Energy dependence in heavy-ion optical-potential elastic scattering

1977 ◽  
Vol 16 (5) ◽  
pp. 1865-1872 ◽  
Author(s):  
R. C. Fuller
1979 ◽  
Vol 320 (2) ◽  
pp. 422-432 ◽  
Author(s):  
R. Donangelo ◽  
L.F. Canto ◽  
Mahir S. Hussein

2003 ◽  
Vol 723 (1-2) ◽  
pp. 93-103 ◽  
Author(s):  
M.A.G. Alvarez ◽  
L.C. Chamon ◽  
M.S. Hussein ◽  
D. Pereira ◽  
L.R. Gasques ◽  
...  

2015 ◽  
Vol 86 ◽  
pp. 00008 ◽  
Author(s):  
Shradha Dubey ◽  
S. Mukherjee ◽  
D. Patel ◽  
Y. K. Gupta ◽  
L. S. Danu ◽  
...  

1988 ◽  
Vol 477 (4) ◽  
pp. 713-722 ◽  
Author(s):  
Wei-hsing Ma ◽  
Shu-ping Zhao ◽  
Zheng-yong Feng ◽  
Chung-kuang Chen

2012 ◽  
Vol 21 (07) ◽  
pp. 1250067 ◽  
Author(s):  
BASUDEB SAHU ◽  
BIDHUBHUSAN SAHU

The nucleus–nucleus potential is expressed phenomenologically by a new radial form as an alternative to the conventional Woods–Saxon form. By virtue of novel representation of the surface diffuseness, the potential added with the electrostatic part generates a unique barrier potential which provides simultaneous explanations of two important mechanisms namely elastic scattering and fusion in a heavy-ion reaction within the framework of optical potential model of scattering and region-wise absorption in analytical form. The drastic falloff of experimental results of fusion cross-section (σ fus ) at extreme sub-barrier energy (E) and its manifestation depicting maximum in S( = Eσ fus e2πη) factor and steep rise in L( = d ln (Eσ fus )/dE) factor are explained with remarkable success.


2019 ◽  
Vol 34 (32) ◽  
pp. 1950259 ◽  
Author(s):  
S. M. Troshin ◽  
N. E. Tyurin

We comment briefly on relations between the elastic and inelastic cross-sections valid for the shadow and reflective modes of the elastic scattering. Those are based on the unitarity arguments. It is shown that the redistribution of the probabilities of the elastic and inelastic interactions (the form of the inelastic overlap function becomes peripheral) under the reflective scattering mode can lead to increasing ratio of [Formula: see text] at the LHC energies. In the shadow scattering mode, the mechanism of this increase is a different one, since the impact parameter dependence of the inelastic interactions probability is central in this mode. A short notice is also given on the slope parameter and the leading contributions to its energy dependence in both modes.


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