51. Elastic and inelastic electron-nucleus scattering form factors of some light nuclei:Na23,Mg25,Al27, andCa41
- Author
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Hasan Abu Kassim, Fadhil I. Sharrad, Anwer A. Al-Sammarrae, and Khalid S. Jassim
- Subjects
Physics ,Nuclear and High Energy Physics ,Light nucleus ,Particle physics ,Scattering ,Nuclear Theory ,Nuclear structure ,Electron ,Inelastic scattering ,Formalism (philosophy of mathematics) ,medicine.anatomical_structure ,medicine ,Atomic physics ,Electron scattering ,Nucleus - Abstract
Nuclear structure (energy levels, elastic and inelastic electron-nucleus scattering, and transition probability) of $^{23}\mathrm{Na}$, $^{25}\mathrm{Mg}$, $^{27}\mathrm{Al}$, and $^{41}\mathrm{Ca}$ nuclei have been studied using shell-model calculations. A set of two-body interactions are used in this paper. The universal $sd$ of the Wildenthal interaction in the proton-neutron formalism, universal $sd$-shell interaction A, universal $sd$-shell interaction B, and GXFP1 interaction for the $fp$ shell is used with the nucleon-nucleon realistic interaction Michigan three-range Yakawa as a two-body interaction for core-polarization calculations. Two shell-model codes, cpm3y and nushell for Windows, have been used to calculate the results. The wave functions of radial single-particle matrix elements have been calculated with harmonic-oscillator and Woods-Saxon potentials. The level schemes are compared with the experimental data up to 5.776, 5.251, and 4.51 MeV for $^{23}\mathrm{Na}$, $^{25}\mathrm{Mg}$, and $^{27}\mathrm{Mg}$, respectively. Very good agreements are obtained for all nuclei in this study. Results from electron scattering form-factor calculations have shown that the core-polarization effects are essential to obtain a reasonable description of the data with no adjustable parameters.
- Published
- 2014
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