Double-folding model potential forLi6scattering withHe4: Absence of anomalous reduction factor

1993 ◽  
Vol 48 (2) ◽  
pp. 785-791 ◽  
Author(s):  
T. Sinha ◽  
Subinit Roy ◽  
C. Samanta
Keyword(s):  
Model Potential ◽  
Reduction Factor ◽  
Folding Model ◽  
Double Folding Model ◽  
Double Folding

scholarly journals A comprehensive description of elastic scattering angular distributions for eight different density distribution of 32S nucleus

2020 ◽  
Vol 66 (3 May-Jun) ◽  
pp. 336
Author(s):  
T. Ulucay ◽  
M. Aygun
Keyword(s):  
Elastic Scattering ◽  
Optical Model ◽  
Model Potential ◽  
Angular Distributions ◽  
Folding Model ◽  
Density Distributions ◽  
Double Folding Model ◽  
Optical Model Potential ◽  
Wide Energy ◽  
Double Folding

The elastic scattering angular distributions of 32S projectile by 12C, 27Al, 40Ca, 48Ca, 48Ti, 58Ni, 63Cu, 64Ni, 76Ge, 96Mo and 100Mo targets over the energy range 83.3 - 180 MeV are analyzed in the framework of the double folding model based on the optical model. The real part of the optical model potential is obtained by using double folding model for eight different density distributions of 32S which consist of Ngo, SP, 2pF, G1, G2, S, 3pF, and HFB. The imaginary part of the optical model potential is accepted as the Woods-Saxon (WS) potential. The theoretical results successfully reproduce the experimental data over both a wide energy and a wide target nucleus. Finally, simple and useful formulas which predict imaginary potential depths of each density are derived based on the elastic scattering results.

scholarly journals Nuclear mean field and double-folding model of the nucleus-nucleus optical potential

2016 ◽  
Vol 94 (3) ◽  
Author(s):  
Dao T. Khoa ◽  
Nguyen Hoang Phuc ◽  
Doan Thi Loan ◽  
Bui Minh Loc
Keyword(s):  
Optical Potential ◽  
Mean Field ◽  
Folding Model ◽  
Double Folding Model ◽  
Double Folding

Comparison between different proximity potentials and the double-folding model for spherical–deformed interacting nuclei

2016 ◽  
Vol 94 (1) ◽  
pp. 102-111 ◽  
Author(s):  
M. Ismail ◽  
I.A.M. Abdul-Magead
Keyword(s):  
Coulomb Barrier ◽  
Analytical Formula ◽  
Orientation Angle ◽  
Heavy Ion ◽  
Folding Model ◽  
Deformation Parameters ◽  
Double Folding Model ◽  
Double Folding ◽  
Coulomb Part ◽  
Simple Analytical Formula

The Coulomb barrier parameters have been calculated for a spherical–deformed interacting pair of nuclei using 14 different versions of the proximity approaches and a simple analytical formula for the Coulomb part of the heavy ion potential. The results of these proximity versions have been compared with more accurate results obtained from the double-folding model (DFM). We have considered the interacting pair 48Ca + 238Pu as an example and assumed the presence of the quadrupole, octupole, and hexadecapole deformation parameters for 238Pu. The orientation angle dependence of the Coulomb barrier parameters has been computed for different sets of deformation parameters. We found that the proximity types named Prox77, BW Prox91, AW Prox95, Bass Prox77, and Bass Prox80 are the best ones of the available 14 versions of the proximity approaches for calculating the nuclear part of the interaction potential for a spherical–deformed pair of nuclei.

scholarly journals Double-Folding Nucleus-Nucleus Optical Potential: Parallel MPI and OpenMP Implementations

2020 ◽  
Vol 226 ◽  
pp. 02004
Author(s):  
Maxim Bashashin ◽  
Elena Zemlyanaya ◽  
Konstantin Lukyanov
Keyword(s):  
Total Cross Section ◽  
Cross Section ◽  
Optical Potential ◽  
Folding Model ◽  
The Real ◽  
Folding Nucleus ◽  
Double Folding Model ◽  
Double Folding

The computation of the real part of the nucleus-nucleus optical potential based on the microscopic double-folding model was implemented within both the MPI and OpenMP parallelising techniques. Test calculations of the total cross section of the 6He + 28Si scattering at the energy 50 A MeV show that both techniques provide significant comparable speedup of the calculations.

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