NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.Abu-Ibrahim Found 27 matches. 2022AB02 Phys.Rev. C 105, 014626 (2022) I.A.M.Abdul-Magead, B.Abu-Ibrahim Neutron skin of neutron-rich nuclei NUCLEAR REACTIONS 12C(p, p), E=250, 300 MeV; analyzed and fitted σ(θ, E) experimental data. 12C(21F, X), (22F, X), (23F, X), (24F, X), (25F, X), (26F, X), (27F, X), (29F, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), (24Na, X), (25Na, X), (26Na, X), (27Na, X), (28Na, X), (29Na, X), (30Na, X), (31Na, X), (32Na, X), (33Na, X), (34Na, X), (35Na, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=250, 300 MeV/nucleon; calculated reaction cross sections σ(E); deduced root-mean-square neutron radii and neutron skins of these neutron-rich nuclei from experimental data and calculations; neutron skins exhibited a linear relationship with the isospin (N-Z)/A.
doi: 10.1103/PhysRevC.105.014626
2020AB03 Nucl.Phys. A1000, 121804 (2020) I.A.M.Abdul-Magead, B.Abu-Ibrahim Contribution of the projectile neutrons to the total charge-changing cross sections
doi: 10.1016/j.nuclphysa.2020.121804
2020AB15 J.Phys.(London) G47, 055103 (2020) I.A.M.Abdul-Magead, E.Hamza, B.Abu-Ibrahim Neutron radii and neutron skin of neutron-rich nuclei deduced from proton-nucleus total reaction cross sections NUCLEAR REACTIONS 1H(12C, X), (22C, X), (9Be, X), (14Be, X), E=40 MeV/nucleon; analyzed available data. 22C, 14Be; deduced neutron radii.
doi: 10.1088/1361-6471/ab752c
2014YO06 Phys.Rev. C 90, 024608 (2014) M.Saleh Yousef, M.Almarashi, B.Abu-Ibrahim Scaling laws for total reaction cross sections
doi: 10.1103/PhysRevC.90.024608
2011AB02 Phys.Rev. C 83, 044615 (2011) Nucleus-nucleus total reaction cross sections, and the nuclear interaction radius NUCLEAR REACTIONS 1H(p, x), (n, X), 12C(p, X), (12C, X), 9Be, 12C, 27Al(12C, X), 208Pb(12C, X), E=30-1000 MeV/nucleon; analyzed nucleus-nucleus total reaction σ as a function of projectile mass number (A=8-220) on targets of 12C, 16O, 20Ne, 40Ar and 56Fe. Parameter-free semi-empirical relation for total cross sections. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044615
2011II01 Prog.Theor.Phys.(Kyoto) 126, 1091 (2011) K.Iida, K.Oyamatsu, B.Abu-Ibrahim, A.Kohama Proton-Nucleus Total Reaction Cross Sections in the Optical Limit Glauber Theory -Subtle Dependence on the Equation of State of Nuclear Matter - NUCLEAR REACTIONS 112,124Sn, 80Ni(p, X), E=40, 300, 800 MeV; calculated total σ. Glauber theory.
doi: 10.1143/PTP.126.1091
2010AB13 Phys.Rev. C 81, 057601 (2010) Scaling properties of proton-nucleus total reaction cross sections
doi: 10.1103/PhysRevC.81.057601
2009AB07 J.Phys.Soc.Jpn. 78, 044201 (2009) B.Abu-Ibrahim, S.Iwasaki, W.Horiuchi, A.Kohama, Y.Suzuki Elastic and Total Reaction Cross Sections of Oxygen Isotopes in Glauber Theory NUCLEAR REACTIONS 16O(p, p), E=317, 1000 MeV; 20,21,23O(p, p), E=300 MeV; calculated σ(θ). 12C(15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E=1 GeV/nucleon; calculated total reaction cross sections.
doi: 10.1143/JPSJ.78.044201
2008AB07 Phys.Rev. C 77, 034607 (2008); Publshiers note Phys.Rev. C 81, 019901 (2010) B.Abu-Ibrahim, W.Horiuchi, A.Kohama, Y.Suzuki Reaction cross sections of carbon isotopes incident on a proton NUCLEAR REACTIONS 1H(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (22C, X), E=40, 100, 200, 300, 425, 550, 650, 800 MeV/nucleon; calculated reaction σ, density distributions using Glauber model. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.034607
2007HO09 Phys.Rev. C 75, 044607 (2007); Erratum Phys.Rev. C 76, 039903 (2007) W.Horiuchi, Y.Suzuki, B.Abu-Ibrahim, A.Kohama Systematic analysis of reaction cross sections of carbon isotopes NUCLEAR REACTIONS 12C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (22C, X), E=40-1000 MeV/nucleon; calculated reaction σ. Glauber approximation, eikonal model, comparison with data.
