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NSR database version of May 10, 2024.

Search: Author = A.A.Alzubadi

Found 18 matches.

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2023AL10      East.Eur.J.Phys 2003, 138 (2023)

O.A.Alswaidawi, A.A.Alzubadi

Electroexcitation Form Factors and Deformation of 20, 22Ne Isotopes Based on the Shell Model and Hartree-Fock plus BCS Calculations

NUCLEAR STRUCTURE 20,22Ne; calculated energy levels, J, π, B(Eλ) using the shell model with Skyrme-Hartree-Fock. Comparison with available data.

doi: 10.26565/2312-4334-2023-2-13
Citations: PlumX Metrics


2023AL14      Int.J.Mod.Phys. E32, 2350020 (2023)

O.A.Alswaidawi, A.A.Alzubadi

Hamiltonian sensitivity in calculating the electromagnetic moments and electroexcitation form factor for the sd nuclei using shell model with Skyrme-Hartree-Fock

NUCLEAR MOMENTS 17,18,19,20O, 17,18,19,20,21,22F, 19,20,21,22,23,24,25Ne, 20,21,22,23,24,25,26,27,28,29,30,31Na, 21,22,23,24,25,26,27,28,29,30,31Mg, 23Al, 26,27,28,29,30,31,32,33Al, 27,28,29,30,31,32,33Si, 28,29,30,31,32P, 31,32,33S; calculated magnetic dipole and electric quadrupole moments. Comparison with available data.

doi: 10.1142/S0218301323500209
Citations: PlumX Metrics


2023AL21      Phys.Atomic Nuclei 86, 370 (2023)

A.A.Alzubadi, L.J.Abbas

Electroexcitation Form Factors for Positive- and Negative-Parity States in Some Si Isotopes Using Truncated Large-Scale Shell Model With Skyrme-Hartree-Fock Method

NUCLEAR STRUCTURE 28,29,30Si; calculated the elastic and inelastic electron scattering form factors, energy levels and B(E2) using a truncated large-scale shell model (LSSM) with the Hartree-Fock method.

doi: 10.1134/S1063778823040026
Citations: PlumX Metrics


2023OB01      East.Eur.J.Phys 2003, 76 (2023)

R.S.Obaid, A.A.Alzubadi

A Study of the Weakly Bound Structure of Nuclei Around the Magic Number N=50

NUCLEAR STRUCTURE 88,90,92,94Kr, 90,92,94,96Sr, 92,94,96,98Zr, 94,96,98,100Mo, 100Sn; calculated quadrupole deformation parameters, neutron-, proton-particle states and energies, potential energy curves using the Skyrme-Hartree-Fock (SHF) theory and Hartree-Fock-Bogoliubov (HFB) method.

doi: 10.26565/2312-4334-2023-2-05
Citations: PlumX Metrics


2022BA18      Int.J.Mod.Phys. E31, 2250029 (2022)

H.A.Bahr, A.A.Alzubadi

Relativistic and nonrelativistic mean field analysis of the shell evolution in 44-52Ar isotopes

NUCLEAR STRUCTURE 42,44,46,48,50,52Ar; calculated the ground state properties employing two methods: the nonrelativistic HF+BCS approach with SV-minSkyrme functional using SkyAx code64and the relativistic RHB approach based onDD-PCX parametrization using the DIRHBZ code.

doi: 10.1142/S021830132250029X
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2022KA51      East.Eur.J.Phys 2022, 57 (2022)

N.M.Kareem, A.A.Alzubadi

Study of the Nuclear Structure for Some Nuclei Using Self-Consistent RPA Calculations with Skyrme-Type Interaction

NUCLEAR STRUCTURE 58Ni, 90Zr, 116Sn, 144Sm; calculated static and dynamic nuclear properties, J, π, energy levels of the closed-shell nuclei using the Random Phase Approximation (RPA) method framework and different Skyrme parameterizations, particularly SyO-, Sk255, SyO+, SLy4, BSk17, and SLy5.

