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NSR database version of April 24, 2024.

Search: Author = H.Abu Kassim

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2020AB09      Chin.Phys.C 44, 114107 (2020)

M.K.M.Abu El Sheikh, A.A.Okhunov, H.Abu Kassim, M.U.Khandaker

Prediction of moment of inertia of rotating nuclei

NUCLEAR STRUCTURE ¹¹⁰Ru, ¹⁵⁰Nd, ¹⁵⁶Gd, ^166,168Er, ¹⁷²Yb, ^182,184W, ^186,188,190Os; calculated moment of inertia using the mathematical expression formulated by Bohr for the moment of inertia of even-even nuclei based on the hydrodynamical model. Comparison with available data.

doi: 10.1088/1674-1137/abb0dd
Citations: PlumX Metrics

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
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2017AL16      Int.J.Mod.Phys. E26, 1750032 (2017)

A.A.Al-Sammarraie, M.L.Inche Ibrahim, M.A.Saeed, F.I.Sharrad, H.Abu Kassim

Inelastic electric and magnetic electron scattering form factors of ²⁴Mg nucleus: Role of g factors

NUCLEAR REACTIONS ²⁴Mg(E, E), E not given; calculated the longitudinal and the transverse electron scattering form factors. The universal sd-shell model Hamiltonian (USDA).

doi: 10.1142/S021830131750032X
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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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2015SA07      Eur.Phys.J. A 51, 13 (2015)

S.M.Saleh Ahmed, R.Yahaya, S.Radiman, M.Samudi Yasir, H.Abu Kassim, M.Uddin Khandaker

Analytic view at alpha clustering in even-even heavy nuclei near magic numbers 82 and 126

NUCLEAR STRUCTURE ^172,174Pt, ^174,176,178Hg, ^{178,180,182,184}Pb, ^{188,190,192,194,196,198,208,210,212,214,216,218}Po, ^{196,198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{210,212,214,216,218,220,222,224,226,228,230}Th; calculated α-decay T_1/2, Q, α preformation factor using CFM (cluster formation model). Preformation factors compared with other calculations.

doi: 10.1140/epja/i2015-15013-4
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2015UD05      Nucl.Instrum.Methods Phys.Res. B362, 151 (2015)

M.U.Khandaker, H.Haba, M.Murakami, N.Otuka, H.Abu Kassim

Excitation functions of deuteron-induced nuclear reactions on natural platinum up to 24 MeV

NUCLEAR REACTIONS Pt(d, x)¹⁹²Au/¹⁹³Au/¹⁹⁴Au/¹⁹⁵Au/¹⁹⁶Au/¹⁹⁸Au/¹⁹⁹Au/¹⁹⁵Pt/¹⁹⁷Pt/¹⁹⁰Ir/¹⁹²Ir/¹⁹⁴Ir, E<24 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TENDL-2013 library, experimental data.

doi: 10.1016/j.nimb.2015.09.045
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2485.

2014JA01      Phys.Rev. C 89, 014304 (2014)

K.S.Jassim, A.A.Al-Sammarrae, F.I.Sharrad, H.Abu Kassim

Elastic and inelastic electron-nucleus scattering form factors of some light nuclei: ²³Na, ²⁵Mg, ²⁷Al, and ⁴¹Ca

NUCLEAR STRUCTURE ²³Na, ²⁵Mg, ²⁷Al, ⁴¹Ca; calculated levels, J, π, B(E2) by shell-model using USD, USDA, and USDB effective interactions; comparison with experimental data.

