NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = M.Y.Hassan Found 31 matches. 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
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
2008HA03 J.Phys.(London) G35, 025104 (2008) M.Y.M.Hassan, H.Hosny, I.A.Abdallah, A.El-Nahhas Elastic and inelastic proton-nucleus scattering using eikonal phase for the Symmetrized Woods-Saxon optical potential NUCLEAR REACTIONS 12C, 16O, 24Mg, 90Zr, 120Sn, 144Sm, 176Yb, 208Pb(p, p), e=800 MeV; 12C, 154Sm, 176Yb(p, p'), E=800 MeV; calculated cross sections and angular distributions. Compared results to available data.
doi: 10.1088/0954-3899/35/2/025104
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
2004FA14 Czech.J.Phys. 54, 633 (2004) 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
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
2004GH02 Eur.Phys.J. A 19, 221 (2004) A.Sh.Ghazal, M.S.M.Nour El-Din, M.Y.M.Hassan Effect of density-dependent nucleon-nucleon cross-section on elastic scattering NUCLEAR REACTIONS 12C(12C, 12C), E=300, 360, 1016, 1441, 2400 MeV; calculated reaction σ, σ(θ); deduced effect of density-dependent nucleon-nucleon cross-section. Glauber phase-shift formula, comparison with data.
doi: 10.1140/epja/i2003-10101-8
2003FA06 Czech.J.Phys. 53, 473 (2003) 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
2002FA14 Int.J.Mod.Phys. E11, 425 (2002) 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
2002HA08 Acta Phys.Slovaca 52, 23 (2002) First and Second Order Corrections to the Eikonal Phase Shifts for the Interactions of α-Particle with 12C and Ca Isotopes NUCLEAR REACTIONS 12C, 40,44,48Ca(α, X), (α, α), E=1370 MeV; calculated optical potentials, elastic scattering σ(θ), transparency function. First- and second-order corrections, comparison with data.
2000EL03 Phys.Rev. C61, 044604 (2000) M.M.H.El-Gogary, A.S.Shalaby, M.Y.M.Hassan, A.M.Hegazy Full Glauber Series Analysis for Elastic Scattering with Consistent Center-of-Mass Correlations NUCLEAR REACTIONS 12C(α, α), E=1.37, 4.2 GeV; 12C(12C, 12C), E=1.016, 1.44 GeV; 12C(16O, 16O), E=1.503 GeV; 16O(16O, 16O), E=0.704 GeV; calculated σ(θ). Full Glauber series calculations with consistent center-of-mass correlations.
doi: 10.1103/PhysRevC.61.044604
1998EL14 Phys.Rev. C58, 3513 (1998) M.M.H.El-Gogary, A.S.Shalaby, M.Y.M.Hassan Elastic Scattering between Two Cluster Nuclei (A, B ≥ 4) at Medium and High Energies NUCLEAR REACTIONS 4He(α, α), E at 4.32, 5.07, 7 GeV/c; 12C, 40Ca(α, α), E at 1.37 GeV/c; 12C(12C, 12C), E=1.0, 1.4, 2.4 GeV; 16O(12C, 12C), E=1.5 GeV; calculated σ(θ); deduced higher-order terms, phase variation effects. Glauber multiple scattering theory.
doi: 10.1103/PhysRevC.58.3513
1997MA46 Phys.Rev. C56, 1418 (1997) H.M.M.Mansour, M.Hammad, M.Y.M.Hassan Polarized Nuclear Matter using Extended Seyler-Blanchard Potentials
doi: 10.1103/PhysRevC.56.1418
1997SH34 Phys.Rev. C56, 2889 (1997) A.S.Shalaby, M.M.H.El-Gogary, M.Y.M.Hassan Comment on ' Method for Calculating Elastic Scattering between Two Composite Many-Body Systems at High Energies '
doi: 10.1103/PhysRevC.56.2889
1996RA12 Phys.Rev. C53, 1670 (1996) S.Ramadan, M.Abd-Alla, M.Y.M.Hassan Thermostatic Properties of Semi-Infinite Polarized Nuclear Matter NUCLEAR STRUCTURE A ≤ 250; calculated level density parameter vs mass. Semi-infinite polarized nuclear matter.
doi: 10.1103/PhysRevC.53.1670
1995MO11 Acta Phys.Pol. B26, 43 (1995) S.A.Moharram, A.S.Shalaby, A.Y.Ellithi, M.Y.M.Hassan, H.M.M.Mansour The Effect of Multiple-Scattering and Density Distribution on the Elastic Scattering of High-Energy Electrons NUCLEAR REACTIONS 12C(e, e), E=240.17-450 MeV; 16O(e, e), E=240, 420 MeV; 40Ca(e, e), E=183-251.5 MeV; 208Pb(e, e), E=175 MeV; calculated σ(θ). Multiple scattering Glauber theory, eikonal approximation.
