Description of the <sup>11</sup>B+<sup>209</sup>Bi elastic scattering: applying different nucleon-nucleon interactions

Abstract We analyzed the elastic scattering angular distributions of 11 B from 209 Bi over the energy range of 49.8–84.1 MeV using different potentials. We used the cluster folding (CF) method to calculate the real part of the nuclear optical potential (OP). The 7 Li+ α cluster structure of the tightly bound 11 B projectile is considered in this method. In addition, we employed the conventional double folding (DF) method using both energy-dependent (SPP2, S1Y, and R3Y) and energy-independent (BNP and KH) effective nucleon-nucleon (NN) interactions. We use either the Woods-Saxon (WS) form or an FM approach that matches the real potential for the imaginary part. For comparison, the phenomenological Woods-Saxon (WS) potential is used. We found that all the considered potentials accurately describe the differential cross sections. Furthermore, these potential parameters have similar energy behavior. These potentials are divided into two groups based on their energy dependence and their corresponding physical quantities.

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Publication Details

Journal
Physica Scripta
Published
2025-03-07
DOI
https://doi.org/10.1088/1402-4896/adbe12
Primary Topic
Superconducting Materials and Applications
Type
article
Field-Weighted Citation Impact
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article

Description of the 11B+209Bi elastic scattering: applying different nucleon-nucleon interactions

M. N. El-Hammamy, Ahmed Hammad Amer, Z. L. Mohamed
Physica Scripta
Superconducting Materials and Applications
article

Description of the 11B+209Bi elastic scattering: applying different nucleon-nucleon interactions

M. N. El-Hammamy, Ahmed Hammad Amer, Z. L. Mohamed
article en

Abstract

Abstract We analyzed the elastic scattering angular distributions of 11 B from 209 Bi over the energy range of 49.8–84.1 MeV using different potentials. We used the cluster folding (CF) method to calculate the real part of the nuclear optical potential (OP). The 7 Li+ α cluster structure of the tightly bound 11 B projectile is considered in this method. In addition, we employed the conventional double folding (DF) method using both energy-dependent (SPP2, S1Y, and R3Y) and energy-independent (BNP and KH) effective nucleon-nucleon (NN) interactions. We use either the Woods-Saxon (WS) form or an FM approach that matches the real potential for the imaginary part. For comparison, the phenomenological Woods-Saxon (WS) potential is used. We found that all the considered potentials accurately describe the differential cross sections. Furthermore, these potential parameters have similar energy behavior. These potentials are divided into two groups based on their energy dependence and their corresponding physical quantities.

Physica ScriptaVol. 100(4)
Damanhour University (EG), South Valley University (EG), Tanta University (EG), New Valley University
Openalex Percentile: Top 96%
Superconducting Materials and Applications
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