doi: 10.26565/2312-4334-2022-4-04
Citations: PlumX Metrics


2022KA57      Phys.Atomic Nuclei 85, 625 (2022)

N.M.Kareem, A.A.Alzubadi

Self-Consistent RPA Calculations for the Excitation to the Negative Parity States in Closed-Shell Nuclei

NUCLEAR STRUCTURE 16O, 34Si, 40,48Ca; calculated nuclear densities with associated root-mean-square radii, neutron skin thicknesses, the binding energy per nucleon, and the single-particle radial nuclear density distributions using the self-consistent random phase approximation and applied with different Skyrme parameterizations; SyO-, SyO+, BSk17, Sk255, SLy4 and SLy5.

doi: 10.1134/S1063778823010234
Citations: PlumX Metrics


2022RA30      Int.J.Mod.Phys. E31, 2250086 (2022)

R.A.Radhi, A.A.Alzubadi

Electromagnetic moments and magnetic form factors of the ground states of odd-A nuclei in the vicinity of Z = 20 closure

NUCLEAR STRUCTURE 35,37,39K, 39,41,43,45,47,49,51Ca, 41,43,45,47,49Sc, 43,45,47,49Ti, 49,51V; calculated nuclear dipole and quadrupole moments using Skyrme-Hartree-Fock (SHF) method. Comparison with available data.

doi: 10.1142/S0218301322500860
Citations: PlumX Metrics


2021AL34      Phys.Scr. 96, 055304 (2021)

A.A.Alzubadi, A.J.Alhaideri, N.F.Lattoofi

Study of static and dynamic properties of even-even 14-24O and 38-54Ca in the frame of Random Phase Approximation (RPA) method with different Skyrme parameterizations

NUCLEAR STRUCTURE 14,16,18,20,22,24,26O, 38,40,42,44,46,48,50,52,54Ca; calculated nuclear charge radii, the binding energy per nucleon using the framework of the random phase approximation method with different Skyrme parameterizations. Comparison with available data.

doi: 10.1088/1402-4896/abe9f0
Citations: PlumX Metrics


2021RA21      Nucl.Phys. A1015, 122302 (2021)

R.A.Radhi, A.A.Alzubadi, N.S.Manie

Electromagnetic multipoles of positive parity states in 27Al by elastic and inelastic electron scattering

NUCLEAR REACTIONS 27Al(e-, e-), (e-, e-'), E not given; analyzed available data; calculated energy levels, J, π using shell model with self-consistent Hartree-Fock calculations.

doi: 10.1016/j.nuclphysa.2021.122302
Citations: PlumX Metrics


2020AL27      Int.J.Mod.Phys. E29, 2050090 (2020)

A.A.Allami, A.A.Alzubadi

Study of the nuclear structure of some exotic nuclei using nonrelativistic and relativistic mean-field methods

NUCLEAR STRUCTURE 6,7,8,9,10,11Li, 7,8,9,10,11,12,13,14Be, 17Ne, 23Al, 27P; analyzed available data; calculated rms mass radii, reaction σ, mass density using nuclear shell model with the Skyrme-Hartree-Fock (SHF), as a nonrelativistic approach, and the relativistic Hartree-Fock-Bogoliubov (RHFB) methods.

doi: 10.1142/S0218301320500901
Citations: PlumX Metrics


2020AL28      Phys.Scr. 95, 105306 (2020)

A.H.Ali, A.A.Alzubadi

Calculation magnetic dipole moments, electric quadrupole moments and form factors for some Ti isotopes

NUCLEAR STRUCTURE 43,44,45,46,47,48,49,50,52Ti; calculated magnetic dipole, electric quadrupole moments, form factors using the shell model space. Comparison with available data.

doi: 10.1088/1402-4896/abbaf4
Citations: PlumX Metrics


2020LA15      Int.J.Mod.Phys. E29, 2050084 (2020)

