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NSR database version of May 10, 2024.

Search: Author = M.Y.Farag

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2019FA06      Nucl.Phys. A989, 21 (2019)

M.Y.H.Farag, E.H.Esmael, I.A.M.Abdul-Magead, S.S.Mousa

New empirical formulae for the in-medium nucleon-nucleon cross-section

NUCLEAR REACTIONS 1H(n, x), (p, x), E=40-1000 MeV/nucleon; calculated σ using Glauber model, developed new empirical formula yielding results close to those calculated; deduced formula parameters, application of the formula to the absorption σ of protons on 4He - 27Al.

doi: 10.1016/j.nuclphysa.2019.05.011
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2014FA08      Eur.Phys.J. A 50, 106 (2014)

M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Energy-dependent microscopic optical potential for scattering of nucleons on light nuclei

NUCLEAR REACTIONS 4,6,8He(p, p), E=5-160 MeV;6,7Li, 9,10Be(p, p), E=5-200 MeV; calculated σ, σ(θ), reaction σ using optical model; deduced optical model parameters to fit the data.

doi: 10.1140/epja/i2014-14106-x
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2014FA15      Phys.Rev. C 90, 034615 (2014)

M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Analysis of proton-9, 10, 11, 12Be scattering using an energy-, density-, and isospin-dependent microscopic optical potential

NUCLEAR REACTIONS 9,10,11,12Be(p, p), E=3-200 MeV/nucleon; analyzed data for differential σ(E, θ), reaction σ(E), analyzing power Ay(θ), volume integrals data, matter rms radii, eikonal approximation for 9Be(p, p) data at higher energies. Energy-, density-, and isospin-dependent microscopic optical potential model with the partial-wave expansion method.

doi: 10.1103/PhysRevC.90.034615
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2013FA11      Phys.Rev. C 88, 064602 (2013)

M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Elastic interaction of protons with stable and exotic light nuclei

NUCLEAR REACTIONS 4He(p, p), E=12.04, 17.45, 31, 40, 52.3, 64.9, 71.9, 85, 156 MeV/nucleon; 6He(p, p), E=25.1, 38.3, 40.9, 41.6, 71 MeV/nucleon; 8He(p, p), E=15.7, 26.1, 32.5, 66, 72 MeV/nucleon; 6Li(p, p), E=6, 10, 25.9, 29.9, 35, 40.1, 45.4, 49.75, 65, 72, 135, 155 MeV/nucleon; 7Li(p, p), E=6.15, 10.3, 24.4, 49.74, 65, 155 MeV/nucleon; 9Li(p, p), E=60 MeV/nucleon; 11Li(p, p), E=62 MeV/nucleon; analyzed experimental σ(E, θ) data using calculated Greens function Monte Carlo (GFMC) density for light stable nuclei and large-scale shell model (LSSM) density for exotic (halo) nuclei; deduced optical model parameters, and normalization parameters. Folding optical model with different density distributions and M3Y effective nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.88.064602
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2012FA14      Eur.Phys.J. A 48, 154 (2012)

M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Microscopic study on proton elastic scattering of light exotic nuclei at energies below than 100 MeV/nucleon

NUCLEAR REACTIONS 6He(p, p), E=25.1, 38.3, 40.9, 41.6, 71.0 MeV/nucleon;8He(p, p), E=15.7, 26.1, 32.5, 66.0, 72.0 MeV/nucleon;9Li(p, p), E=60 MeV/nucleon;11Li(p, p), E=62, 68.4, 75.0 MeV/nucleon;10Be(p, p), E=39.1, 59.4 MeV;11Be(p, p), E=38.4, 49.3 MeV/nucleon;12Be(p, p), E=55.0 MeV/nucleon; calculated target nuclei density vs radius, σ(θ), σ, halo nuclei, volume integrals; deduced, analyzed optical model parameters, renormalization parameters. 6,8He(p, p), E=71 MeV/nucleon;calculated analyzing powers. Folding optical model with different density distributions and M3Y effective nucleon-nucleon interaction; calculated results compared to data. Several typing errors on energies.