doi: 10.1103/PhysRevC.75.044607
2005AB02 Prog.Theor.Phys.(Kyoto) 113, 341 (2005) Breakup Effect on the Reactions of 4, 6He and 6Li NUCLEAR REACTIONS 1H, 12C, 40Ca(6He, X), E=100, 200, 400 MeV/nucleon; 1H(α, X), (6Li, X), E=100 MeV/nucleon; calculated dynamic polarization potentials. 1H, 12C, 40Ca(6He, X), E ≈ 50-1000 MeV/nucleon; calculated reaction σ. 1H(6He, 6He), E=200 MeV/nucleon; calculated σ(θ). Eikonal and folding model calculations, role of breakup channels discussed.
doi: 10.1143/PTP.113.341
2005KA49 Eur.Phys.J. A 25, Supplement 1, 261 (2005) R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata A new view to the structure of 19C NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E not given; measured longitudinal momentum distributions; deduced role of neutron evaporation. Comparison with Glauber model calculations.
doi: 10.1140/epjad/i2005-06-183-0
2005KA51 Eur.Phys.J. A 25, Supplement 1, 327 (2005) R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata Observation of a two-proton halo in 17Ne NUCLEAR REACTIONS Be(17Ne, 15OX), E=64 MeV/nucleon; measured fragments longitudinal momentum distributions, interaction σ. 17Ne deduced two-proton halo features. Few-body Glauber model analysis.
doi: 10.1140/epjad/i2005-06-184-y
2004AB12 Nucl.Phys. A738, 440 (2004) Breakup effects in 6He + 12C elastic scattering NUCLEAR REACTIONS 12C(6He, 6He), E=40 MeV/nucleon; calculated σ(θ); deduced breakup channel contribution.
doi: 10.1016/j.nuclphysa.2004.04.082
2004AB13 Phys.Rev. C 70, 011603 (2004) Dynamic polarization potentials for the halo nucleus 6He in medium-energy elastic scattering NUCLEAR REACTIONS 12C(6He, 6He), E=40-800 MeV; calculated reaction σ, σ(θ), dynamic polarization potentials.
doi: 10.1103/PhysRevC.70.011603
2004AB29 Prog.Theor.Phys.(Kyoto) 112, 1013 (2004); Addendum Prog.Theor.Phys.(Kyoto) 114, 901 (2005) Breakup of One-Neutron Halo Nuclei within Eikonal Model NUCLEAR REACTIONS 12C, 208Pb(11Be, n10Be), (19C, n18C), E=68, 520 MeV/nucleon; calculated elastic and inelastic breakup probabilities, σ(E). Eikonal model, comparison with data.
doi: 10.1143/PTP.112.1013
2004CH43 Nucl.Phys. A741, 29 (2004) M.Chiba, R.Kanungo, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, I.Tanihata, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng Neutron removal studies on 19C NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E=64 MeV/nucleon; measured one- and two-neutron removal σ, longitudinal momentum distributions. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.06.009
2004II02 Prog.Theor.Phys.(Kyoto), Suppl. 156, 139 (2004) K.Iida, K.Oyamatsu, B.Abu-Ibrahim Deducing the Density Dependence of the Symmetry Energy from Unstable Nuclei NUCLEAR REACTIONS 58Ni(p, p), E=400, 1047 MeV; 58,80Ni, 124Sn, 208Pb(p, p), E=800 MeV; calculated σ(θ), density dependence features. Glauber model.
doi: 10.1143/PTPS.156.139
2004JE07 Nucl.Phys. A739, 57 (2004) H.Jeppesen, R.Kanungo, B.Abu-Ibrahim, S.Adhikari, M.Chiba, D.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, I.Tanihata, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng One- and two-proton removal from 15O NUCLEAR REACTIONS Be(15O, 14NX), (15O, 13CX), E=56 MeV/nucleon; measured parallel momentum distributions. 15O deduced valence proton configuration. 17Ne deduced halo features.
doi: 10.1016/j.nuclphysa.2004.03.145
2004SU26 Phys.Rev. C 70, 051302 (2004) Y.Suzuki, H.Matsumura, B.Abu-Ibrahim Structure of 15, 16C and phenomenology of the hindered E2 transition in 16C NUCLEAR STRUCTURE 15,16C; calculated levels, J, π, radii. 15,16C, 17F, 18Ne, 17,18O; analyzed transitions B(E2); deduced polarization charge. NUCLEAR REACTIONS 12C(16C, 15CX), E=83 MeV/nucleon; calculated fragment parallel momentum distribution. Comparison with data.
