NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Ismail Found 115 matches. Showing 1 to 100. [Next]2024IS01 Phys.Rev. C 109, 014606 (2024) M.Ismail, S.G.Abd-Elnasser, A.Adel, I.A.M.Abdul-Magead, H.M.Elsharkawy Systematic investigation of α- and cluster-decay modes in superheavy nuclei
doi: 10.1103/PhysRevC.109.014606
2023IS01 Nucl.Phys. A1029, 122547 (2023) M.Ismail, S.G.Abd-Elnasser, H.M.Elsharkawy, I.A.M.Abdul-Magead Alpha decay around shell closures and correlation of half-life times with the neutron energy levels of the emitting nuclei RADIOACTIVITY 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122Ba, 124,126Ba, 154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186Hf, 106Te, 108,109Te, 109,110Xe, 112,113Xe, 114Ba, 144Nd, 146,147,148Sm, 148,149,150,151,152Gd, 150,151,152,153,154Dy, 152Er, 154,155Er, 154,156,158Yb, 156,157,158Hf, 160,162Hf, 162,163,164W, 166W, 161,162Os, 166,167,168,169,170Os, 172,173,174Os, 184Os, 168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190Pt, 172,174Hg, 175,176,177,178,179,180,181,182,183,184,185,186,187,188Hg, 178,180,182,184,186,188,190,192,194Pb(α); calculated T1/2. Comparison with available data.
doi: 10.1016/j.nuclphysa.2022.122547
2022IS03 J.Phys.(London) G49, 075102 (2022) Cluster radioactivity around shell closures: correlation of half-lives with the energy levels of daughter nuclei RADIOACTIVITY 221Fr, 221,222,223,224,225,226Ra, 225Ac(14C), 228Th(20O), 231Pa(23F), 230U(22Ne), 230Th, 231Pa, 232,233,234U(24Ne), 234U(26Ne), 234U, 235U, 236,238Pu(28Mg), 238Pu(30Mg), (32Si), 242Cm(34Si); calculated T1/2 using the universal decay law (UDL) formula, as well as the double-folding model derived from the Michigan three-range Yukawa-Paris NN interaction with zero- and finite-range exchange components.
doi: 10.1088/1361-6471/ac6273
2022IS07 Phys.Scr. 97, 0753032 (2022) M.Ismail, A.Y.Ellithi, A.Adel, M.A.Abbas Improved empirical formulas for α-decay half-lives of heavy and superheavy nuclei RADIOACTIVITY 295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340,341,342,343,344,345,346,347,348,349,350120, 304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339121, 301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340,341,342,343,344,345122, 348122, 350122, 310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339123, 307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340124, 342,344,346,348,350124, 316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339125, 313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340126, 324,326,328,330,332,334,336,338,340,342,344,346,348,350126(α); calculated T1/2.
doi: 10.1088/1402-4896/ac758c
2022IS09 Eur.Phys.J. A 58, 225 (2022) M.Ismail, A.Y.Ellithi, A.Adel, M.A.Abbas An improved unified formula for α-decay and cluster radioactivity of heavy and superheavy nuclei RADIOACTIVITY 221Fr, 221,222,223,224Ra, 226Ra, 225Ac(14C), 228Th(20O), 230U(22Ne), 230Th, 231Pa, 232,233,234U(24Ne), 234U(26Ne), 234,235U, 236,238Pu(28Mg), 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si), 220Ra(12C), 222Ra(18O), 226Ra(20O), 224,226,228Th(24Ne), 230U(32S), 230U(24Ne), 230U(20O), 232U(28Mg), 236Pu(24Ne), 238Cm(32Si), 240Cm(34Si), 242Cm(32Si), 220Ra(16O), 224Ra(20O), 224Th(14C), 224Th(16O), 226Th(14C), 226Th(18O), 228Th, 230U(14C), 230U(28Mg), 232U(32Si), 234Pu(24Ne), 234Pu(28Mg), 234,236Pu(32Si), 238Cm(28Mg), 240Cm(32Si), 242Cm(34Si), 242Cf(32Si), 244Cf(34Si), 246Cf(38S), 244Cm(34Si), 242Cf(35S), 223Ra, 225Ac(18O), 229Th(24Ne), 225Np(12C), 225,227Np(16O), 227Np(18O), 231Np(20O), 233Np(22Ne), 237Np, 237Pu(32Si), 237Am(28Mg), 237,239Am(32Si), 239,241Am(34Si), 229Th(14C), 231Pa(22O), 231Pa(28Si), 233U(28Mg), 225,227Np(14C), 229Np(18O), 231Np(22Ne), 233Np(24Ne), 235Np(28Mg), 237Pu(30Al), 239Am(30Mg), 239,241Cm(32Si), 243Cm(34Si), 249Cf(50Ca), 249Cf(42S), 249Cf(48Ca), 251Cf(46Ar), 232Pa, 236Np(28Mg), 236Np(30Mg), 238Am(28Mg), 238Am(32Si); calculated T1/2. Comparison with available data.
doi: 10.1140/epja/s10050-022-00882-9
2021IS07 Int.J.Mod.Phys. E30, 2150038 (2021) M.Ismail, A.Y.Ellithi, A.Khaled, H.Anwer New results on nuclear magicity and possible extension of the nuclear landscape NUCLEAR STRUCTURE Z=70-212; analyzed available data; calculated 3D surfaces of the shell-plus-pairing correction energy, proton shell corrections; deduced 83 magic nuclei.
doi: 10.1142/S0218301321500385
2020IS03 Phys.Rev. C 101, 024607 (2020) Prediction of α-decay chains and cluster radioactivity of 300-304121 and 302-306122 isotopes using the double-folding potential RADIOACTIVITY 300,301,302,303,304121, 296,297,298,299,300119, 292,293,294,295,296Ts, 288,289,290,291,292Mc, 284,285,286,287,288Nh, 280,281,282,283,284Rg, 276,277,278,279,280Mt, 272,273,274,275,276Bh, 268,269,270,271,272Db, 264,265,266,267,268Lr(α); 302,303,304,305,306122, 298,299,300,301,302120, 294,295,296,297,298Og, 290,291,292,293,294Lv, 286,287,288,289,290Fl, 282,283,284,285,286Cn, 278,279,280,281,282Ds, 274,275,276,277,278Hs, 270,271,272,273,274Sg, 266,267,268,269,270Rf(α); calculated α-decay half-lives using the density-dependent cluster model, with the α-nucleus potential from the double-folding model with a realistic NN interaction. Comparison with three semiempirical formulas: the Viola-Seaborg-Sobiczewski formula, the modified Brown formula, and the one based on fission theory. N=165-177; compared theoretical and experimental α-decay half-lives. N=288-342, Z=121; N=292-342, Z=122; calculated correlation between the logarithm of the α-preformation factor, Sα, and the fragmentation potential for odd-odd Z=121 and even-even Z=122 nuclei. 300121, 302122(α), (16O), (28Mg), (32Si), (68Ni), (76Zn), (79Ga), (80Ge), (83As), (84Se), (85Br), (86Kr), (89Rb), (90Sr), (91Sr), (92Sr), (93Sr), (94Sr), (96Y), (96Zr), (99Nb), (102Mo); calculated Q values, α-decay and cluster decay half-lives within the double-folding model based on M3Y-Paris NN interaction, unified formula (UF), Horai's scaling law, and the universal decay law (UDL).
doi: 10.1103/PhysRevC.101.024607
2020IS07 Int.J.Mod.Phys. E29, 2050065 (2020) Sequences of single-particle energy levels of even-even SHN with Z = 116 - 132 based on α-decay systematics NUCLEAR STRUCTURE Z=116-132; calculated Q-values, T1/2 within the density-dependent cluster model; deduced systematics.
