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NSR database version of April 11, 2024.

Search: Author = B.Abu-Ibrahim

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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
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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
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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
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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
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2011AB02      Phys.Rev. C 83, 044615 (2011)

B.Abu-Ibrahim

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
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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
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2010AB13      Phys.Rev. C 81, 057601 (2010)

B.Abu-Ibrahim, A.Kohama

Scaling properties of proton-nucleus total reaction cross sections

doi: 10.1103/PhysRevC.81.057601
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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
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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
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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
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2005AB02      Prog.Theor.Phys.(Kyoto) 113, 341 (2005)

B.Abu-Ibrahim

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
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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
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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
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2004AB12      Nucl.Phys. A738, 440 (2004)

B.Abu-Ibrahim, Y.Suzuki

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
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2004AB13      Phys.Rev. C 70, 011603 (2004)

B.Abu-Ibrahim, Y.Suzuki

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
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2004AB29      Prog.Theor.Phys.(Kyoto) 112, 1013 (2004); Addendum Prog.Theor.Phys.(Kyoto) 114, 901 (2005)

B.Abu-Ibrahim, Y.Suzuki

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1906.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1902.


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
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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
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2003AB26      Nucl.Phys. A728, 118 (2003); Erratum Nucl.Phys. A732, 218 (2004)

B.Abu-Ibrahim, Y.Suzuki

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
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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
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2002AB16      Nucl.Phys. A706, 111 (2002)

B.Abu-Ibrahim

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
Citations: PlumX Metrics


2000AB16      Phys.Rev. C61, 051601 (2000)

B.Abu-Ibrahim, Y.Suzuki

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
Citations: PlumX Metrics


2000AB31      Phys.Rev. C62, 034608 (2000)

B.Abu-Ibrahim, Y.Suzuki

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
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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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