Alpha elastically scattered by light nuclei using semi-microscopic and full microscopic methods

The present work aims to use semi-microscopic and full microscopic methods to analyze experimental data for alpha elastically scattered by 6,7Li, 9Be, and 11B in the energy range from 26 to 166 MeV. In the semi-microscopic method, the double folding São Paulo Potential (SPP) was used as a real part of the optical potential, while the Woods-Saxon form was used as an imaginary part. In the present calculations, the real part of the optical potential is derived by folding the nucleon-nucleon (NN) interaction into the nuclear matter density distribution of the projectile and target nuclei using the computer code SPOMC3. The optical model parameters and the normalization factors have an influence on the fitting of the experimental data. The volume integral of the imaginary part of the optical potential and the cross-section were found to be energy-dependent. In the full-microscopic method, the SPP was used as both a real and an imaginary part.

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Publication Details

Journal
Delta Journal of Science
Published
2024-09-01
DOI
https://doi.org/10.21608/djs.2024.306136.1175
Primary Topic
Nuclear physics research studies
Type
article
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article

Alpha elastically scattered by light nuclei using semi-microscopic and full microscopic methods

Rowan Farag Madyan, Ahmed Amar, Salwa Saad
Delta Journal of Science
Nuclear physics research studies
article

Alpha elastically scattered by light nuclei using semi-microscopic and full microscopic methods

Rowan Farag Madyan, Ahmed Amar, Salwa Saad
article en

Abstract

The present work aims to use semi-microscopic and full microscopic methods to analyze experimental data for alpha elastically scattered by 6,7Li, 9Be, and 11B in the energy range from 26 to 166 MeV. In the semi-microscopic method, the double folding São Paulo Potential (SPP) was used as a real part of the optical potential, while the Woods-Saxon form was used as an imaginary part. In the present calculations, the real part of the optical potential is derived by folding the nucleon-nucleon (NN) interaction into the nuclear matter density distribution of the projectile and target nuclei using the computer code SPOMC3. The optical model parameters and the normalization factors have an influence on the fitting of the experimental data. The volume integral of the imaginary part of the optical potential and the cross-section were found to be energy-dependent. In the full-microscopic method, the SPP was used as both a real and an imaginary part.

Delta Journal of ScienceVol. 49(1)
Tanta University (EG)
Openalex Percentile: Top 96%
Nuclear physics research studies
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