doi: 10.1140/epja/i2012-12154-x
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2009HA04      Phys.Rev. C 79, 014612 (2009)

M.Y.M.Hassan, M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Microscopic model analysis of 11Li +p elastic scattering at 62, 68.4, and 75 MeV/nucleon

NUCLEAR REACTIONS 1H(11Li, 11Li), E=62, 68.4, 72 MeV/nucleon; calculated σ, optical potentials in the framework of single folding model. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.014612
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2009HA18      Phys.Rev. C 79, 064608 (2009)

M.Y.M.Hassan, M.Y.H.Farag, E.H.Esmael, H.M.Maridi

Elastic scattering and breakup effect analysis of 11Be+12C at 38.4 MeV/nucleon

NUCLEAR REACTIONS 12C(11Be, 11Be), E=38.4 MeV/nucleon; analyzed σ(θ) and folded potentials using optical model in the framework of Double folding model with M3Y effective nucleon-nucleon interactions. 11Be; deduced microscopic dynamical polarization potential (DPP).

doi: 10.1103/PhysRevC.79.064608
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2008HA34      Phys.Scr. 78, 045202 (2008)

M.Y.M.Hassan, M.Y.H.Farag, A.Y.Abul-Magd, T.E.I.Nassar

Nucleus-nucleus reaction cross sections for deformed nuclei

NUCLEAR REACTIONS 27Al(12C, X), (20Ne, X), E=30-900 MeV/nucleon; 64Zn(12C, X), E=30-900 MeV/nucleon; 90Zr(12C, X), E=10-35 MeV/nucleon; 238U(20Ne, X), (40Ar, X), E=30-900 MeV/nucleon; calculated reaction cross sections using the Coulomb-modified Glauber model. Compared results to available data.

doi: 10.1088/0031-8949/78/04/045202
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2004FA08      Czech.J.Phys. 54, 317 (2004)

M.Y.H.Farag

Effect of the in-medium nucleon-nucleon interaction on the nucleus-nucleus cross-sections

NUCLEAR REACTIONS 12C, 27Al, 57Fe, 66Zn, 89Y(12C, X), (12C, 12C), E=25-343 MeV/nucleon; 12C, 27Al, 40Ca(20Ne, X), (20Ne, 20Ne), E=25-343 MeV/nucleon; calculated total, elastic, and reaction σ, in-medium effects. Modified Glauber models.

doi: 10.1023/B:CJOP.0000018128.04049.fa
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2004FA14      Czech.J.Phys. 54, 633 (2004)

M.Y.H.Farag, M.Y.M.Hassan

Nucleus-nucleus elastic scattering with Pauli correlation effect

NUCLEAR REACTIONS 16O(16O, 16O), E=63 MeV; 28Si(16O, 16O), E=142.5 MeV; 24Mg(32S, 32S), E=110 MeV; calculated σ(θ), Pauli correlation effect. Optical model, comparison with data.

doi: 10.1023/B:CJOP.0000029692.91734.09
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2004FA19      Acta Phys.Pol. B35, 2085 (2004)

M.Y.H.Farag, E.H.Esmael, M.Y.M.Hassan

The dependence of the nucleon-nucleon scattering amplitude on the momentum transfer


2003FA06      Czech.J.Phys. 53, 473 (2003)

M.Y.H.Farag, M.Y.M.Hassan

Pauli correlation effect for the elastic scattering of protons by different nuclei at 800 MeV

NUCLEAR REACTIONS 16O, 20Ne(p, p), E=800 MeV; calculated optical potential, σ(θ); deduced Pauli correlation effects. Single folding model, comparison with data.

doi: 10.1023/A:1024601508818
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2002FA10      Czech.J.Phys. 52, 927 (2002)

M.Y.H.Farag

Description of elastic and reaction cross-sections of heavy ions using modified Glauber model

NUCLEAR REACTIONS 12C(16O, 16O), E=608, 1503 MeV; 28Si(16O, 16O), E=1503 MeV; 12C(12C, 12C), E=1016 MeV; 208Pb(13C, 13C), E=390 MeV; calculated reaction σ, elastic σ(θ), optical potential features. Glauber model, comparisons with data.

