Studying of the Nucleus-Nucleus Interaction Using Wave Function of the Nucleus and Hyperspherical Formalism

2016 ◽  
Vol 71 (11) ◽  
pp. 979-984 ◽  
Author(s):  
Fatemeh Pakdel ◽  
Ali Akbar Rajabi

AbstractThe current study presents the results of the use of the wave function of a nucleus in place of the nucleus density distribution to calculate the nucleus-nucleus interaction potential. The wave function is obtained by solving the D-dimensional wave equation using the hyperspherical formalism. The interaction potential between two nuclei is calculated using the double folding model. The numerical results for the interaction potential and the scattering cross section are presented to evaluate the formalism used to calculate the nucleus wave function.

2019 ◽  
Vol 35 (09) ◽  
pp. 2050050
Author(s):  
Laleh Nickhah ◽  
Ali Akbar Rajabi ◽  
Majid Hamzavi

In this paper, we examine the distribution of nuclei’s charge (the quadrupole moment of nuclei) for stable nuclei with [Formula: see text] when interacting with the [Formula: see text]O nuclei. The interaction potential between the nuclei was achieved using the double-folding method. The wave functions of the interacting nuclei were replaced by the density functions in the double-folding model. The wave functions of the interacting nuclei were obtained through the D-dimensional Schrödinger equation with the pseudo-Coulomb potential plus ring-shaped potential by the Nikiforov–Uvarov solution method.


2020 ◽  
Vol 226 ◽  
pp. 02004
Author(s):  
Maxim Bashashin ◽  
Elena Zemlyanaya ◽  
Konstantin Lukyanov

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.


Author(s):  
Yoshiharu Hirabayashi ◽  
Shigeo Ohkubo

Abstract We show the existence of the α+α * cluster structure at the highly excited energy around Ex =20 MeV in 8Be for the first time in the coupled channels calculations. An extended double folding model derived using a realistic precise cluster wave function with a well-developed N+3N cluster structure for the first excited state of 4He was employed. The calculation reproduces the experimental phase shifts in α+α scattering up to Ec.m. =21 MeV well. The result shows that the well-developed core-excited α+α * structure appears as resonances for L=0 and 2 near the α+α * threshold which correspond to the experimental states at Ex =20.20MeV and Ex =22.24MeV in 8Be.


2016 ◽  
Vol 94 (3) ◽  
Author(s):  
Dao T. Khoa ◽  
Nguyen Hoang Phuc ◽  
Doan Thi Loan ◽  
Bui Minh Loc

2016 ◽  
Vol 94 (1) ◽  
pp. 102-111 ◽  
Author(s):  
M. Ismail ◽  
I.A.M. Abdul-Magead

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.


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