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Multiplicities of forward-backward particles in S-32-emulsion interactions at 4.5 A GeV/c
Faculty
Science
Year:
2002
Type of Publication:
Article
Pages:
1375-1389
Authors:
Shaat, EA, Abdelsalam, A, Rashed, N, Osman, W, Ali-Mossa, N, Abou-Mousa, Z, Osman, OM, Badawy, BM, El-Falaky, E
DOI:
10.1088/0954-3899/28/6/317
Journal:
JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS IOP PUBLISHING LTD
Volume:
28
Research Area:
Physics
ISSN
ISI:000176449200019
Keywords :
Multiplicities , forward-backward particles , S-32-emulsion interactions , , , GeV/c
Abstract:
An exclusive study of the characteristics of the interactions accompanied by the backward emission (theta(Lab) > 90degrees) of relativistic and fast hadrons in the collisions of 4.5 A GeV/c S-32 beam with emulsion nuclei is carried out. The experimental multiplicity distributions of different particles emitted in the forward (theta(Lab) < 90degrees) and backward hemispheres due to the interactions with the two emulsion components (CNO, AgBr) are presented and analysed. The correlations between the multiplicities of the different emitted particles are also investigated. This study reveals that there are signatures for a collective mechanism, which plays a role in the production of particles in the backward and hemisphere. Hence, the backward multiplicity distribution of the emitted shower or grey particles at 4,5 A GeV/c incident momentum can be represented by a decay exponential law formula independent of the projectile size. The exponent of the power was found to increase with decreasing target size. The experimental data favour the idea that the backward particles were emitted due to the decay of the system in the latter stage of the reaction, While the mean values of the shower particles emitted in the forward hemisphere (n(s)(f)) are strongly dependent on the projectile size and incident energy, the mean value of the multiplicity of the shower particles flying into the backward hemisphere (n(s)(b)) are found to be only a function of the target size (i.e. impact parameter). Therefore, the results yield quite interesting information regarding the mechanism of the backward particle production in heavy ion interactions. The present data are believed to support the mechanism, which considers the backward particle production as a consequence of the isotropic decay of a highly excited target system, in its rest frame, after the forward particle emission.
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