doi: 10.1142/S0218301320500652
2020IS09 J.Phys.(London) G47, 055105 (2020) M.Ismail, A.Y.Ellithi, M.M.Selim, N.Abou-Samra, O.A.Mohamedien Semi-analytic calculations of barrier penetration and alpha particle preformation probabilities RADIOACTIVITY 106,107,108,109Te, 113I, 112,113Xe, 114Ba, 144Nd, 145Pm, 146,147,148Sm, 147,148Eu, 148,149,150,151,152Gd, 150,151,152,153,154Dy, 152,154Ho, 152,153,154,155Er, 153Tm, 155,156Tm, 154,155,156,157,158Yb, 156,157,158,159,160Hf, 162Hf, 174Hf, 159,160W, 162,164,166W, 180W, 160Re, 162,163Re, 162Os, 168,169,170Os, 172,173,174Os, 186Os, 166Ir, 169,170Ir, 176,177Ir, 168Pt, 170,171Pt, 174,176Pt, 177,178Pt, 180,181Pt, 183Pt, 188Pt, 190Pt, 170Au, 174Au, 183Au, 185Au, 174Hg, 176,177Hg, 180Hg, 182,183,184,185,186Hg, 188Hg, 177,179Tl, 186,188,190,192,194Pb, 210Pb, 190,192,194Po, 195,196,197,198,199,200,201,202Po, 204,205,206,207Po, 210Po, 212Po, 213,214,215,216Po, 218Po, 196,197,198,199,200,201,202,203,204,205,206,207,208,209At, 211,212,213,214,215At, 195Rn, 198Rn, 201Rn, 203,204Rn, 206,207,208,209,210Rn, 212Rn, 214,215,216,217,218Rn, 220,222Rn, 201Fr, 203,204,205,206,207,208,209,210,211Fr, 213Fr, 215,216,217,218,219Fr, 205,206,207Ra, 209,210,211,212Ra, 214Ra, 216,217,218Ra, 220,222,224,226Ra, 206Ac, 208,209Ac, 211,213,215,217Ac, 218,219Ac, 221,222Ac, 227Ac, 213Th, 216,218,220,222,224,226,228,230,232Th, 217,219Pa, 221,223Pa, 226,227Pa, 231Pa, 226,228U, 229U, 230,232U, 233,234U, 236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240Cf, 245,246Cf, 248,250,252,254Cf, 251,253Es(α); calculated T1/2. Comparison with experimental and UDL data.
doi: 10.1088/1361-6471/ab7291
2020IS11 Phys.Atomic Nuclei 83, 691 (2020) M.Ismail, A.Abdurrahman, A.R.Abdulghany Correlation Between the Behavior of α-Decay Half-Life Time and Q Values with Neutron Number Variation of Daughter Nuclei NUCLEAR STRUCTURE Z=80-122; analyzed available data for α-decay of 2000 nuclei; calculated T1/2 using the density-dependent cluster model with M3Y-effective nucleon-nucleon interaction.
doi: 10.1134/S1063778820050130
2019IS05 Ann.Phys.(New York) 406, 1 (2019) M.Ismail, W.M.Seif, W.M.Tawfik, A.M.Hussein Effect of choosing the Qα-values and daughter density distributions on the magic numbers predicted by α decays NUCLEAR STRUCTURE Z=118, 120, 122, 124; calculated α-decay T1/2. Comparison with available data.
doi: 10.1016/j.aop.2019.03.020
2019IS06 J.Phys.(London) G46, 075105 (2019) α-decay chains and cluster radioactivity of 295-299119 and 298-302120 isotopes using zero- and finite-range NN interactions RADIOACTIVITY 295119, 291Ts, 287Mc, 283Nh, 279Rg, 275Mt, 271Bh, 267Db, 263Lr, 259Md, 296119, 292Ts, 288Mc, 284Nh, 280Rg, 276Mt, 272Bh, 268Db, 264Lr, 260Md, 297119, 293Ts, 289Mc, 285Nh, 281Rg, 277Mt, 273Bh, 269Db, 265Lr, 261Md, 298119, 294Ts, 290Mc, 286Nh, 281Rg, 278Mt, 274Bh, 270Db, 266Lr, 262Md, 299119, 295Ts, 291Mc, 287Nh, 283Rg, 279Mt, 275Bh, 271Db, 267Lr, 263Md, 298120, 294Og, 290Lv, 286Fl, 282Cn, 278Ds, 274Hs, 270Sg, 266Rf, 262No, 299120, 295Og, 291Lv, 287Fl, 283Cn, 279Ds, 275Hs, 271Sg, 267Rf, 263No, 300120, 296Og, 292Lv, 288Fl, 284Cn, 280Ds, 276Hs, 272Sg, 268Rf, 264No, 301120, 297Og, 293Lv, 289Fl, 285Cn, 281Ds, 277Hs, 273Sg, 269Rf, 265No, 302120, 298Og, 294Lv, 290Fl, 286Cn, 282Ds, 278Hs, 274Sg, 270Rf, 266No(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1361-6471/ab1c28
2019SE03 Int.J.Mod.Phys. E28, 1950009 (2019) W.M.Seif, M.Ismail, I.A.M.Abdul-Magead, F.A.Fareed Influence of the deformation and orientation on the interaction potential of the 28Si + 28Si system and its fusion process NUCLEAR REACTIONS 28Si(28Si, X), E(cm)<40 MeV; calculated fusion σ. Comparison with available data.
doi: 10.1142/S0218301319500095
2018IS02 Phys.Rev. C 97, 044301 (2018) Theoretical predictions for α decay chains of 290-298118Og isotopes using a finite-range nucleon-nucleon interaction RADIOACTIVITY 294Og, 293,294Ts, 290,291,292,293Lv, 287,288,289,290Mc, 286,287,288,289Fl, 282,283,284,285,286Nh, 281,283,285Cn, 278,279,280,281,282Rg, 277,279,281Ds, 274,275,276,278Mt, 275Hs(α), (SF); calculated half-lives for α and SF decays using double-folding model with constant preformation factor, Viola-Seaborg-Sobiczewski (VSS) formula, modified Brown (mB1) formula, and semiempirical formula. Comparison with experimental half-lives. 290,291,292,293,294,295,296,297,298Og, 286,287,288,289,290,291,292,293,294Lv, 282,283,284,285,286,287,288,289,290Fl, 278,279,280,281,282,283,284,285,286Cn, 274,275,276,277,278,279,280,281,282Ds, 270,271,272,273,274,275,276,277,278Hs, 266,267,268,269,270,271,272,273,274Sg, 262,263,264,265,266,267,268,269,270Rf(α), (SF); calculated half-lives for α and SF decays using double-folding model with constant preformation factor, double-folding model with preformation factor extracted from cluster formation model, Viola-Seaborg-Sobiczewski (VSS) formula, modified Brown (mB1) formula, and semiempirical formula, and Q(α) values using WS4+ mass model.
doi: 10.1103/PhysRevC.97.044301
2017IS01 Nucl.Phys. A958, 202 (2017) M.Ismail, W.M.Seif, A.Adel, A.Abdurrahman Alpha-decay of deformed superheavy nuclei as a probe of shell closures RADIOACTIVITY Z=80-103, 111-122(α); calculated α-decay T1/2 (also for daughter nuclei) using density-dependent cluster model based on M3Y-Reid NN interaction; deduced neutron and proton magic numbers. Compared with data.
