NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = N.Yusof Found 5 matches. 2021BH10 J.Phys.(London) G48, 075105 (2021) M.Bhuyan, B.Maheshwari, H.A.Kassim, N.Yusof, S.K.Patra, B.V.Carlson, P.D.Stevenson The kinks in charge radii across N = 82 and 126 revisited NUCLEAR STRUCTURE 126,128,130,132,134,136,138Sn, 202,204,206,208,210,212,214Pb; analyzed available data; deduced isotopic shift over the isotopic chains, energy levels, J, π, yrast states within the relativistic mean-field (RMF) and relativistic-Hartree-Bogoliubov (RHB) approach.
doi: 10.1088/1361-6471/abf7d7
2020BI13 Nucl.Phys. A1004, 122042 (2020) S.K.Biswal, M.K.Abu El Sheikh, N.Biswal, N.Yusof, H.A.Kassim, S.K.Patra, M.Bhuyan Nuclear matter properties of finite nuclei using relativistic mean field formalism NUCLEAR STRUCTURE N=20, 40, 82, 126; analyzed available data; calculated variation of the symmetry energy with density in the symmetric nuclear matter, symmetry energy for N = 20, 40, 82, 126, and 172 (predicted) isotonic chains as a function of neutron skin-thickness as calculated using the RMF model.
doi: 10.1016/j.nuclphysa.2020.122042
2019MA80 Nucl.Phys. A992, 121619 (2019) B.Maheshwari, H.Abu Kassim, N.Yusof, A.K.Jain Evolution of nuclear structure in and around Z = 50 closed shell: Generalized seniority in Cd, Sn and Te isotopes NUCLEAR STRUCTURE N=50-88; calculated first excited 2+ and 11/2-states, quadrupole moments, B(E2, 2+TO 0+), g-factor for the first 2+ excited states of Cd, Sn, Te; deduced linearly varying quadrupole moments are described using a consistent multi-j configuration within the Generalized Seniority Schmidt Model (GSSM) scheme; deduced asymmetric double-hump behavior of B(E2) values; compared calculated energies of the first 11/2- states and empirical g-factor trend with experimental data.
doi: 10.1016/j.nuclphysa.2019.121619
2015AB01 Phys.Rev. C 91, 015811 (2015) A.Abdul Aziz, N.Yusof, M.Zamrun Firihu, H.A.Kassim Reliability of the double-folding potential for fusion cross sections of light systems NUCLEAR REACTIONS 12C, 16O, 24Mg, 28Si(12C, X), 16O(16O, X), 24Mg, 28Si(24Mg, X), 28Si(28Si, X), E not given; calculated barrier height, position, and fusion barrier energies using Akyuz-Winther (A-W), M3Y double-folding (DFM), and α-α double-folding cluster (DFC) potentials. 12C(12C, X), E=2-8 MeV; 16O(16O, X), E=6-15 MeV; 12C(16O, X), E=3-13 MeV; calculated σ(E) and modified astrophysical S(E) factor using A-W, DFM and DFC potentials, thermonuclear reaction rates for T9=0.5-3.0. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.015811
2015AL21 Phys.Rev. C 92, 034327 (2015) A.A.Al-Sammarraie, F.I.Sharrad, N.Yusof, H.Abu Kassim Longitudinal and transverse electron-nucleus scattering form factors of 25Mg NUCLEAR STRUCTURE 25Mg; calculated one-body density-matrix (OBDM) elements, levels, J, π, proton and neutron-fractional occupancy using Michigan three-range Yukawa (CPM3Y) code with and without inclusion of the core-polarization, and USDA, USDB Hamiltonians. Comparison with experimental data. NUCLEAR REACTIONS 25Mg(e, e), (e, e') at q<3 fm-1; calculated longitudinal and C2 and C4 and total electron-scattering form factors using Sk42 potential and USDA Hamiltonian for several transitions in 25Mg, M1, M3 and M5 form factors. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.034327
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