Heavy-ion fusion cross-section calculations in classical microscopic equations of motion approach

Pramana ◽  
1987 ◽  
Vol 28 (1) ◽  
pp. 41-44 ◽  
Author(s):  
S S Godre ◽  
Y R Waghmare

1985 ◽  
Vol 85 (4) ◽  
pp. 358-358
Author(s):  
F. Porto ◽  
S. Sambataro


2013 ◽  
Vol 22 (02) ◽  
pp. 1350010 ◽  
Author(s):  
M. ISMAIL ◽  
W. M. SEIF

We assume a simple model to describe the ion–ion potential with dynamical change in its surface diffuseness. In particular, this model is used to calculate the heavy-ion fusion cross-section using different values of the surface diffuseness. Both the static and dynamic nuclear Woods–Saxon potentials with diffuseness values ranging between 0.65 fm and 1.3 fm are used to reproduce the fusion cross-sections data of the 19 F +208 Pb and 16 O +154 Sm reactions. The results estimate that there are different physical processes which could contribute to the fusion cross-section with different weights at each energy value. Each of these processes has its own nuclear potential.



1984 ◽  
Vol 30 (6) ◽  
pp. 1962-1965 ◽  
Author(s):  
M. S. Hussein




2004 ◽  
Vol 13 (01) ◽  
pp. 361-366 ◽  
Author(s):  
M. KOWAL ◽  
Z. ŁOJEWSKI

We are studying the potential energy describing the entrance channel of a heavy-ion collisions for the axially symmetric deformed and arbitrarily oriented nuclear shapes. The paper presents an analysis of the influence of different orientations of the deformed ions on the height and shape of the fusion barrier. The net effect of the deformation degree of freedom on the transmission at sub-barrier energies is to enhance the fusion cross section. This problem is very important especially in the perspective of the synthesis of super-heavy elements.



2010 ◽  
Vol 19 (05n06) ◽  
pp. 997-1008 ◽  
Author(s):  
AVAZBEK NASIROV ◽  
GIORGIO GIARDINA ◽  
GIUSEPPE MANDAGLIO ◽  
MARINA MANGANARO ◽  
AKHTAM MUMINOV

The mixing of the quasifission component to the fissionlike cross section causes ambiguity in the quantitative estimation of the complete fusion cross section from the observed angular and mass distributions of the binary products. We show that the partial cross section of quasifission component of binary fragments covers the whole range of the angular momentum values leading to capture. The calculated angular momentum distributions for the compound nucleus and dinuclear system going to quasifission may overlap: competition between complete fusion and quasifission takes place at all values of initial orbital angular momentum. Quasifission components formed at large angular momentum of the dinuclear system can show isotropic angular distribution and their mass distribution can be in mass symmetric region similar to the characteristics of fusion-fission components. As result the unintentional inclusion of the quasifission contribution into the fusion-fission fragment yields can lead to overestimation of the probability of the compound nucleus formation.



1978 ◽  
Vol 74 (1-2) ◽  
pp. 35-38 ◽  
Author(s):  
D.J. Morrissey ◽  
W. Loveland ◽  
R.J. Otto ◽  
G.T. Seaborg


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