doi: 10.1016/j.nuclphysa.2016.11.010
2017IS06 Int.J.Mod.Phys. E26, 1750026 (2017) M.Ismail, A.Y.Ellithi, A.El-Depsy, O.A.Mohamedien Correlation between alpha preformation probability, decay half-life and barrier assault frequency RADIOACTIVITY 158,159,160,161,162,163,164,165,166,167W, 161,162,163,164,165,166,167,168,169,170,171,172,173,174Os, 186Os, 166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182Pt, 172,173,174,175,176,177,178,179,180Hg, 182,183,184,185,186Hg, 188Hg, 178,180,182,184,186,188,190Pb, 191,192Pb(α); calculated T1/2, preformation probability and assault frequency. Comparison with available data.
doi: 10.1142/S0218301317500264
2017IS15 J.Phys.(London) G44, 125106 (2017) The isovector nuclear density and improved description of cluster decay half-lives using isospin-dependent NN interaction RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C), 228Th(20O), 231Pa(23F), 230U(20Ne), 230Th, 231Pa, 232,233,234U(24Ne), 234U(26Ne), (28Mg), 235U(28Mg), 236,238Pu(28Mg), 238Pu(30Mg), (32Si), 242Cm(34Si); calculated T1/2. Comparison with experimental data.
doi: 10.1088/1361-6471/aa957f
2017SE07 J.Phys.(London) G44, 055102 (2017) Preformation probability inside α emitters around the shell closures Z = 50 and N = 82 RADIOACTIVITY 105,106,107,108,109,110Te, 111I, 109,110,111,112,113Xe, 112Cs, 114Ba, 144Nd, 145Pm, 146,147,148Sm, 147,148Eu, 148,149,150,151,152Gd, 150,151,152,153,154Dy, 152,154Ho, 113I, 152,153,154,155,156Er, 153,154,155,156Tm, 154,155,156,157,158Yb, 155,156Lu, 158,160Lu, 156,157,158,159,160Hf, 162Hf, 158,160Ta, 163Ta, 158,159,160,161,162,163,164,165,166,167,168W, 160,161,162,163,164,165,166Re, 161,162,163,164,165,166,167,168,169,170,171,172,173,174Os, 186Os, 166,167,168,169Ir, 177Ir, 166,167,168,169,170,171,172,173,174,175,176,177,178Pt, 180,181,182,183,184Pt, 186,188,190Pt, 170Au, 172,173Au, 175,177Au, 183,184,185Au, 172Hg, 174,175,176Hg, 180Hg, 182,183,184,185,186Hg, 188Hg, 177Tl, 179,180,181Tl, 183Tl, 151Ho, 153Ho, 159Lu, 157,159Ta, 167,169Re, 170,171Ir, 173Ir, 187Tl, 157Lu(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/1361-6471/aa6595
2016IS01 Can.J.Phys. 94, 102 (2016) Comparison between different proximity potentials and the double-folding model for spherical-deformed interacting nuclei NUCLEAR REACTIONS 238Pu(48Ca, X), E not given; calculated Coulomb barrier parameters. Comparison with available data.
doi: 10.1139/cjp-2015-0280
2016IS02 J.Phys.(London) G43, 015101 (2016) M.Ismail, A.Y.Ellithi, A.Adel, H.Anwer On magic numbers for super- and ultraheavy systems and hypothetical spherical double-magic nuclei NUCLEAR STRUCTURE Z=72-282; calculated 3D surface of the shell-plus-pairing energy corrections, contour maps of the shell-plus-pairing energy corrections for protons and neutrons, The proton/neutron shell correction energy and residual pairing correction; deduced proton/neutron magic numbers for N=96-540.
doi: 10.1088/0954-3899/43/1/015101
2016IS04 Nucl.Phys. A947, 64 (2016) M.Ismail, A.Y.Ellithi, A.Adel, A.R.Abdulghany Toward a better parameterization of nuclear density for α-decay calculation NUCLEAR STRUCTURE 208Pb; calculated neutron and proton density distribution, radius using proton and neutron densities given by 3pF (Three Parameter Fermi) distributions with neutron and proton radii and using HFB. RADIOACTIVITY 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218Po(α); calculated T1/2 using α-daughter potential, daughter proton and neutron densities given by 3pF (Three Parameter Fermi) distributions with neutron and proton radii and using HF density, α-preformation factor. T1/2 compared to data.
doi: 10.1016/j.nuclphysa.2015.12.008
2016IS05 Int.J.Mod.Phys. E25, 1650004 (2016) M.Ismail, A.Y.Ellithi, A.Adel, H.Anwer Structural properties of heavy and superheavy nuclei in a semi-microscopic approach NUCLEAR STRUCTURE Z=93-126; calculated 3D Coulomb energy surface of 317No, shell-plus-pairing energy corrections of the deformed isotopes and isotones 254No, 280No, 270Hs, 276Hs, 364126, 378126, 3D plot of the macroscpoic energy of 322Sg, half-density radii, deformation energy, ground state shapes, deformation parameters. Semi-microscopic model in which the Skyrme energy density functional with an empirical two-parameter Fermi density distribution is used to replace the macroscopic part in the MM approach.
doi: 10.1142/S021830131650004X
2016IS06 Int.J.Mod.Phys. E25, 1650026 (2016) M.Ismail, W.M.Seif, M.M.Botros Adiabatic and coupled channels calculations for near barrier fusion of 16O+238U using realistic nucleon-nucleon interaction NUCLEAR REACTIONS 238U(16O, X)254Fm, E(cm) < 96 MeV; calculated σ, fusion barrier distribution using potentials derived from the DD M3Y-Reid NN force. Comparison with experimental data.
doi: 10.1142/S0218301316500269
2016IS07 Phys.Rev. C 93, 054618 (2016) Nuclear spin of odd-odd α emitters based on the behavior of α-particle preformation probability RADIOACTIVITY 166,167,169,171,172,173,174,175,177Ir, 170,173,177,179,181,183,184,185,186Au, 177,179,180,181Tl, 184,185,186,187,188,189,190,191,192,193,194,195Bi, 191,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216At, 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221Fr, 206,207,208,209,210,211,212,213,214,215Ac(α); calculated half-lives and preformation probabilities; deduced Jπ values from systematics of preformation probabilities. Wentzel-Kramers-Brillouin (WKB) approximation in combination with Bohr-Sommerfeld quantization condition using a realistic density-dependent CDM3Y1-Paris NN interaction. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.054618
2016IS08 Phys.Rev. C 94, 024316 (2016) M.Ismail, W.M.Seif, A.Abdurrahman Relative stability and magic numbers of nuclei deduced from behavior of cluster emission half-lives RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 228Th(20O); 230U(22Ne); 231Pa(23F); 230Th, 231Pa, 232,233,234U(24Ne); 235U(25Ne); 234U(26Ne); 234,235U, 236,238Pu(28Mg); 238Pu(30Mg), (32Si); 242Cm(34Si); calculated cluster preformation probabilities, decay widths. Z=85-122(14C), (20O), (20Ne), (24Ne); calculated half-lives versus daughter neutron number for 7436 cluster decay processes. Density-dependent cluster model based on M3Y-ReidNN interaction; predicted magic neutron numbers at N=126, 148, 152, 154, 160, 162, 172, 176, 178, 180, 182, 184, and 200, and magic proton numbers at Z=82, 98, 100 102, 106, 108, 114, and 116. Comparison with available experimental data.
doi: 10.1103/PhysRevC.94.024316
2016IS10 Int.J.Mod.Phys. E25, 1650069 (2016) M.Ismail, A.Y.Ellithi, A.EL-Depsy, O.A.Mohamedien A systematic calculation of alpha decay half-lives using a new approach for barrier penetration probability NUCLEAR STRUCTURE Z=52-108; calculated T1/2. Comparison with experimental data.