1991TA01 J.Phys.(London) G17, 271 (1991) I.M.A.Tag Eldin, E.H.Esmael, M.Y.M.Hassan, M.N.H.Comsan Elastic Scattering of Intermediate Energy Hadrons from 12C NUCLEAR REACTIONS 12C(p, p), E=150-1040 MeV; 12C(p-bar, p-bar), E=46.8, 179.7 MeV; 12C(π-, π-), E=180, 260 MeV; analyzed σ(θ). Glauber multiple scattering theory.
doi: 10.1088/0954-3899/17/3/010
1990TA13 J.Phys.(London) G16, 1051 (1990) I.M.A.Tag Eldin, E.H.Esmael, M.Y.M.Hassan, M.N.H.Comsan Study of the Optical Potential for Hadron-Nucleus Scattering using Glauber's Theory NUCLEAR REACTIONS 12C, 40Ca(p, p), E=0.1-1 GeV; 12C, 40Ca(π+, π+), E=90-280 MeV; 12C, 40Ca(π-, π-), E=180, 260 MeV; 12C, 40Ca(p-bar, p-bar), E=46.8, 179.7 MeV; calculated potential parameters. Glauber theory.
doi: 10.1088/0954-3899/16/7/016
1989HA24 Ann.Phys.(Leipzig) 46, 207 (1989) M.Y.M.Hassan, M.N.H.Comsan, I.M.A.Tageldin Analytical l-Dependent Folding Potential According to Alpha-Cluster Model - I NUCLEAR REACTIONS 12C, 16O(n, n), (α, α), E not given; calculated folding potential parameters. Alpha-cluster model matter densities.
doi: 10.1002/andp.19895010308
1988HA38 Ann.Phys.(Leipzig) 45, 285 (1988) M.Y.M.Hassan, G.M.Al-Halmoushi, S.Moharram On the Relation between Effective Potentials and Realistic Potentials NUCLEAR STRUCTURE 12C, 16O; calculated binding energy. Realistic, effective potentials.
doi: 10.1002/andp.19885000407
1980HA38 Ann.Phys.(Leipzig) 37, 16 (1980) M.Y.M.Hassan, S.Moharram, M.M.Osman Alpha Cluster in Hartree-Fock Calculations NUCLEAR STRUCTURE 12C; calculated ground state energy, rms radius. Hartree-Fock method, α-cluster, velocity dependent effective interactions.
doi: 10.1002/andp.19804920103
1979HA50 Acta Phys.Pol. B10, 77 (1979) Hartree Fock Calculations for Even-Even N = Z Nuclei in the 2s-1d Shell Using Velocity-Dependent Effective Potential of s-Wave Interaction NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 40Ca; calculated binding energies, rms radii. Hartree-Fock calculations, velocity-dependent S-wave interaction.
1979HA51 Acta Phys.Pol. B10, 555 (1979) M.Y.M.Hassan, S.Moharram, H.M.Abdel-Monem Hartree-Fock Calculations for Even-Even Nuclei in the 2p-1f Shell using a Velocity Dependent s-Wave Effective Interaction NUCLEAR STRUCTURE 42,44,46,48Ca, 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe, 56,58,60,62Ni, 60,62,64,68Zn, 64,70,72Ge; calculated binding energies, quadrupole moments, energy gaps, pick up strengths. Hartree-Fock calculations, inert 40Ca core, velocity-dependent S-wave effective interaction.
1979HA52 Atomkernenergie 33, 215 (1979) Analysis of C12(p, Li6)Be7 Reaction in the Energy Range 36-56.8 MeV NUCLEAR REACTIONS 12C(p, 6Li), E=36-56.8 MeV; calculated σ(θ). Zero range DWBA knockout mechanism.
1979HA53 Atomkernenergie 33, 217 (1979) On the Structure of 12C NUCLEAR STRUCTURE 12C; calculated first excited state T1/2. Brink model. NUCLEAR REACTIONS 12C(p, p), E=152 MeV; calculated σ(θ). Brink model parameters from electron scattering data.
1979HA59 Acta Phys.Pol. B10, 845 (1979) M.Y.M.Hassan, S.Moharram, M.M.Osman, H.M.Abdel Monem Nuclear Structure Calculations with a Velocity Dependent Effective Potential for s-d and p-f Shell Nuclei NUCLEAR STRUCTURE A=12-40; calculated binding energy, quadrupole moment. Hartree-Fock method, velocity dependent effective potential.
1978HA04 Z.Phys. A285, 37 (1978) M.Y.M.Hassan, E.H.Ismail, A.Rabie On the Knock-Out Mechanism for the 12C(p, α)9B Reaction NUCLEAR REACTIONS 12C(p, α); calculated σ(θ). Reaction mechanism study.
doi: 10.1007/BF01410221
1978HA43 Atomkernenergie 32, 193 (1978) M.Y.M.Hassan, A.Rabie, M.S.M.Noor El-Din On the Deformation of the α-Clusters Inside Light Nuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne; calculated elastic scattering form factor. Phenomenological model with α-cluster deformation.
1975HA48 Z.Phys. A275, 169 (1975) Elastic and Inelastic Scattering of 185 MeV Protons from 6Li NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=185 MeV; calculated σ(θ). Plane wave impulse approximation.
doi: 10.1007/BF01409593
1971DA25 Phys.Rev. C4, 1985 (1971) J.Dabrowski, E.Fedorynska, P.Haensel, M.Y.M.Hassan Binding Energy of 3H and n-d-Doublet Scattering Length with Charge-Dependent Forces NUCLEAR STRUCTURE 3H; calculated binding energy, n-d doublet scattering length. Charge-dependent forces.
doi: 10.1103/PhysRevC.4.1985
1966HA17 Nucl.Phys. 78, 593 (1966) M.Y.M.Hassan, Z.Skladanowski, Z.Szymanski Equilibrium Deformations of the Odd-Mass Nuclei in the Rare-Earth Region
doi: 10.1016/0029-5582(66)90897-2
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