Abstract
Using the double folding model (DF), the real part of the central potential for {sup 12} C + {sup 12} C system is derived. This potential as well as the single folding cluster model potential (SFC) were used to calculate the total and differential cross sections for {sup 12} C elastically scattered on {sup 12} C at three laboratory energies; E{sub 1ab}. = 300, 344.5 and 360 MeV. The calculations were carried out using five sets of nucleon nucleon (NN) interaction of the integrable Gaussian form and two sets of parameters for the nuclear matter density of the harmonic oscillator form. The transparency of the target nucleus was found to increase as the projectile energy increases. Good fits between the present calculations and the experimental data as well as the previously published calculations were obtained. The present simple methods used to calculate the real part of the optical potential stand on equal footing with the density dependent (DDM 3 Y) procedure and it reduces the potential computing time enormously. The suitable choice of NN interaction as well as nuclear matter densities is important. 24 figs., 3 tabs.
Khallaf, S A.E.;
[1]
Abdel-Rahman, M A;
Abdel-Raheem, S K;
Mahmoud, S W.Z.
[2]
- Department of Physics, Faculty of Science, Assiut University, Assiut, (Egypt)
- Department of Physics, Faculty of Science, El-Minia University, El-Minia, (Egypt)
Citation Formats
Khallaf, S A.E., Abdel-Rahman, M A, Abdel-Raheem, S K, and Mahmoud, S W.Z.
Elastic scattering of {sup 12} C by {sup 12} C at intermediate energies.
Egypt: N. p.,
1996.
Web.
Khallaf, S A.E., Abdel-Rahman, M A, Abdel-Raheem, S K, & Mahmoud, S W.Z.
Elastic scattering of {sup 12} C by {sup 12} C at intermediate energies.
Egypt.
Khallaf, S A.E., Abdel-Rahman, M A, Abdel-Raheem, S K, and Mahmoud, S W.Z.
1996.
"Elastic scattering of {sup 12} C by {sup 12} C at intermediate energies."
Egypt.
@misc{etde_521462,
title = {Elastic scattering of {sup 12} C by {sup 12} C at intermediate energies}
author = {Khallaf, S A.E., Abdel-Rahman, M A, Abdel-Raheem, S K, and Mahmoud, S W.Z.}
abstractNote = {Using the double folding model (DF), the real part of the central potential for {sup 12} C + {sup 12} C system is derived. This potential as well as the single folding cluster model potential (SFC) were used to calculate the total and differential cross sections for {sup 12} C elastically scattered on {sup 12} C at three laboratory energies; E{sub 1ab}. = 300, 344.5 and 360 MeV. The calculations were carried out using five sets of nucleon nucleon (NN) interaction of the integrable Gaussian form and two sets of parameters for the nuclear matter density of the harmonic oscillator form. The transparency of the target nucleus was found to increase as the projectile energy increases. Good fits between the present calculations and the experimental data as well as the previously published calculations were obtained. The present simple methods used to calculate the real part of the optical potential stand on equal footing with the density dependent (DDM 3 Y) procedure and it reduces the potential computing time enormously. The suitable choice of NN interaction as well as nuclear matter densities is important. 24 figs., 3 tabs.}
place = {Egypt}
year = {1996}
month = {Dec}
}
title = {Elastic scattering of {sup 12} C by {sup 12} C at intermediate energies}
author = {Khallaf, S A.E., Abdel-Rahman, M A, Abdel-Raheem, S K, and Mahmoud, S W.Z.}
abstractNote = {Using the double folding model (DF), the real part of the central potential for {sup 12} C + {sup 12} C system is derived. This potential as well as the single folding cluster model potential (SFC) were used to calculate the total and differential cross sections for {sup 12} C elastically scattered on {sup 12} C at three laboratory energies; E{sub 1ab}. = 300, 344.5 and 360 MeV. The calculations were carried out using five sets of nucleon nucleon (NN) interaction of the integrable Gaussian form and two sets of parameters for the nuclear matter density of the harmonic oscillator form. The transparency of the target nucleus was found to increase as the projectile energy increases. Good fits between the present calculations and the experimental data as well as the previously published calculations were obtained. The present simple methods used to calculate the real part of the optical potential stand on equal footing with the density dependent (DDM 3 Y) procedure and it reduces the potential computing time enormously. The suitable choice of NN interaction as well as nuclear matter densities is important. 24 figs., 3 tabs.}
place = {Egypt}
year = {1996}
month = {Dec}
}