doi: 10.1142/S0218301316500695
2016IS13 Chin.Phys.C 40, 124102 (2016) M.Ismail, A.Y.Ellithi, A.Adel, H.Anwer Islands of stability and quasi-magic numbers for super- and ultra-heavy nuclei NUCLEAR STRUCTURE Z=72-282, N=96-540; calculated the shell and the residual pairing correction energies for 5569 even-even nuclei; deduced quasi-magic numbers and deformed islands of stability that reside in a range defined by Green's formula and the two-neutrons drip line.
doi: 10.1088/1674-1137/40/12/124102
2016IS14 Eur.Phys.J. A 52, 317 (2016) M.Ismail, W.M.Seif, A.S.Hashem Ternary fission of 260No in equatorial configuration RADIOACTIVITY 260No(SF); calculated possible channels of equatorial ternary fission using three-cluster model with three-body potential from folded M3Y-Reid nucleon-nucleon force plus Coulomb force with relative orientation of deformed heavy nuclei taken into account, considered even-mass clusters with mass from 4 to 52 as emitted light particles; deduced reaction Q-value, most probable equatorial ternary fission combinations.
doi: 10.1140/epja/i2016-16317-5
2016SE08 J.Phys.(London) G43, 075101 (2016) W.M.Seif, M.Ismail, A.I.Refaie, L.H.Amer Optimum orientation versus orientation averaging description of cluster radioactivity RADIOACTIVITY 232,233U(α), (24Ne), (28Mg), 234U(α), (24Ne), (26Ne), (28Mg), 236Pu(α), (28Mg), 238Pu(α), (28Mg), (30Mg), (32Si); calculated T1/2. Comparison with available data.
doi: 10.1088/0954-3899/43/7/075101
2015EL02 Eur.Phys.J. A 51, 62 (2015) N.A.Elmahdy, A.S.Denikin, M.Ismail, A.Y.Ellithi 6Li breakup and suppression of complete fusion above the Coulomb barrier NUCLEAR REACTIONS 59Co(6Li, x), E(cm)=11-27 MeV;144Sm(6Li, x), E(cm)=19-40 MeV;209Bi(6Li, x), E(cm)=25-50 MeV; calculated fusion σ, breakup σ, partial contributions vs orbital momentum using CC and DWBA. Compared to published data.
doi: 10.1140/epja/i2015-15062-7
2015IS04 J.Phys.(London) G42, 075108 (2015) M.Ismail, A.Y.Ellithi, A.Adel, A.R.Abdulghany Effect of deformations on the binding energy of centrally depressed nuclei NUCLEAR STRUCTURE 208Pb, 238U, 252Cf, 280Cn, 285,286,287,288,289,298Fl, 306120, 320126, 339136, 500174; calculated binding energies, proton radii, quadrupole and hexadecapole deformations. Comparison with available data.
doi: 10.1088/0954-3899/42/7/075108
2015IS05 Phys.Rev. C 92, 014311 (2015) M.Ismail, W.M.Seif, A.Y.Ellithi, A.Abdurrahman Single universal curve for α decay derived from semi-microscopic calculations RADIOACTIVITY A=105-294, Z=52-118(α); deduced single universal curve for α decay from parametrization of available experimental α-decay half-lives and Q values for 496 nuclei, and semi-microscopic calculations based on realistic Michigan-three-Yukawa Reid nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.92.014311
2014IS01 Nucl.Phys. A922, 168 (2014) Examples of the failure of proximity approach when the nuclear surface is irregular or has concave regions NUCLEAR REACTIONS 48Ca(48Ca, X), E not given;150Nd(150Nd, X), E not given;226Ra(60Cr, X), E not given;244Pu(49Ca, X), E not given;226Ra(146Ce, X), E not given; calculated Coulomb radius, fusion barrier, potential energy surface vs deformation for different deformations and orienattions using DFM (double folding model).
doi: 10.1016/j.nuclphysa.2013.12.005
2014IS03 Phys.Rev. C 89, 034617 (2014) Effect of deformation parameters, Q value, and finite-range NN force on α-particle preformation probability RADIOACTIVITY 210,212,214,216,218,220,222,224,226Th, 222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 246,248,250,252,254,256Fm(α); calculated preformation probability Sα, α-decay half-lives, β2 and β4 deformation parameters. Double-folding nuclear and Coulomb potentials for deformed nuclei. Deformed density-dependent cluster model and CDM3Y1 NN interaction.
doi: 10.1103/PhysRevC.89.034617
2014IS07 Can.J.Phys. 92, 1411 (2014) M.Ismail, A.Y.Ellithi, M.M.Botros, A.F.Abdel Reheem Fusion barrier parameters for a spherically deformed pair of nuclei NUCLEAR REACTIONS 224Ra(48Ca, X)272Hs, 244Pu(48Ca, X)292Fl, E not given; calculated Coulomb barrier parameters, impact of deformations. The double folding model with effective density dependent M3Y-NN force, and the energy density functional method based on Skyrme force, comparison with available data.
doi: 10.1139/cjp-2013-0476
2014IS09 Phys.Rev. C 90, 064624 (2014) Investigation of possible correlation between α-particle preformation probability and energy levels for α emitters with 74 ≤ Z ≤ 83 RADIOACTIVITY 158,159,160,161,162,163,164,165,166,167W, 161,162,163,164,165,166,167,168,169,170,171,172,173,174,186Os, 166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182Pt, 171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188Hg, 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192Pb, 185,187,189,191,193,195,197Bi(α); calculated preformation probability of an α cluster, and α-decay half-lives. Realistic density-dependent CDM3Y1-Paris nucleon-nucleon (NN) interaction used to calculate the microscopic α-nucleus potential in the double-folding model. Prediction or confirmation of nuclear spins and parities in this mass region. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.064624
2013IS06 Nucl.Phys. A912, 18 (2013) Effect of energy level sequences and neutron-proton interaction on α-particle preformation probability RADIOACTIVITY 211,213Bi, 208,210,212,214,216Po, 209,211,213,215,217At, 210,212,214,216,218Rn, 211,213,215,217,219Fr, 212,214,216,218,220Ra, 213,215,217,219,211Ac, 214,216,218,220,222Th, 215,217,219,221,223Pa, 218,224U(α); calculated α preformation probability, T1/2 using realistic density-dependent NN interaction with finite-range exchange part. Compared with data.
doi: 10.1016/j.nuclphysa.2013.05.009
2013IS08 Can.J.Phys. 91, 401 (2013) M.Ismail, W.M.Seif, A.Y.Ellithi, A.S.Hashem (A = 10)-Accompanied spontaneous ternary fission of californium isotopes RADIOACTIVITY 238,240,242,244,246,248,250,252,254,256Cf(SF); calculated ternary fission Q-values. 10Be; deduced fragment mass distributions. Three-cluster model based on three different nuclear interactions, namely, the Yukawa-exponential, the folding model with Migdal force, and the proximity potentials.
doi: 10.1139/cjp-2012-0549
2013IS13 Phys.Rev. C 88, 054604 (2013) Prediction of nuclear spin based on the behavior of α-particle preformation probability RADIOACTIVITY 189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218Po, 193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222Rn, 202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,226Ra, 208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232Th, 222,223,224,225,226,227,228,229,230,231,232,233,234U, 228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,244Pu, 238,241,242,243,244,245,246,247,248Cm, 240,241,242,243,244,245,246,247,248,249,250,251,252,253,254Cf, 248,249,250,251,252,253,254,255,256,257Fm, 251,252,253,254,255,256,257No(α); calculated preformation probability Sα, half-lives using BDM3Y1-Paris NN interaction within the semiclassical Wentzel-Kramers-Brillouin approximation. 193,195At, 195,197,199Po, 197,199,201Fr, 209,211,213,223,225Th, 215,217Ac, 217,219Pa, 221,223Ra, 251,253No, 249,251Fm, 251,253Es, 253,255Md; predicted J, π or correlated spins of adjacent nuclei. Comparison with experimental data taken from NuDaT2.6.