NUCLEAR REACTIONS ²³Na, ²⁵Mg, ²⁷Al, ⁴¹Ca(e, e), (e, e'), at momentum transfer of 0.1-3.5 fm^-1; calculated longitudinal and transverse form factors using shell model with USD, USDA, and USDB effective interactions, and core-polarization effects. Form factors for M1, M3, M5, and M7 transitions in ⁴¹Ca. Comparisons with experimental data.

doi: 10.1103/PhysRevC.89.014304
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2014OK02      J.Phys.(London) G41, 075102 (2014)

A.A.Okhunov, Ph.N.Usmanov, H.Abu Kassim

Influence of 1⁺ states on the g_R-factors of ground band in isotopes of ¹⁶⁰Dy and ^{170, 174}Yb

NUCLEAR STRUCTURE ¹⁶⁰Dy, ^170,174Yb; calculated wave functions, B(M1), B(E2), g-factors. Comparison with experimental data.

doi: 10.1088/0954-3899/41/7/075102
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2013IN01      Phys.Rev. C 87, 024611 (2013)

M.L.Inche Ibrahim, Z.Muhammad, H.Abu Kassim

Analysis of the nuclear potential for heavy-ion systems through large-angle quasi-elastic scattering

NUCLEAR REACTIONS ²⁰⁸Pb(⁷⁰Zn, ⁷⁰Zn), (⁷⁰Zn, X), E=235-246 MeV; ²⁰⁸Pb(⁶⁴Ni, ⁶⁴Ni), (⁶⁴Ni, X), E=219-234 MeV; ²⁰⁸Pb(⁵⁶Fe, ⁵⁶Fe), (⁵⁶Fe, X), E=209-215 MeV; ²⁰⁸Pb(⁵⁴Cr, ⁵⁴Cr), (⁵⁴Cr, X), E=186-197 MeV; ²⁰⁸Pb(⁴⁸Ti, ⁴⁸Ti), (⁴⁸Ti, X), E=173-188 MeV; analyzed quasi-elastic to Rutherford scattering cross section ratios, diffuseness parameter of nuclear potential, large-angle quasi-elastic scattering. Single and coupled channel calculations using CQEL computer code. ²⁰⁸Pb(⁵⁶Fe, ⁵⁶Fe), (⁵⁶Fe, X), E=209-215 MeV; analyzed quasi-elastic to Rutherford scattering cross section ratio using Woods Saxon and Sao Paulo potentials.

doi: 10.1103/PhysRevC.87.024611
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2013JA09      Rom.J.Phys. 58, 319 (2013)

K.S.Jassim, H.Abu Kassim

Core Polarization Effects of Some Odd sd-Shell Nuclei Using M3Y Effective Nucleon-Nucleon Interaction

NUCLEAR REACTIONS ¹⁷O, ²⁷Al, ³⁹K(E, E'), E not given; calculated form factors. The two-body Michigan three Yukawas (M3Y) interactions.

2013SH13      Chin.Phys.C 37, 034101 (2013)

F.I.Sharrad, H.Y.Abdullah, N.Al-Dahan, N.M.Umran, A.A.Okhunov, H.Abu Kassim

Low-lying states of ¹⁸⁴W and ¹⁸⁴Os nuclei

NUCLEAR STRUCTURE ¹⁸⁴W, ¹⁸⁴Os; calculated energy levels, J, π, B(E2), intrinsic quadrupole moments, potential energy surface. IBM-1 model, comparison with available data.

doi: 10.1088/1674-1137/37/3/034101
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2013SH14      Rom.J.Phys. 58, 99 (2013)

F.I.Sharrad, a.A.Okhunov, H.Y.Abdullah, H.Abu Kassim

Low-Lying States of Odd Nuclei in the South-West ²⁰⁸Pb Region

NUCLEAR STRUCTURE ^203,205Au, ^203,205Hg, ^203,205,207Tl, ^203,205,207Pb; calculated energy levels, J, π, B(E2). Shell code OXBASH, comparison with experimental data.

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.

2012SH35      Rom.J.Phys. 57, 1346 (2012)

F.I.Sharrad, H.Y.Abdullah, N.Al-Dahan, A.A.Mohammed-Ali, A.A.Okunov, H.Abu Kassim

SHAPE Transition and Collective Excitations in Neutron-Rich ^170-178Yb Nuclei

NUCLEAR STRUCTURE ^{170,172,174,176,178}Yb; calculated energy levels, B(E2), potential energy surfaces. IBM-1 calculations, comparison with available data.