doi: 10.1023/A:1019813521177
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2002FA14      Int.J.Mod.Phys. E11, 425 (2002)

M.Y.H.Farag, M.Y.M.Hassan

Relativistic Optical Model for Proton-Nucleus Elastic Scattering

NUCLEAR REACTIONS 12C(p, p), E=800, 1040 MeV; 16O, 20Ne, 24Mg(p, p), E=800 MeV; calculated σ(θ). Relativistic optical model, comparisons with data.

doi: 10.1142/S0218301302000983
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2001FA24      Eur.Phys.J. A 12, 405 (2001)

M.Y.H.Farag

Modified Glauber Model for the Total Reaction Cross-Section of 12C + 12C Collisions

NUCLEAR REACTIONS 12C(12C, X), E=25-340 MeV/nucleon; calculated transparency funciton, reaction σ. 12C(12C, 12C), E=300, 360 MeV; calculated σ(θ). Modified Glauber model, comparisons with data.

doi: 10.1007/s10050-001-8664-2
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2000FA24      Acta Phys.Hung.N.S. 11, 195 (2000)

M.Y.H.Farag

Three- and Four-Body Events for the 16O + 16O Collisions

NUCLEAR REACTIONS 16O(16O, X), E(cm) ≈ 14-32 MeV; calculated fusion σ. 16O(16O, 3α), (16O, 2α), (16O, pα), (16O, np), E(cm)=60-200 MeV; calculated σ, fragment angular distributions; deduced role of sequential decay. Statistical scission model.


1999OS05      Acta Phys.Hung.N.S. 10, 73 (1999)

A.Osman, M.Y.H.Farag

Angular Distributions of the Multifragmentation of Deformed Nuclei in Heavy Ion Reactions

NUCLEAR REACTIONS 19F(9Be, X), E=35-407 MeV; calculated fission fragments angular distributions following compound nucleus decay. Statistical scission model.


1998FA23      Turk.J.Phys. 22, 29 (1998)

M.Y.H.Farag

Alpha Particle Fragments Produced From Multifragmentation of 16O + 16O

NUCLEAR REACTIONS 16O(16O, αX), E=70-160 MeV; calculated α-fragments angular distributions, nuclear temperature dependence. Statistical scission model.


1997FA27      Acta Phys.Hung.N.S. 5, 117 (1997)

M.Y.H.Farag

On the Mechanism of Multifragmentation of 12C + 16O Reactions

NUCLEAR REACTIONS 16O(12C, X), E=70-350 MeV; calculated fission σ, α fragments σ(θ). Statistical scission model.


1996OS07      Nuovo Cim. 109A, 1449 (1996)

A.Osman, M.Y.H.Farag

Multifragmentation of 24Mg + 24Mg Heavy-Ion Reactions Leading to Alpha-Particles

NUCLEAR REACTIONS 24Mg(24Mg, F), E(cm)=35-80 MeV; calculated σ(θα) following primary fission fragment breakup. Statistical scission model.

doi: 10.1007/BF02780615
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1995OS04      Nuovo Cim. 108A, 155 (1995)

A.Osman, M.Y.H.Farag

Angular Distributions of Alpha Fragments from Carbon-Induced Fission

NUCLEAR REACTIONS 12C(12C, F), E=70-160 MeV; calculated σ(θα) following fission at various temperatures. Statistical scission model, 6α fragmentation product.

doi: 10.1007/BF02816736
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1988OS04      Ann.Phys.(Leipzig) 45, 331 (1988)

A.Osman, M.Y.H.Farag

Bound Three Alpha Particles Model for the 12C Nucleus as a Three-Body Problem

NUCLEAR STRUCTURE 12C; calculated α-α interaction form factor for different levels.

doi: 10.1002/andp.19885000503
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1985OS03      Acta Phys.Pol. B16, 59 (1985)

A.Osman, M.Y.H.Farag

Study of the 6Li Nucleus as a Three-Body Problem

NUCLEAR STRUCTURE 6Li; calculated binding energies, form factors. Three-body model.


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