doi: 10.1103/PhysRevC.88.054604
2013SI26 J.Phys.Soc.Jpn. 82, 114201 (2013) D.Singh, M.A.Ansari, R.Ali, N.P.M.Sathik, B.S.Tomar, M.Ismail Reaction Mechanism in 16O Ion Interaction with Light Nuclei 45Sc, 74Ge and Mass-Asymmetry Effect on Incomplete Fusion Dynamics NUCLEAR REACTIONS 45Sc(16O, 4np2α)48Cr, 74Ge(16O, 4npα)81Rb, 74Ge(16O, 5np2α)76Br, E<120 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with statistical model calculations.
doi: 10.7566/JPSJ.82.114201
2012AD01 Nucl.Phys. A876, 119 (2012) A.Adel, V.A.Rachkov, A.V.Karpov, A.S.Denikin, M.Ismail, W.M.Seif, A.Y.Ellithi Effect of neutron rearrangement on subbarrier fusion reactions NUCLEAR REACTIONS 7Li(54Cr, X), 9Li(52Cr, X), E(cm)=7-14 MeV;11Li(50Cr, X), E(cm)=5-14 MeV;16O(52Cr, X), 18O(50Cr, X), E(cm)=24-30 MeV;16O(116Sn, X), 18O(114Sn, X), E(cm)=45-63 MeV;32S(58Ni, X), (64Ni, X), E(cm)=52-74 MeV;40Ca(48Ca, X), E(cm)=46-58 MeV;40Ca(124Sn, X), E(cm)=106-130 MeV;48Ca(50Cr, X), 44Ca(54Cr, X), E(cm)=56-66 MeV;58Ni(58Ni, X), (64Ni, X), E(cm)=88-114 MeV; calculated fusion σ using empirical channel coupling with neutron transfer.
doi: 10.1016/j.nuclphysa.2012.01.004
2012IS05 Int.J.Mod.Phys. E21, 1250062 (2012) Shell corrections for heavy and superheavy nuclei NUCLEAR STRUCTURE Z=100-126; calculated total shell-plus-pairing energy corrections, single particle energy levels. Strutinsky method.
doi: 10.1142/S0218301312500620
2012IS06 Nucl.Phys. A888, 34 (2012) Comparative study of Coulomb barrier parameters for deformed nuclei using double-folding model and proximity approach NUCLEAR REACTIONS 150Nd(150Nd, X), 180Hf(86Kr, X), 238Pu(48Ar, X), E not given; calculated Coulomb barrier parameters vs deformation axis using double folding model with proximity approach.
doi: 10.1016/j.nuclphysa.2012.05.011
2012IS07 Phys.Rev. C 86, 014616 (2012) Correlation between α-particle preformation probability and the energy levels of parent nuclei RADIOACTIVITY 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230Th, 218,220,222,224,226,228,230,232,234,236U, 233,236Cm, 237Cf, 249Md, 253Lr, 257Db, 260,265,267Sg, 261,262Bh, 263,265Hs, 281Ds, 285Cn, 285Nh, 288,289Fl, 289Mc, 293,294Ts, 294Og(α); calculated preformation probability Sα, half lives using the realistic density-dependent BDM3Y1-Reid BDM3Y1-Paris nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.014616
2012IS08 Phys.Rev. C 86, 044317 (2012) M.Ismail, A.Y.Ellithi, M.M.Botros, A.Abdurrahman Penetration factor in deformed potentials: Application to α decay with deformed nuclei RADIOACTIVITY 210Pb, 212,214,216,218Po, 214,216,218,220,222Rn, 216,218,220,222,224,226Ra, 218,220,222,224,226,228,230,232Th, 220,222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256,258No, 256,258,260Rf, 260,266Sg, 264,266,270Hs, 270,280Ds, 284Cn, 286,288Fl, 290,292Lv, 294118(α); calculated half-lives using deformed density dependent cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044317
2011IS06 Nucl.Phys. A859, 1 (2011) Orientation dependent behavior of the Coulomb barrier parameters for deformed-deformed nuclei NUCLEAR REACTIONS 238Pu(48Ar, X), 238U, 248Cm(26Mg, X), 238U(22Ne, X), E not given; calculated Coulomb barrier height, radius vs quadrupole deformation at different orientations.
doi: 10.1016/j.nuclphysa.2011.04.005
2011IS10 Phys.Rev. C 84, 034610 (2011) Azimuthal angle dependence of the Coulomb barrier parameters for the interaction between two deformed nuclei NUCLEAR REACTIONS 28Si(28Si, X), E(cm)=30-65 MeV; 150Nd(150Nd, X), E(cm)=350-600 MeV; 238U(238U, X), E not given; 248Cm(238U, X), E not given; calculated azimuthal angle dependence of the Coulomb barrier parameters using the DFM and the corresponding values from the proximity method, fusion σ(E) for deformed nuclei. Double-folding model with the realistic M3Y nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.84.034610
2011IS11 Nucl.Phys. A872, 25 (2011) Prediction of accidental cancellation of different deformation components and optimum fusion orientations NUCLEAR REACTIONS 244Pu(48Ca, X), E not given; calculated orientations of colliding nuclei for different β2, β3, β4; deduced fusion barrier height, fusion radius using density dependent BDM3Y1-Paris NN interaction. Also considered β6, β8 deformations. Comparison with data.
doi: 10.1016/j.nuclphysa.2011.09.009
2011IS12 Int.J.Mod.Phys. E20, 2407 (2011) M.Ismail, M.M.Botros, A.A.Wheida Accuracy of the multipole expansion of density distribution in the presence of octupole deformation NUCLEAR STRUCTURE 40Ca, 208Pb; calculated multipole expansion, octupole deformation. Zero-range nucleon-nucleon (NN) interaction.
doi: 10.1142/S0218301311020423
2010IS01 Phys.Rev. C 81, 024602 (2010) M.Ismail, A.Y.Ellithi, M.M.Botros, A.Adel Systematics of α-decay half-lives around shell closures RADIOACTIVITY 178,180,184,186,190,194Pb(α); 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po(α); 238,240,242,244,246,248Cm(α);240,242,244,246,248,250,252,254Cf(α); 246,248,250,252,254,256Fm(α); 252,254,256No(α); 262,264,266,268,270,272Sg(α); 264,266,268,270,272,274,276Hs(α); 268,270,272,274,276,278Ds(α); 282,284,286,288,290,292,294,296,298,300,302,304Cn(α); 286,288,290,292,294,296,298,300,302,304,306Fl(α); 286,288,290,292,294,296,298,300,302,304,306,308Lv(α);290,292,294,296,298,300,302,304,306,308,310Og(α); 290,292,294,296,298,300,302,304,306,308,310120(α); calculated α-decay half-lives using the preformed α model with the M3Y Paris effective interaction for different values of pre-formation probabilities. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.024602
2010IS02 Phys.Rev. C 81, 034607 (2010) Simple interpretation of nuclear orientation for Coulomb barrier distributions derived from a realistic effective interaction NUCLEAR REACTIONS 244Pu(48Ca, X), E not given; calculated Coulomb barrier heights and radii of the interacting pair as function of quadrupole, octupole and hexadecapole deformations of the target nucleus. Double-folding procedure for the interaction of pair of spherical and deformed nuclei.
