Sensibility of grey particle production system to energy and centrality in 60 A and 200 A GeV 16O-Nucleus interactions

被引:9
作者
Abdelsalam, A. [1 ,4 ]
El-Nagdy, M. S. [2 ,4 ]
Badawy, B. M. [3 ,4 ]
Osman, W. [1 ,4 ]
Fayed, M. [1 ,4 ]
机构
[1] Cairo Univ, Fac Sci, Dept Phys, Giza, Egypt
[2] Helwan Univ, Fac Sci, Dept Phys, Helwan, Egypt
[3] Atom Energy Author, Nucl Res Ctr, Reactor Phys Dept, Nasr City, Cairo Governora, Egypt
[4] Cairo Univ, Fac Sci, Mohamed El Nadi High Energy Lab, Giza, Egypt
关键词
Grey particle multiplicity; dependence on target size; dependence on centrality; emission characteristics; nuclear limiting fragmentation; NUCLEUS-NUCLEUS COLLISIONS; RELATIVISTIC HEAVY-IONS; LIMITING FRAGMENTATION; TARGET FRAGMENTATION; EMULSION NUCLEI; GEV-C; PROTONS; MULTIPLICITY; GEV/NUCLEON; MODEL;
D O I
10.1142/S0218301316500348
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The grey particle production following 60 A and 200 A GeV O-16 interactions with emulsion nuclei is investigated at different centralities. The evaporated target fragment multiplicity is voted as a centrality parameter. The target size effect is examined over a wide range, where the C, N and O nuclei present the light target group while the Br and Ag nuclei are the heavy group. In the framework of the nuclear limiting fragmentation hypothesis, the grey particle multiplicity characteristics depend only on the target size and centrality while the projectile size and energy are not effective. The grey particle is suggested to be a multisource production system. The emission direction in the 4 pi space depends upon the production source. Either the exponential decay or the Poisson's peaking curves are the usual characteristic shapes of the grey particle multiplicity distributions. The decay shape is suggested to be a characteristic feature of the source singularity while the peaking shape is a multisource super-position. The sensibility to the centrality varies from a source to other. The distribution shape is identified at each centrality region according to the associated source contribution. In general, the multiplicity characteristics seem to be limited w.r.t. the collision system centrality using light target nuclei. The selection of the black particle multiplicity as a centrality parameter is successful through the collision with the heavy target nuclei. In the collision with the light target nuclei it may be qualitatively better to vote another centrality parameter.
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页数:21
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