doi: 10.1103/PhysRevC.70.051302
2003AB05 Comput.Phys.Commun. 151, 369 (2003) B.Abu-Ibrahim, Y.Ogawa, Y.Suzuki, I.Tanihata Cross section calculations in Glauber model: I. Core plus one-nucleon case NUCLEAR REACTIONS 12C(12C, X), (13C, X), E=100-1000 MeV/nucleon; calculated total reaction σ. 12C(19C, n18C), E=100-1000 MeV/nucleon; calculated elastic and inelastic neutron-removal σ. 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ). 9Be(11Be, 10BeX), E=63 MeV/nucleon; 12C(8B, 7BeX), E=1.44 GeV/nucleon; calculated fragment longitudinal momentum distribution. Glauber model, comparisons with data.
doi: 10.1016/S0010-4655(02)00734-8
2003AB26 Nucl.Phys. A728, 118 (2003); Erratum Nucl.Phys. A732, 218 (2004) The optical potential of 6He in the eikonal approximation NUCLEAR REACTIONS 12C(6He, 6He), E=40, 70, 200, 800 MeV/nucleon; 12C(α, α), E=40 MeV/nucleon; calculated σ(θ), phase shifts, optical potential, role of breakup channel. Eikonal approximation.
doi: 10.1016/j.nuclphysa.2003.08.025
2003II02 Phys.Lett. B 576, 273 (2003) K.Iida, K.Oyamatsu, B.Abu-Ibrahim Proton-nucleus elastic scattering and the equation of state of nuclear matter NUCLEAR REACTIONS 58Ni(p, p), E=400, 1047 MeV; 58,80Ni, 116,124Sn, 208Pb(p, p), E=800 MeV; calculated σ(θ); deduced dependence on nuclear matter density parameter. Glauber model.
doi: 10.1016/j.physletb.2003.10.019
2002AB16 Nucl.Phys. A706, 111 (2002) Calculation of Nucleus-Nucleus Cross Sections at Intermediate Energies using Glauber Theory NUCLEAR REACTIONS 12C(6He, X), (7Li, X), (7Be, X), (8He, X), (8Li, X), (8B, X), (9Li, X), (9Be, X), (9C, X), (10Be, X), (12C, X), (27Al, X), E=30, 200, 800 MeV/nucleon; calculated reaction σ. 12C(12C, 12C), E=200 MeV/nucleon; 12C(α, α), (6He, 6He), E=41.5 MeV/nucleon; calculated σ(θ). Glauber theory, optical potential, comparison with data.
doi: 10.1016/S0375-9474(02)00683-8
2000AB16 Phys.Rev. C61, 051601 (2000) Utility of Nucleon-Target Profile Function in Cross Section Calculations NUCLEAR REACTIONS 9Be, 12C, 27Al(α, X), (6He, X), (9Be, X), E=800 MeV/nucleon; 12C, 27Al(12C, X), E=800 MeV/nucleon; calculated reaction σ. 12C(α, α), E=1.37 GeV; 12C(α, α), (6He, 6He), E=800 MeV/nucleon; calculated σ(θ). Nuclear-target profile function, Glauber theory. Comparisons with data.
doi: 10.1103/PhysRevC.61.051601
2000AB31 Phys.Rev. C62, 034608 (2000) Scatterings of Complex Nuclei in the Glauber Model NUCLEAR REACTIONS 9Be, 12C, 27Al(6He, X), (7Li, X), (7Be, X), (8He, X), (8Li, X), (8B, X), (9Li, X), (9Be, X), (9C, X), (10Be, X), 12C, 27Al(12C, X), E=800 MeV/nucleon; calculated reaction σ. 12C(p, p), E=200, 398, 800 MeV; 12C(α, α), E=1.37 GeV; 12C, 208Pb(12C, 12C), E=200 MeV/nucleon; calculated σ(θ). 12C, 27Al, 63Cu, 208Pb(6He, X), (9Li, X), E=800 MeV/nucleon; calculated dissociation σ, Coulomb and nuclear contributions. Glauber model.
doi: 10.1103/PhysRevC.62.034608
1999AB37 Nucl.Phys. A657, 391 (1999) B.Abu-Ibrahim, K.Fujimura, Y.Suzuki Calculation of the Complete Glauber Amplitude for p + 6He Scattering NUCLEAR REACTIONS 6He(p, p), E=41, 71, 717 MeV; 4He(p, p), E=72, 700 MeV; calculated σ(θ). Glauber model, α+n+n cluster wave function. Comparison with data, other models.
doi: 10.1016/S0375-9474(99)00339-5
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