doi: 10.1103/PhysRevC.81.034607
2010IS05 Phys.Atomic Nuclei 73, 1660 (2010) M.Ismail, A.Y.Ellithi, M.M.Botros, A.Adel Binding energies of even-even superheavy nuclei in a semi-microscopic approach NUCLEAR STRUCTURE Z=98-120; calculated binding energies, quadrupole, hexadecapole deformations, half-density radii. Skyrme nucleon-nucleon interaction, Thomas-Fermi approach.
doi: 10.1134/S1063778810100042
2009IS03 Nucl.Phys. A828, 333 (2009) M.Ismail, W.M.Seif, M.M.Botros Effect of octupole and higher deformations on Coulomb barrier NUCLEAR REACTIONS 244Pu(48Ca, X)292114, E≈3-5 MeV/nucleon; calculated Coulomb barrier height/position using a double-folding model including effect of deformation.
doi: 10.1016/j.nuclphysa.2009.07.013
2008SI05 Chin.J.Phys.(Taiwan) 46, 27 (2008) D.Singh, M.Afzal Ansari, R.Ali, N.P.M.Sathik, M.Ismail A Study of Excitation Functions for Some Residues Produced in 16O+74Ge System Below 7 MeV/nucleon NUCLEAR REACTIONS 74Ge(16O, 4n), (16O, 2np), (16O, 3np), (16O, 4np), (16O, nα), (16O, 3nα), (16O, 2npα), (16O, 3npα), (16O, 3n2α), E=60.2-111.6 MeV; measured Eγ, Iγ, cross sections using stacked foil activation. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6092. 2007IS07 Phys.Rev. C 75, 064610 (2007) M.Ismail, A.Y.Ellithi, M.M.Botros, A.E.Mellik Azimuthal angle dependence of Coulomb and nuclear interactions between two deformed nuclei NUCLEAR REACTIONS 238U(238U, X), E not given; calculated azimuthal angle variation of the coulomb and nuclear heavy-ion potentials within the framework of the double folding model.
doi: 10.1103/PhysRevC.75.064610
2006IS05 Phys.Atomic Nuclei 69, 1463 (2006) M.Ismail, W.M.Seif, H.Abou-Shady, A.Bakry Study of Coulomb Interaction for Two Diffuse Spherical-Deformed Nuclei NUCLEAR REACTIONS 238U(16O, X), E not given; calculated Coulomb coupling form factors, finite diffuseness effects.
doi: 10.1134/S1063778806090055
2005IS03 Phys.Rev. C 71, 027601 (2005) M.Ismail, A.Y.Ellithi, H.Abou-Shady Effect of finite range of the NN force and NN cross section on reaction cross section for neutron rich nuclei NUCLEAR REACTIONS 9,11Li, 12C(12C, X), 9Li(238U, X), E ≈ 100-1600 MeV/nucleon; calculated reaction σ, effect of finite range in NN force.
doi: 10.1103/PhysRevC.71.027601
2005IS14 Phys.Rev. C 72, 064616 (2005) M.Ismail, W.M.Seif, M.M.Osman, H.El-Gebaly, N.M.Hassan Orientation dependence of the heavy-ion potential between two deformed nuclei NUCLEAR REACTIONS 238U(238U, X), E(cm)=640-840 MeV; calculated interaction potential, fusion σ, deformation and orientation dependence. Hamiltonian energy density approach.
doi: 10.1103/PhysRevC.72.064616
2004AF03 Int.J.Mod.Phys. E13, 585 (2004) M.Afzal Ansari, M.A.Abd.Alslam, N.P.Sathik, M.Ismail, M.H.Rashid Excitation functions of α-induced reactions in cobalt and pre-equilibrium effects NUCLEAR REACTIONS 59Co(α, 2n), (α, nα), (α, 2nα), E=17-50 MeV; 59Co(α, 2nα), (α, n2p), E=40-50 MeV; measured excitation functions; deduced pre-equilibrium effects. Stacked-foil activation.
doi: 10.1142/S0218301304002405
2004IS01 Phys.Rev. C 69, 014606 (2004) M.Ismail, M.M.Osman, H.El-Gebaly, F.Salah, W.M.Seif Effect of in-medium NN cross section and finite range force on the reaction cross section for a deformed target nucleus NUCLEAR REACTIONS 238U(12C, X), E=100, 400, 700 MeV/nucleon; calculated reaction σ, effect of in-medium NN interaction, orientation and deformation dependence.
doi: 10.1103/PhysRevC.69.014606
2004IS10 Acta Phys.Hung.N.S. 21, 27 (2004) M.Ismail, M.M.Osman, H.El-Gebaly, H.Abou-Shady Effect of β6 Deformation Parameter on Fusion Cross-Section and Barrier Distribution NUCLEAR REACTIONS 238U(16O, X), E(cm)=72-90 MeV; calculated fusion σ, barrier distribution, deformation and orientation effects. Microscopic potential, comparisons with data.
doi: 10.1556/APH.21.2004.1.3
2003IS04 Phys.Lett. B 563, 53 (2003) M.Ismail, W.M.Seif, H.El-Gebaly On the Coulomb interaction between spherical and deformed nuclei NUCLEAR REACTIONS 238U(16O, X), E not given; calculated Coulomb potential, deformation and orientation effects.
doi: 10.1016/S0370-2693(03)00600-2
2003IS11 Yad.Fiz. 66, 1654 (2003); Phys.Atomic Nuclei 66, 1607 (2003) M.Y.Ismail, A.Y.Ellithi, M.M.Osman, M.M.Botros The Deformation and Orientation Effect on Reaction Cross Section with Deformed Targets NUCLEAR REACTIONS 120Sn, 154Sm, 238U(12C, X), (16O, X), (28Si, X), (40Ca, X), (60Ni, X), (90Zr, X), (208Pb, X), E=30, 44, 77 MeV/nucleon; 17N(12C, X), E=0-900 MeV/nucleon; 238U(12C, X), E=40-100 MeV/nucleon; calculated reaction σ vs target deformation and orientation. Glauber-Sitenko theory, optical-limit approximation, comparisons with data.
doi: 10.1134/1.1611565
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
2002IS06 Phys.Rev. C66, 017601 (2002) M.Ismail, A.Y.Ellithi, F.Salah Accuracy of Multipole Expansion of Density Distribution in Calculating the Potential for Deformed Spherical Interacting Pair
doi: 10.1103/PhysRevC.66.017601
2002SA34 Phys.Rev. C66, 014602 (2002); Erratum Phys.Rev. C67, 059903 (2003) N.P.M.Sathik, M.Afzal Ansari, B.P.Singh, M.Ismail, M.H.Rashid Preequilibrium Emission in α Induced Reactions on Bromine and Thallium NUCLEAR REACTIONS 203Tl(α, n), 79Br, 203Tl(α, 2n), 203,205Tl(α, 3n), 81Br, 203,205Tl(α, 4n), E ≈ 20-50 MeV; measured production σ. Stacked-foil activation technique, comparison with model predictions.
doi: 10.1103/PhysRevC.66.014602
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
1999IS06 Pramana 52, 609 (1999) Complete and Incomplete Fusion Studies in 7Li and 16O Induced Reactions on 51V by Measurement of Excitation Functions and Recoil Ranges NUCLEAR REACTIONS 51V(7Li, X)51Cr/52Mn/54Mn/56Mn, E=40-50 MeV; 51V(16O, X)51Cr/52Mn/54Mn/56Co/57Co/58Co/56Ni/61Cu/62Zn/63Zn, E=60-90 MeV; measured production σ, recoil ranges; deduced complete, incomplete fusion reaction mechanisms. Activation technique. Comparison with statistical model.
