99%