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NSR database version of April 27, 2024.

Search: Author = R.A.Radhi

Found 23 matches.

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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


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


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
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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
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2016JA01      Pramana 86, 87 (2016)

K.S.Jassim, R.A.Radhi, N.M.Hussain

Inelastic magnetic electron scattering form factors of the 26Mg nucleus

NUCLEAR STRUCTURE 26Mg; calculated energy levels, J, π, transverse M3 form factors, B(M3). Nuclear shell model, comparison with available data.

doi: 10.1007/s12043-015-1012-x
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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
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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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2014RA17      Eur.Phys.J. A 50, 115 (2014)

R.A.Radhi, Z.A.Dakhil, N.S.Manie

Microscopic calculations of quadrupole moments in Li and B isotopes

NUCLEAR STRUCTURE 7,8,9,11Li, 8,10,11,12,13,14,15B; calculated quadrupole moment, effective charge, matter radii. 10,14B; calculated low-lying levels, J, π. Results compared with available data. Shell model with p and large spsdpf shell model spaces.

doi: 10.1140/epja/i2014-14115-9
Citations: PlumX Metrics


2014TA20      Int.J.Mod.Phys. E23, 1450038 (2014)

A.H.Taqi, R.A.Radhi, A.M.Hussein

Low excitations of 16O using generalized density matrix random phase approximation GDRPA

NUCLEAR STRUCTURE 16O; calculated energy levels, J, π, form factors. Random Phase Approximation (RPA) formalism.

doi: 10.1142/S0218301314500384
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2013SH38      Chin.J.Phys.(Taiwan) 51, 452 (2013)

F.I.Sharrad, A.K.Hamoudi, R.A.Radhi, H.Y.Abdullah, A.A.Okhunov, H.Abu Kassim

Elastic Electron Scattering from Some Light Nuclei

NUCLEAR REACTIONS 4He, 12C, 16O, 28Si, 32S, 40Ca(E, E), E not given; calculated form factors; deduced two-body short range correlation, occupation probability of higher states. Comparison with experimental data.


2009RA21      J.Phys.(London) G36, 105102 (2009)

R.A.Radhi, N.M.Adeeb, A.K.Hashim

Electro excitations of 9Be using large-basis shell model wavefunctions with higher energy configurations

NUCLEAR REACTIONS 9Be(e, e), (e, e'), E not given; calculated Coulomb form factors, excitation energies and transition probabilities. USDB, OXBASH shell model, comparison with experiment.

doi: 10.1088/0954-3899/36/10/105102
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2008RA01      Nucl.Phys. A798, 16 (2008)

R.A.Radhi, A.A.Abdullah, A.H.Raheem

Calculations of elastic and inelastic electron scattering on 19F using large-basis no core-shell model wave functions

NUCLEAR REACTIONS 19F(e, e), (e, e'), E not given; calculated form factors using a large basis no core shell model including higher energy configurations.

doi: 10.1016/j.nuclphysa.2007.10.010
Citations: PlumX Metrics


2008RA15      Nucl.Phys. A806, 179 (2008)

R.A.Radhi, E.A.Salman

Collective E2 transitions in 18O

NUCLEAR STRUCTURE 18O; calculated excited state level energies, B(E2) and form factors including core-polarization effects.

doi: 10.1016/j.nuclphysa.2008.03.008
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2007RA28      Eur.Phys.J. A 34, 107 (2007)

R.A.Radhi

Perturbative role in the inelastic electron scattering from 29Si

NUCLEAR REACTIONS 29Si(e, e'), E not given; calculated form factors, including core polarization effects, with a refined shell model.

doi: 10.1140/epja/i2007-10488-0
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2006MA63      Chin.Phys.Lett. 23, 2699 (2006)

F.A.Majeed, R.A.Radhi

Dipole and Quadrupole Electroexcitations of the Isovector T = 1 Particle-Hole States in 12C

NUCLEAR STRUCTURE 12C; calculated particle-hole states energies, J, π, dipole and quadrupole transition form factors. Harmonic oscillator shell model.

doi: 10.1088/0256-307X/23/10/021
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2003RA04      Nucl.Phys. A716, 87 (2003)

R.A.Radhi, A.Bouchebak

Microscopic calculations of C2 and C4 form factors in sd-shell nuclei

NUCLEAR REACTIONS 20Ne, 24Mg, 28Si, 32S(e, e'), E not given; calculated longitudinal Coulomb form factors, core-polarization effects. Comparisons with data.

NUCLEAR STRUCTURE 17O, 21Ne, 23Na, 25Mg, 27Al, 33S, 35,37Cl, 39K; calculated quadrupole moments. Microscopic model, comparisons with data.

doi: 10.1016/S0375-9474(02)01335-0
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2003RA05      Nucl.Phys. A716, 100 (2003)

R.A.Radhi

Microscopic calculations of C2 form factors of 6Li

NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated longitudinal Coulomb form factors, core-polarization effects. Microscopic model, comparison with data.

doi: 10.1016/S0375-9474(02)01376-3
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2003RA08      Eur.Phys.J. A 16, 381 (2003)

R.A.Radhi

Core polarization effects on C4 form factors of sd-shell nuclei

NUCLEAR REACTIONS 20Ne, 24Mg, 28Si, 32S(e, e'), E not given; calculated longitudinal Coulomb form factors, transition probabilities, core polarization effects. Modified surface delta interaction, comparison with data.

doi: 10.1140/epja/i2002-10065-1
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2003RA09      Eur.Phys.J. A 16, 387 (2003)

R.A.Radhi

Single-particle quadrupole electromagnetic transitions in p-shell and sd-shell nuclei

NUCLEAR REACTIONS 15N, 17O, 39K(e, e'), E not given; calculated longitudinal Coulomb form factors, transition probabilities, core polarization effects. Modified surface delta interaction, comparison with data.

NUCLEAR STRUCTURE 17O, 21Ne, 23Na, 25Mg, 27Al, 33S, 35,37Cl, 39K; calculated quadrupole moments.

doi: 10.1140/epja/i2002-10050-8
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2003RA30      Nucl.Phys. A724, 333 (2003)

R.A.Radhi, N.T.Khalaf, A.A.Najim

Elastic magnetic electron scattering from 17O, 25Mg, and 27Al

NUCLEAR REACTIONS 17O, 25Mg, 27Al(e, e), E not given; calculated electron scattering form factors, core polarization effects. Configuration mixing shell model.

doi: 10.1016/S0375-9474(03)01009-1
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2002RA38      Nucl.Phys. A707, 56 (2002)

R.A.Radhi

Nuclear Structure Study with Inelastic Electron Scattering from 27Al

NUCLEAR REACTIONS 27Al(e, e'), E not given; calculated form factors, core polarization effects. Mass-dependent Wildenthal interaction, comparison with data.

doi: 10.1016/S0375-9474(02)00794-7
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2001RA41      Nucl.Phys. A696, 442 (2001)

R.A.Radhi, A.A.Abdullah, Z.A.Dakhil, N.M.Adeeb

Core-Polarization Effects on C2 Form Factors of p-Shell Nuclei

NUCLEAR STRUCTURE 6,7Li, 10B, 12,13C; calculated transition probabilities, form factors; deduced core-polarization effects. Comparisons with data.

doi: 10.1016/S0375-9474(01)01218-0
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