doi: 10.1007/BF02829867
1999IS07 Phys.Rev. C60, 037603 (1999) Exchange Part of the Real α-Nucleus Potential NUCLEAR REACTIONS 16O, 40Ca(α, X), E=0, 20.7 MeV/nucleon; calculated interaction potential. Oscillator model wave functions.
doi: 10.1103/PhysRevC.60.037603
1999IS08 J.Phys.(London) G25, 2137 (1999) M.Ismail, A.Sh.Ghazal, H.Abu-Zahra On Improving the Exchange Heavy Ion Potential between Two Deformed Nuclei NUCLEAR REACTIONS 238U(238U, X), E not given; calculated exchange potential; deduced effect of finite-range NN force.
doi: 10.1088/0954-3899/25/10/311
1998IS02 Phys.Rev. C57, 1290 (1998) M.Ismail, R.P.Sharma, M.H.Rashid The 181Ta(7Li, 5n)183Os Reaction: Measurement and analysis of the excitation function and isomeric cross-section ratios NUCLEAR REACTIONS, ICPND 181Ta(7Li, 5n), E=30-50 MeV; measured Eγ, Iγ, total residual σ, isomer ratio. Statistical model calculations.
doi: 10.1103/PhysRevC.57.1290
1998IS08 Pramana 50, 173 (1998) Measurement and Analysis of the Excitation Function and Isomeric Cross Section Ratios for α-Induced Reaction on Ir, Au, Re and Ta Nuclei NUCLEAR REACTIONS, ICPND 191Ir(α, X)192Au/193Au/194Au, E=16-48 MeV; 193Ir(α, X)195Au/192Ir/194Au/193Au, E=20-48 MeV; 181Ta(α, X)183Re/184Re/184mRe, E=19-39 MeV; 185Re(α, X)184Re/184mRe, E=33-48 MeV; 197Au(α, X)200Tl/199Tl/198Tl/198mTl/197Tl/197mHg, E=15-52 MeV; measured production σ; deduced excitation functions, isomer production ratios. Stacked-foil activation technique.
doi: 10.1007/BF02847528
1998IS14 Pramana 51, 743 (1998) Near-Barrier Fusion Reactions Induced by α on 197Au, 193Ir, 191Ir, 185Re, 181Ta, 121Sb and 69Ga Nuclei NUCLEAR REACTIONS 197Au, 191,193Ir, 185Re, 181Ta, 121Sb, 69Ga(α, X), E(cm) ≈ 14-30 MeV; measured fusion excitation functions; deduced role of coupling to deformation, collective states. Stacked foil activation. Statistical model, coupled channels analysis.
doi: 10.1007/BF02832606
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
1997IS14 Pramana 49, 623 (1997) M.Ismail, R.P.Sharma, M.H.Rashid Measurement of Excitation Functions and Mean Projected Recoil Ranges of Nuclei in 12C-Induced Reactions on Vanadium NUCLEAR REACTIONS, ICPND 51V(12C, X)24Na/54Mn/56Co/57Co/58Co, E=34-83 MeV; measured production σ, recoil ranges. Stacked foil, thick-target thick-recoil-catcher techniques.
doi: 10.1007/BF02848336
1996IS02 Phys.Rev. C53, 2352 (1996) Real Part of the Heavy-Ion Optical Potential Derived from Relativistic Mean Field Theory NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=6.3-197.8 MeV/nucleon; calculated optical potentials real part. Relativistic mean field theory based energy density.
doi: 10.1103/PhysRevC.53.2352
1996IS03 Phys.Lett. 378B, 40 (1996) On the Accuracy of Calculating the Exchange Part of the Real Heavy Ion Potential NUCLEAR REACTIONS 16O(16O, 16O), 40Ca(40Ca, 40Ca), E ≤ 20.7 MeV/nucleon; calculated potential characteristics.
doi: 10.1016/0370-2693(96)00373-5
1996IS05 Phys.Rev. C54, 3308 (1996) Accuracy of Calculating the Exchange Part of the Real Alpha-Nucleus Potential NUCLEAR REACTIONS 16O(α, α), E=0-46.4 MeV/nucleon; calculated real potential; deduced density matrix expansion associated error in nucleon-nucleon force.
doi: 10.1103/PhysRevC.54.3308
1996IS08 Acta Phys.Pol. B27, 2217 (1996) Test of the Validity of the Density Matrix Expansion Method for Ion-Ion Collision Process NUCLEAR STRUCTURE 16O, 40Ca; calculated off-diagonal to diagonal density matrix ratio vs interparticle distance. Density matrix expansion based approximation. NUCLEAR REACTIONS 16O(16O, X), 40Ca(40Ca, X), E=0-46.6 MeV/nucleon; calculated ion-ion interaction potentials. Density matrix expansion based approximation.
1993IS01 Pramana 40, 227 (1993) Measurement of Excitation Functions and Mean Projected Recoil Ranges of Nuclei in α-Induced Reactions on F, Al, V, Co and Re Nuclei NUCLEAR REACTIONS, ICPND 19F(α, n), E < 40 MeV; 27Al(α, n2pα), 27Al, 59Co(α, 3n2pα), 27Al, 59Co, 185Re(α, 2nα), 51V(α, n), (α, 3np), 51V, 59Co(α, 3nα), 185Re, 59Co(α, 4n2p), (α, n2p), 59Co, 185Re(α, 3n2p), (α, nα), 185Re(α, 4n), (α, n2p), (α, 3np), 187Re, 59Co(α, 2n), 187Re(α, n), E ≤ 65 MeV; measured residuals production σ(E). Stacked foil technique. Model comparison.
doi: 10.1007/BF02900190
1991KH05 Nucl.Phys. A529, 363 (1991) D.T.Khoa, N.Ohtsuka, S.W.Huang, M.Ismail, A.Faessler, M.El-Shabshiry, J.Aichelin Photon Production in Heavy-Ion Collisions and Nuclear Equation of State NUCLEAR REACTIONS 12C(12C, X), 40Ca(40Ca, X), 93Nb(93Nb, X), E=84, 200 MeV/nucleon; calculated γ production σ. Quantum molecular dynamics model.
doi: 10.1016/0375-9474(91)90799-C
1990IS01 Phys.Rev. C41, 87 (1990) Measurement and Analysis of the Excitation Function for Alpha-Induced Reactions on Ga and Sb Isotopes NUCLEAR REACTIONS, ICPND 69Ga(α, n), E ≈ 7-30 MeV; 69Ga(α, 2n), E ≈ 18-50 MeV; 69Ga(α, 4n2p), E ≈ 35-65 MeV; 69Ga(α, 3np), E ≈ 40-65 MeV; 71Ga(α, n), E ≈ 8-28 MeV; 71Ga(α, 3n), E ≈ 25-65 MeV; 71Ga(α, 4n), E=35-65 MeV; 121Sb(α, n), E ≈ 10-34 MeV; 121Sb(α, 2n), E ≈ 14-44 MeV; 121Sb(α, 4n), E ≈ 36-60 MeV; 121Sb(α, 3np), E ≈ 36-60 MeV; 123Sb(α, n), E ≈ 10-30 MeV; 123Sb(α, 3n), E ≈ 25-60 MeV; 123Sb(α, 4n), E ≈ 36-60 MeV; 27Al(α, 3n4p), E ≈ 32-64 MeV; 27Al(α, 5n4p), E ≈ 38-64 MeV; measured residual production σ(E); deduced reaction mechanism. Stacked foil, activation technique.
