1995
DOI: 10.1103/physrevc.52.356
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Centrality dependence of pion and proton spectra in C+C and C+Ta interactions at 4.2 GeV/cper nucleon

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Cited by 14 publications
(15 citation statements)
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“…The procedure of the generation of a collision event in the QGSM consisted of three steps: (i) defining the configurations of the colliding nucleons, (ii) production of quark-gluon strings, and (iii) the breakup (fragmentation) of strings into observed hadrons. For simulating the nucleonnucleon and pion-nucleon interactions in the QGSM, the binary, "undeveloped" cylindrical, diffractive, cylindrical, and planar topological quark diagrams were used [21][22][23][24]. The binary processes give the main contribution to the QGSM and correspond to a quark rearrangement (in an interacting pair of nucleons) without direct particle emission in the string decay.…”
Section: The Qgsmmentioning
confidence: 99%
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“…The procedure of the generation of a collision event in the QGSM consisted of three steps: (i) defining the configurations of the colliding nucleons, (ii) production of quark-gluon strings, and (iii) the breakup (fragmentation) of strings into observed hadrons. For simulating the nucleonnucleon and pion-nucleon interactions in the QGSM, the binary, "undeveloped" cylindrical, diffractive, cylindrical, and planar topological quark diagrams were used [21][22][23][24]. The binary processes give the main contribution to the QGSM and correspond to a quark rearrangement (in an interacting pair of nucleons) without direct particle emission in the string decay.…”
Section: The Qgsmmentioning
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%
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