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NSR database version of April 27, 2024.

Search: Author = A.H.Taqi

Found 8 matches.

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2023AK03      East.Eur.J.Phys 2003, 324 (2023)

M.A.Akbar, A.H.Taqi

Isoscalar Giant Octupole Resonance ISGOR of 116Cd using Self-Consistent Skyrme QRPA

NUCLEAR STRUCTURE 116Cd; calculated fraction energy-weighted sum rules (EWSR/MeV) for ISGOR ISGOR centroid energies, constrained energies, and scaling energies based on ten Skyrme-type interaction with the quasi-particle random phase approximation (QRPA), which considers the pairing effect, enhanced RPA model. Comparison with available data.

doi: 10.26565/2312-4334-2023-2-37
Citations: PlumX Metrics

2023HA37      Ukr.J.Phys. 68, 577 (2023)

M.A.Hasan, A.H.Taqi

Proton and Neutron Pairing Properties within a Mixed Volume-Surface Pairing Type Using the Hartree-Fock-Bogolyubov Theory

NUCLEAR STRUCTURE Z=2-110; analyzed available data; deduced a more accurate mass formula with the Skyrme (SKI3) force, the global descriptive power of the Skyrme–Hartree–Fock–Bogoliubov model for pairing properties.

doi: 10.15407/ujpe68.9.577
Citations: PlumX Metrics

2023SA21      East.Eur.J.Phys 2003, 329 (2023)

F.A.Saber, A.H.Taqi

Hole-Hole Collective Excitations in 106, 112, 130Sn Isotopes

NUCLEAR STRUCTURE 106,112,130Sn; calculated energy levels, J, π using using collective models, i.e., hole-hole Tamm-Dancoff Approximation (hh TDA) and hole-hole Random Phase Approximation (hh RPA). Comparison with available data.

doi: 10.26565/2312-4334-2023-2-38
Citations: PlumX Metrics

2021TA32      Ukr.J.Phys. 66, 928 (2021)

A.H.Taqi, M.A.Hasan

Skyrme-Hartree-Fock-Bogoliubov Calculations of Even and Odd Neutron-Rich Mg Isotopes

NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,52,54,56,58,60Mg; calculated binding energies, one- and two-neutron separation energies, quadrupole deformation parameters, neutron and proton radii. Hartree-Fock-Bogoliubov calculations based on the D1S Gogny force, and predictions of some nuclear models such as the Finite Range Droplet Model (FRDM) and Relativistic Mean-Field (RMF)model.

doi: 10.15407/ujpe66.11.928
Citations: PlumX Metrics

2019TA06      Nucl.Phys. A983, 103 (2019)

A.H.Taqi, G.L.Alawi

Isoscalar giant resonance in 100, 116, 132Sn isotopes using Skyrme HF-RPA

NUCLEAR STRUCTURE 100,116,132Sn; calculated E0, E1, E2 and E3 strength distributions, centroid energy and transition strength distribution using Hartree-Fock (HF) based Random-Phase Approximation (RPA) and several Skyrme interactions; deduced nuclear matter parameters and properties at saturation density using the fit to the data.

doi: 10.1016/j.nuclphysa.2019.01.001
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2016TA16      Chin.J.Phys.(Taiwan) 54, 185 (2016)

A.H.Taqi, A.H.Ibrahim

Electron scattering of 14N based on two-hole excitations

NUCLEAR REACTIONS 14N(E, E'), E not given; calculated form factors. Comparison with available data.

doi: 10.1016/j.cjph.2016.04.003
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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
Citations: PlumX Metrics

2010TA07      Acta Phys.Pol. B41, 1327 (2010)

A.H.Taqi, A.A.Rasheed, S.H.Amin

Particle-Particle and Hole-Hole Random Phase Approximation Calculations for 42Ca and 38Ca Nuclei

NUCLEAR STRUCTURE 38,42Ca; calculated energy levels, J, π, form factors.

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