Role of nuclear surface vibrations in low energy heavy ion collisions

1986 ◽  
Vol 324 (2) ◽  
pp. 139-146
Author(s):  
K. Nishinohara ◽  
N. Takigawa
1980 ◽  
Vol 57 (2) ◽  
pp. 205-214 ◽  
Author(s):  
A. R. Farhan ◽  
H. Überall ◽  
O. Dragún ◽  
E. Maqueda

2012 ◽  
Vol 57 (8) ◽  
pp. 796
Author(s):  
N.K. Dhiman

We consider the cluster decay of 56Ni* formed in heavy-ion collisions, by using different parameters proposed by different authors for the Fermi density distribution and the nuclear radius. Our study reveals that different technical parameters do not alter significantly the structure of fractional yields. The cluster decay half-lives of different clusters lie within ±10% for different Fermi density parameters and nuclear radii and, therefore, justify the current set of parameters used in the literature for the calculation of cluster decays.


2020 ◽  
Vol 102 (5) ◽  
Author(s):  
Sudhir Pandurang Rode ◽  
Partha Pratim Bhaduri ◽  
Amaresh Jaiswal ◽  
Ankhi Roy

2018 ◽  
Vol 2018 ◽  
pp. 1-8
Author(s):  
Z. J. Jiang ◽  
Dongfang Xu ◽  
Yan Huang

In heavy ion collisions, charged particles come from two parts: the hot and dense matter and the leading particles. In this paper, the hot and dense matter is assumed to expand according to the hydrodynamic model including phase transition and decouples into particles via the prescription of Cooper-Frye. The leading particles are as usual supposed to have Gaussian rapidity distributions with the number equaling that of participants. The investigations of this paper show that, unlike low energy situations, the leading particles are essential in describing the pseudorapidity distributions of charged particles produced in high energy heavy ion collisions. This might be due to the different transparencies of nuclei at different energies.


Author(s):  
Lu Guo ◽  
Gao-Feng Dai ◽  
En-Guang Zhao ◽  
Shan-Gui Zhou

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