doi: 10.1103/PhysRevC.41.87
1990OH05 J.Phys.(London) G16, L155 (1990) N.Ohtsuka, M.El-Shabshiry, M.Ismail, A.Faessler, J.Aichelin Does Photon Production in Heavy-Ion Collisions Depend on the Equation of State ( Question ) NUCLEAR REACTIONS 12C(12C, X), 40Ca(40Ca, X), E=84, 200 MeV/nucleon; calculated γ production σ. Quantum molecular dynamics method.
doi: 10.1088/0954-3899/16/8/009
1989EL01 J.Phys.(London) G15, L59 (1989) M.El-Shabshiry, A.Faessler, M.Ismail Effects of the Pauli Blocking and Surface Contribution to the Optical Potential on the Ion-Ion Reaction Cross Section NUCLEAR REACTIONS 12C, 16O(12C, X), E ≈ 10-100 MeV/nucleon; calculated reaction σ(E); deduced potential features. Eikonal approximation, Pauli blocking.
doi: 10.1088/0954-3899/15/4/003
1989FA04 Z.Phys. A333, 153 (1989) A.Faessler, M.Rashdan, M.Ismail, N.Ohtsuka, W.Wadia Nuclear Shapes and Interaction Potentials of Two Colliding 208Pb Nuclei at Finite Temperature NUCLEAR REACTIONS 208Pb(208Pb, X), E not given; calculated composite system free energy. Finite temperature, complex potential energy density.
1989IS01 Nucl.Phys. A496, 795 (1989) M.Ismail, M.Rashdan, A.Faessler, R.Linden, N.Ohtsuka, W.Wadia Relativistic Effects on the Optical Potential of Deformed U + U Nuclei NUCLEAR REACTIONS U(U, U), E=83.2 MeV/nucleon; calculated optical potential parameters. Relativistic approach, deformed nuclei.
doi: 10.1016/0375-9474(89)90125-5
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
1989IS03 J.Phys.(London) G15, 1291 (1989) M.Ismail, M.Osman, H.El-Gibaly, A.Faessler Proximity Analysis of the Optical Potentials between (Pb + U) and (U + U) Systems NUCLEAR REACTIONS U(Pb, Pb), (U, U), E not given; analyzed potentials; deduced proximity theorem validity.
doi: 10.1088/0954-3899/15/8/024
1989IS05 Pramana 32, 605 (1989) Hybird Model Analysis of the Excitation Function for Alpha Induced Reaction on 121Sb and 123Sb NUCLEAR REACTIONS, ICPND 121,123Sb(α, n), E=14.1-30.5 MeV; 123Sb(α, 3n), E=25.90-57.32 MeV; 123Sb(α, 4n), E=34.4-57.32 MeV; 121Sb(α, 2n), E=14.1-44.15 MeV; 121Sb(α, 4n), E=36.7-57.32 MeV; 121Sb(α, 3np), E=38.7-57.32 MeV; 27Al(α, 3n4p), E=28.59-57.32 MeV; 27Al(α, 5n4p), E=38.7-57.32 MeV; measured σ(E). Activation technique, stacked foils. Model analysis.
doi: 10.1007/BF02847385
1988IS01 Pramana 30, 193 (1988) Measurement and Analysis of Alpha-Induced Reactions on Ta, Ag and Co NUCLEAR REACTIONS, ICPND 181Ta(α, n), (α, 2n), (α, 3n), (α, 4n), 107Ag(α, 4n2p), 109Ag(α, 2n), 59Co(α, 5n4p), (α, 5n2p), (α, 4n2p), (α, 3n2p), (α, n2p), E=60 MeV; measured residual production σ(E). Hybrid model.
doi: 10.1007/BF02846693
1988RA22 Z.Phys. A330, 417 (1988) M.Rashdan, A.Faessler, N.Ohtsuka, R.Linden, W.Wadia, M.Ismail The Effect of Nuclear and Coulomb Interactions on the Nuclear Shapes of Two Colliding 208Pb Nuclei NUCLEAR REACTIONS 208Pb(208Pb, 208Pb), E not given; calculated nuclear shape changes; deduced nuclear, Coulomb interactions role.
1987FA08 Z.Phys. A326, 501 (1987) A.Faessler, M.Ismail, N.Ohtsuka, M.Rashdan, W.Wadia U + U Potential in the Sudden and Adiabatic Approximation NUCLEAR REACTIONS 238U(238U, 238U), E=5.2, 20.9 MeV/nucleon; calculated optical, Coulomb potentials. Sudden, adiabatic approximation.
1987RA13 Nucl.Phys. A468, 168 (1987) M.Rashdan, A.Faessler, M.Ismail, N.Ohtsuka The Temperature Dependence of the HI Optical Potential NUCLEAR STRUCTURE 40Ca, 208Pb; calculated free, binding energies per particle, density distribution vs temperature. Realistic effective nucleon-nucleon interaction. NUCLEAR REACTIONS 40Ca(40Ca, X), 208Pb(208Pb, X), E not given; calculated optical potentials vs temperature. Realistic effective nucleon-nucleon interaction.
doi: 10.1016/0375-9474(87)90322-8
1986IS03 Z.Phys. A323, 399 (1986) M.Ismail, M.Rashdan, A.Faessler, M.Trefz, H.M.M.Mansour The Effect of Deformation on the Nucleus-Nucleus Optical Model Potential and how It Produces Pockets NUCLEAR REACTIONS 238U, 208Pb(238U, 238U), E=6, 11.8, 20.9 MeV/nucleon; calculated optical model potentials, parameters vs separation distance; deduced deformation role, pocket production.
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
1985IS01 J.Phys.(London) G11, 763 (1985) M.Ismail, A.Faessler, M.Trefz, W.H.Dickhoff The Volume and Surface Contributions to the Ion-Ion Optical Potential NUCLEAR REACTIONS 12C, 40,48Ca, 16O(12C, 12C), 16O, 40,48Ca(16O, 16O), 40,48Ca(40Ca, 40Ca), 48Ca(48Ca, 48Ca), E=5.18-82.94 MeV/nucleon; calculated ion-ion potential volume, surface contributions, parameter energy dependence, reaction σ(E). Bethe-Goldstone equation, Reid soft core potential.
doi: 10.1088/0305-4616/11/6/013
1984FA02 J.Phys.(London) G10, L35 (1984) A.Faessler, W.Wadia, M.Rashdan, M.Ismail Microscopic Calculation of the Interaction Potential between Two 12C Nuclei NUCLEAR REACTIONS 12C(12C, 12C), E not given; calculated interaction potential. Alpha particle model.
doi: 10.1088/0305-4616/10/2/002
1984FA05 Z.Phys. A316, 195 (1984) The Volume Contribution of the Ion-Ion Optical Potential from Realistic Complex Nucleon-Nucleon Interaction NUCLEAR REACTIONS 40,48Ca, 56Ni, 90Zr, 208Pb(40Ca, 40Ca), (16O, 16O), 16O(16O, 16O), 48Ca, 56Ni, 90Zr, 208Pb(48Ca, 48Ca), 56Ni, 90Zr, 208Pb(56Ni, 56Ni), E not given; calculated nucleon-nucleon potential parameters. Double folding procedure.
doi: 10.1007/BF01412262
1984OS06 J.Phys.(London) G10, 1399 (1984) M.M.Osman, M.Ismail, H.M.Hasan, W.Wadia, M.Rashdan A Test of a Simple Approximation for Treating the Antisymmetrisation Effect in Ion-Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=50-1000 MeV; calculated interaction potential real part vs inter-ion distance. Density matrix expansion, different effective nucleon-nucleon forces.
doi: 10.1088/0305-4616/10/10/011
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