NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = K.A.Ramadan Found 11 matches. 2004MB04 Ukr.J.Phys. 49, 756 (2004) H.M.M.Mansour, Kh.A.Ramadan, M.Hammad Properties of nuclear and neutron matter using D1 Gogny force
2003IS18 Int.J.Mod.Phys. E12, 863 (2003) M.Ismail, M.Osman, Kh.A.Ramadan, W.Seif Effect of the adiabatic vibrational coupling on the fusion of the 16O-238U interaction NUCLEAR REACTIONS 238U(16O, X), E(cm) ≈ 70-100 MeV; calculated fusion σ, barrier distribution, effect of vibrational coupling.
doi: 10.1142/S0218301303001636
2003MA10 Turk.J.Phys. 27, 107 (2003) Semi-Infinite Polarized Nuclear Matter with a Seyler-Blanchard Interaction
2002MA65 Int.J.Mod.Phys. E11, 445 (2002) Neutron Matter Properties Using Generalized Skyrme Force
doi: 10.1142/S0218301302000971
2002RA22 Int.J.Mod.Phys. E11, 143 (2002) Nuclear Matter Properties using Different Sets of Parameters in the Gogny Interaction
doi: 10.1142/S021830130200079X
2000IS06 Acta Phys.Pol. B31, 1783 (2000) Improving the Calculation of the Potential between Spherical and Deformed Nuclei NUCLEAR REACTIONS 238U(12C, X), (16O, X), (40Ar, X), (40Ca, X), (64Ni, X), (90Zr, X), (208Pb, X), E not given; calculated interactions potentials, deformation effects. 238U(16O, X), E(cm)=75-100 MeV; 238U(90Zr, X), E(cm)=330-410 MeV; calculated fusion σ. Finite-range nucleon-nucleon force.
2000IS09 J.Phys.(London) G26, 1621 (2000) Microscopic Calculation of Sub-Barrier Fusion Cross Section and Barrier Distribution using M3Y-Type Forces NUCLEAR REACTIONS 154Sm(16O, X), E(cm)=50-75 MeV; calculated fusion σ, barrier distribution; deduced effect of finite-range nucleon-nucleon interaction, sensitivity to deformation parameters. Comparisons with data.
doi: 10.1088/0954-3899/26/10/312
1998MA14 Phys.Rev. C57, 1744 (1998) Polarized Nuclear Matter using a Modified Density Dependent Seyler-Blanchard Potential
doi: 10.1103/PhysRevC.57.1744
1997IS08 Mod.Phys.Lett. A 12, 2065 (1997) M.Y.Ismail, Kh.A.Ramadan, M.M.Osman, F.Salah, A.Y.Ellithi The Orientation Dependence of the Real Part of the Ion-Ion Potential between Two Nuclei NUCLEAR REACTIONS 238U(α, X), (16O, X), (40Ca, X), (238U, X), E not given; calculated ion-ion potential; deduced orintation dependence. Extended Skyrme forces.
doi: 10.1142/S0217732397002119
1989IS02 J.Phys.(London) G15, 1033 (1989) M.Ismail, M.Osman, J.W.Guirguis, Kh.A.Ramadan, H.A.Zahra Comparison between the Double Folding Model and the Energy Density Approach for Calculating the Ion-Ion Potential NUCLEAR REACTIONS 40Ca(12C, 12C), E=45, 51 MeV; 208Pb(12C, 12C), E=96 MeV; 90Zr(12C, 12C), E=98 MeV; 40Ca(16O, 16O), E=74.4 MeV; 60Ni(16O, 16O), E=61.4, 141.7 MeV; 208Pb(16O, 16O), E=86, 192, 312.6 MeV; 120Sn, 208Pb, 60Ni(40Ar, 40Ar), E=1760 MeV; 40Ca(40Ca, 40Ca), E=143.6 MeV; calculated ion-ion potentials; deduced parameter comparison. Different models.
doi: 10.1088/0954-3899/15/7/011
1986MA50 Phys.Rev. C34, 1278 (1986) H.M.M.Mansour, M.Ismail, M.Osman, Kh.A.Ramadan Real Part of the Interaction Potential between Two 238U Nuclei NUCLEAR REACTIONS 238U(238U, 238U), E=6.02 MeV/nucleon; calculated interaction potential characteristics; deduced interacting nuclei relative orientation role.
doi: 10.1103/PhysRevC.34.1278
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