Comment on ‘‘Elastic scattering of 318 MeVLi6fromC12andSi28: Unique phenomenological and folding-model potentials’’ and the validity of the M3Y effective interaction

1994 ◽  
Vol 49 (4) ◽  
pp. 2254-2257 ◽  
Author(s):  
G. R. Satchler ◽  
W. G. Love
Keyword(s):  
Elastic Scattering ◽  
Effective Interaction ◽  
Folding Model ◽  
Model Potentials

Optical model and folding model potentials for elastic scattering of 56 MeV polarized deuterons

1986 ◽  
Vol 455 (3) ◽  
pp. 413-433 ◽  
Author(s):  
N. Matsuoka ◽  
H. Sakai ◽  
T. Saito ◽  
K. Hosono ◽  
M. Kondo ◽  
...  
Keyword(s):  
Elastic Scattering ◽  
Optical Model ◽  
Folding Model ◽  
Model Potentials ◽  
Polarized Deuterons

FOLDING MODEL ANALYSIS OF 6He+120Sn ELASTIC SCATTERING

2013 ◽  
Vol 22 (11) ◽  
pp. 1350086 ◽  
Author(s):  
ZAKARIA M. M. MAHMOUD ◽  
AWAD A. IBRAHEEM ◽  
SHERIF R. MOKHTAR
Keyword(s):  
Experimental Data ◽  
Elastic Scattering ◽  
Imaginary Part ◽  
Optical Model ◽  
Effective Interaction ◽  
Phenomenological Analysis ◽  
Folding Model ◽  
The Real ◽  
Hartree Fock ◽  
Double Folding

In this study, the elastic scattering of 6 He projectile from 120 Sn nucleus has been analyzed in terms of optical model (OM). Microscopic double folding (DF) model has been used to generate the real central part of the OM potential. The imaginary part has been restricted to Woods–Saxon phenomenological form. Skyrme–Hartree–Fock, Symmetrized Fermi and Gaussian-Exponential densities for 6 He nucleus while Hartree–Fock–Bogolyubov (HFB) density of 120 Sn nucleus have been used to construct the real DF potential. For the effective interaction, the widely used M3Y has been adopted in the DF procedure. The results of DF have been compared with both literature experimental data and phenomenological analysis.

Elastic scattering of 318 MeVLi6fromC12andSi28: Unique phenomenological and folding-model potentials

1993 ◽  
Vol 47 (2) ◽  
pp. 674-681 ◽  
Author(s):  
A. Nadasen ◽  
T. Stevens ◽  
J. Farhat ◽  
J. Brusoe ◽  
P. Schwandt ◽  
...  
Keyword(s):  
Elastic Scattering ◽  
Folding Model ◽  
Model Potentials

Folding model analysis of α-particle elastic scattering with a semirealistic density-dependent effective interaction

1982 ◽  
Vol 384 (1-2) ◽  
pp. 65-87 ◽  
Author(s):  
A.M. Kobos ◽  
B.A. Brown ◽  
P.E. Hodgson ◽  
G.R. Satchler ◽  
A. Budzanowski
Keyword(s):  
Elastic Scattering ◽  
Effective Interaction ◽  
Model Analysis ◽  
Folding Model ◽  
Density Dependent

Different folding models for 6Li+28Si elastic scattering

2020 ◽  
Vol 29 (09) ◽  
pp. 2050075
Author(s):  
Awad A. Ibraheem ◽  
M. El-Azab Farid ◽  
Eman Abd El-Rahman ◽  
Zakaria M. M. Mahmoud ◽  
Sherif R. Mokhtar
Keyword(s):  
Elastic Scattering ◽  
Optical Potential ◽  
Optical Model ◽  
Effective Interaction ◽  
Text Structure ◽  
Normalization Factor ◽  
Wide Range ◽  
Cluster Density ◽  
Double Folding ◽  
Good Agreement

In this work, the elastic scattering of 6Li+[Formula: see text]Si system at wide range energies from 76 to 318[Formula: see text]MeV is analyzed. The analysis is carried out in the framework of the optical model (OM). Two different methods are adopted for nuclear optical potential of this system. The first method is the double folding cluster (DFC) for the real part supplied with an imaginary part in the Woods–Saxon (WS) form. In the second one, the double folding (DF) model based upon São Paulo potential (SPP) is used as real and imaginary parts each multiplied by a corresponding normalization factor. For [Formula: see text]Si, the full [Formula: see text]-cluster density is considered while the [Formula: see text]-deuteron ([Formula: see text]–[Formula: see text]) structure is considered for 6Li. Therefore, the DFC real central part is calculated by folding both [Formula: see text]–[Formula: see text] and [Formula: see text]–[Formula: see text] effective interaction between target and nuclei over the cluster densities of the target and projectile. The derived renormalized potentials give a successful description of the data. The present results are in good agreement with the previous work. This agreement confirms the validity of the present methods to generate nucleus–nucleus optical potentials.

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