N.F.Lattoofi, A.A.Alzubadi

Study of giant dipole resonances for neodymium isotopes with an exciton model

NUCLEAR REACTIONS 142,143,144,145,148,150Nd(γ, n), (γ, np), (γ, 2n), E=6-26 MeV; calculated σ using EMPIRE 3.2.2 code. Comparison with available data.

doi: 10.1142/S0218301320500846
Citations: PlumX Metrics


2019RA25      Few-Body Systems 60, 57 (2019)

R.A.Radhi, A.A.Alzubadi

Study the Nuclear Form Factors of Low-Lying Excited States in 7Li Nucleus Using the Shell Model with Skyrme Effective Interaction

NUCLEAR STRUCTURE 7Li; calculated energy levels, J, π, nuclear magnetic and quadrupole moments using NuShellX@MSU.

doi: 10.1007/s00601-019-1524-x
Citations: PlumX Metrics


2018AL08      Phys.Rev. C 97, 024316 (2018)

A.A.Alzubadi, R.A.Radhi, N.S.Manie

Shell model and Hartree-Fock calculations of longitudinal and transverse electroexcitation of positive and negative parity states in 17O

NUCLEAR STRUCTURE 17O; calculated levels, J, π, rms radii using different single particle potentials, B(E2), B(E3) in the psdpn and zbme shell-model spaces. Shell-model calculations with SLy4 and SkXcsb Skyrme, HO, and WS single-particle potentials and using NUSHELLX code. Comparison with experimental data.

NUCLEAR REACTIONS 17O(e, e), (e, e'), momentum transfer=0.0-3.0 fm-1; calculated longitudinal and transverse form factors for several levels in 17O. Shell model and Hartree-Fock mean field calculations with SLy4 and SkXcsb Skyrme interaction, HO, and WS potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.024316
Citations: PlumX Metrics


2018RA13      Phys.Rev. C 97, 064312 (2018)

R.A.Radhi, A.A.Alzubadi, A.H.Ali

Magnetic dipole moments, electric quadrupole moments, and electron scattering form factors of neutron-rich sd-pf cross-shell nuclei

NUCLEAR MOMENTS 34Al, 35Si, 38,40,43S, 38,44Cl, 39,40,41,43Ar, 40,41,42,43,44,45,46,47,49,51K; calculated g factors, magnetic dipole moments with free g factor or effective g factor, electric quadrupole moments with core polarization (CP) or Bohr-Mottelson (BM) effective charges. 42Si, 44S, 46Ar, 48Ca; calculated electric quadrupole moments. 27,34Al, 35Si, 43S, 38Cl, 39Ar, 40K; calculated elastic magnetic form factors with contributions from multipoles, longitudinal C2 form factors with contributions form CP and model space (MS) effects. Shell model calculations for sd-pf cross-shell nuclei. Comparison with available experimental values.

doi: 10.1103/PhysRevC.97.064312
Citations: PlumX Metrics


2016RA02      Nucl.Phys. A947, 12 (2016)

R.A.Radhi, A.A.Alzubadi, E.M.Rashed

Shell model calculations of inelastic electron scattering for positive and negative parity states in 19F

NUCLEAR REACTIONS 19F(e, e'), E not given; calculated longitudinal and transverse form-factor for positive and for negative parity states, charge radius, nuclear magnetic dipole moment using NuShellX@MSU shell model and Hartree-Fock, one-body density matrix and single-particle matrix elements and also harmonic oscillator for comparison. Results compared to data.

doi: 10.1016/j.nuclphysa.2015.12.002
Citations: PlumX Metrics


2015AL31      Int.J.Mod.Phys. E24, 1550099 (2015)

A.A.Alzubadi, Nabeel F.Latooffi, R.A.Radhi

Shell model and Hartree-Fock calculations for some exotic nuclei

NUCLEAR STRUCTURE 11Li, 11,14Be, 8B; calculated mass density distributions, the associated nuclear radii and elastic electron scattering form factors. Shell model (SM) and Hartree-Fock (HF) methods.

doi: 10.1142/S0218301315500998
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