Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors
In combination with the global set of two-body correlations (FC’s), comprising tensor correlations (TCs) as well as short-range correlations (SRCs), you get light nuclei 13C and 15N inelastic longitudinal C2 form factors and new efficient distance nucleonic system’s two-body density operator in this...
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EDP Sciences
2025-01-01
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| Series: | E3S Web of Conferences |
| Online Access: | https://www.e3s-conferences.org/articles/e3sconf/pdf/2025/27/e3sconf_geotech2025_05013.pdf |
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| author | Rashed Eman Mosa |
| author_facet | Rashed Eman Mosa |
| author_sort | Rashed Eman Mosa |
| collection | DOAJ |
| description | In combination with the global set of two-body correlations (FC’s), comprising tensor correlations (TCs) as well as short-range correlations (SRCs), you get light nuclei 13C and 15N inelastic longitudinal C2 form factors and new efficient distance nucleonic system’s two-body density operator in this research. Nucleon-nucleon interactions are described with reference to these correlations incorporating intense short- range repulsion with robust tensor force. Adjusting for core polarization effects. Using these operators, we can observe the shape of transition model with calculating of two-body charge densities (2BCDD’s) at ground states, as subsequent experiment distributions; This transition 13C from ground state(Jiπ, T): (−1/2 , 1/2) to the state (Jfπ, T): (−3/2 , 1/2) with an excitation energy (Ex) = 3.68 Mev and from ground state (Jiπ, T): (−3/2 , 1/2) to the state (Jfπ, T): (−5/2 , 1/2) with an excitation energy (Ex) = 7.55 Mev and 15N nucleus from ground state (Jiπ, T): (−1/2 , 1/2) to the state (Jfπ, T): (−3/2 , 1/2) having an excitation energy (Ex) = 6.32 Mev to calculating the inelastic longitudinally form factors C2 pertaining to the charge density, specifically focusing on the excitation of the mentioned levels. |
| format | Article |
| id | doaj-art-8be52b6b86844e8fb59e7f00d266068c |
| institution | Kabale University |
| issn | 2267-1242 |
| language | English |
| publishDate | 2025-01-01 |
| publisher | EDP Sciences |
| record_format | Article |
| series | E3S Web of Conferences |
| spelling | doaj-art-8be52b6b86844e8fb59e7f00d266068c2025-08-20T03:53:51ZengEDP SciencesE3S Web of Conferences2267-12422025-01-016270501310.1051/e3sconf/202562705013e3sconf_geotech2025_05013Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factorsRashed Eman Mosa0College of Engineering, University of SulaimaniIn combination with the global set of two-body correlations (FC’s), comprising tensor correlations (TCs) as well as short-range correlations (SRCs), you get light nuclei 13C and 15N inelastic longitudinal C2 form factors and new efficient distance nucleonic system’s two-body density operator in this research. Nucleon-nucleon interactions are described with reference to these correlations incorporating intense short- range repulsion with robust tensor force. Adjusting for core polarization effects. Using these operators, we can observe the shape of transition model with calculating of two-body charge densities (2BCDD’s) at ground states, as subsequent experiment distributions; This transition 13C from ground state(Jiπ, T): (−1/2 , 1/2) to the state (Jfπ, T): (−3/2 , 1/2) with an excitation energy (Ex) = 3.68 Mev and from ground state (Jiπ, T): (−3/2 , 1/2) to the state (Jfπ, T): (−5/2 , 1/2) with an excitation energy (Ex) = 7.55 Mev and 15N nucleus from ground state (Jiπ, T): (−1/2 , 1/2) to the state (Jfπ, T): (−3/2 , 1/2) having an excitation energy (Ex) = 6.32 Mev to calculating the inelastic longitudinally form factors C2 pertaining to the charge density, specifically focusing on the excitation of the mentioned levels.https://www.e3s-conferences.org/articles/e3sconf/pdf/2025/27/e3sconf_geotech2025_05013.pdf |
| spellingShingle | Rashed Eman Mosa Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors E3S Web of Conferences |
| title | Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors |
| title_full | Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors |
| title_fullStr | Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors |
| title_full_unstemmed | Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors |
| title_short | Core polarization effects for 13C and 15N nuclei and inelastic longitudinal form factors |
| title_sort | core polarization effects for 13c and 15n nuclei and inelastic longitudinal form factors |
| url | https://www.e3s-conferences.org/articles/e3sconf/pdf/2025/27/e3sconf_geotech2025_05013.pdf |
| work_keys_str_mv | AT rashedemanmosa corepolarizationeffectsfor13cand15nnucleiandinelasticlongitudinalformfactors |