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NSR database version of April 27, 2024.

Search: Author = A.Y.Ellithi

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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 ^{295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340,341,342,343,344,345,346,347,348,349,350}120, ^{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}121, ^{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}122, ³⁴⁸122, ³⁵⁰122, ^{310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}123, ^{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}124, ^{342,344,346,348,350}124, ^{316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}125, ^{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}126, ^{324,326,328,330,332,334,336,338,340,342,344,346,348,350}126(α); calculated T_1/2.

doi: 10.1088/1402-4896/ac758c
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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, ^{221,222,223,224}Ra, 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 T_1/2. Comparison with available data.

doi: 10.1140/epja/s10050-022-00882-9
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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
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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 ^{106,107,108,109}Te, ¹¹³I, ^112,113Xe, ¹¹⁴Ba, ¹⁴⁴Nd, ¹⁴⁵Pm, ^146,147,148Sm, ^147,148Eu, ^{148,149,150,151,152}Gd, ^{150,151,152,153,154}Dy, ^152,154Ho, ^{152,153,154,155}Er, ¹⁵³Tm, ^155,156Tm, ^{154,155,156,157,158}Yb, ^{156,157,158,159,160}Hf, 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, ^{182,183,184,185,186}Hg, ¹⁸⁸Hg, ^177,179Tl, ^{186,188,190,192,194}Pb, ²¹⁰Pb, ^190,192,194Po, ^{195,196,197,198,199,200,201,202}Po, ^{204,205,206,207}Po, ²¹⁰Po, ²¹²Po, ^{213,214,215,216}Po, ²¹⁸Po, ^{196,197,198,199,200,201,202,203,204,205,206,207,208,209}At, ^{211,212,213,214,215}At, ¹⁹⁵Rn, ¹⁹⁸Rn, ²⁰¹Rn, ^203,204Rn, ^{206,207,208,209,210}Rn, ²¹²Rn, ^{214,215,216,217,218}Rn, ^220,222Rn, ²⁰¹Fr, ^{203,204,205,206,207,208,209,210,211}Fr, ²¹³Fr, ^{215,216,217,218,219}Fr, ^205,206,207Ra, ^{209,210,211,212}Ra, ²¹⁴Ra, ^216,217,218Ra, ^{220,222,224,226}Ra, ²⁰⁶Ac, ^208,209Ac, ^{211,213,215,217}Ac, ^218,219Ac, ^221,222Ac, ²²⁷Ac, ²¹³Th, ^{216,218,220,222,224,226,228,230,232}Th, ^217,219Pa, ^221,223Pa, ^226,227Pa, ²³¹Pa, ^226,228U, ²²⁹U, ^230,232U, ^233,234U, ^236,238U, ^{232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ²⁴⁰Cf, ^245,246Cf, ^{248,250,252,254}Cf, ^251,253Es(α); calculated T_1/2. Comparison with experimental and UDL data.

doi: 10.1088/1361-6471/ab7291
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2017EL03      Appl.Radiat.Isot. 128, 318 (2017)

A.El Abd, G.Taha, A.Y.Ellithi

A method for measuring macroscopic cross-sections for thermal neutrons

doi: 10.1016/j.apradiso.2017.07.036
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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 ^{158,159,160,161,162,163,164,165,166,167}W, ^{161,162,163,164,165,166,167,168,169,170,171,172,173,174}Os, ¹⁸⁶Os, ^{166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182}Pt, ^{172,173,174,175,176,177,178,179,180}Hg, ^{182,183,184,185,186}Hg, ¹⁸⁸Hg, ^{178,180,182,184,186,188,190}Pb, ^191,192Pb(α); calculated T_1/2, preformation probability and assault frequency. Comparison with available data.

doi: 10.1142/S0218301317500264
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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
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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 ^{186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218}Po(α); calculated T_1/2 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. T_1/2 compared to data.

doi: 10.1016/j.nuclphysa.2015.12.008
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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
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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 T_1/2. Comparison with experimental data.

doi: 10.1142/S0218301316500695
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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
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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
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2015HA20      Int.J.Mod.Phys. E24, 1550062 (2015)

M.A.M.Hassan, M.S.M.Nour El-Din, A.Ellithi, E.Ismail, H.Hosny

The effect of halo nuclear density on reaction cross-section for light ion collision

NUCLEAR STRUCTURE ¹¹Be, ^15,17,19C, ²²N, ²³O, ^24,26F, ²⁹Ne, ⁶He, ¹¹Li, ¹⁴Be, ^17,19B; calculated rms radii.

NUCLEAR REACTIONS ¹²C(¹¹Be, X), (¹⁵C, X), (¹⁷C, X), (¹⁹C, X), (²²N, X), (²³O, X), (²⁴F, X), (²⁶F, X), (⁶He, X), (¹¹Li, X), (¹⁴Be, X), (¹⁷B, X), (¹⁹B, X), E=740-1005 MeV/nucleon; calculated σ. Optical limit approximation.

doi: 10.1142/S0218301315500627
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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, ^{285,286,287,288,289,298}Fl, 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
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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
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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
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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 ^{238,240,242,244,246,248,250,252,254,256}Cf(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
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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
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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, ^{212,214,216,218}Po, ^{214,216,218,220,222}Rn, ^{216,218,220,222,224,226}Ra, ^{218,220,222,224,226,228,230,232}Th, ^{220,222,224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^{252,254,256,258}No, ^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
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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 ^{178,180,184,186,190,194}Pb(α); ^{188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po(α); ^{238,240,242,244,246,248}Cm(α);^{240,242,244,246,248,250,252,254}Cf(α); ^{246,248,250,252,254,256}Fm(α); ^252,254,256No(α); ^{262,264,266,268,270,272}Sg(α); ^{264,266,268,270,272,274,276}Hs(α); ^{268,270,272,274,276,278}Ds(α); ^{282,284,286,288,290,292,294,296,298,300,302,304}Cn(α); ^{286,288,290,292,294,296,298,300,302,304,306}Fl(α); ^{286,288,290,292,294,296,298,300,302,304,306,308}Lv(α);^{290,292,294,296,298,300,302,304,306,308,310}Og(α); ^{290,292,294,296,298,300,302,304,306,308,310}120(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
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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
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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
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2005EL03      Eur.Phys.J. A 24, 137 (2005)

M.M.H.El-Gogary, A.Y.Ellithi, M.Kh.Hegab, A.A.Mohamed

Elastic scattering via quark structure of nucleons

NUCLEAR REACTIONS ¹H(p, p), E(cm)=23.5, 30.7, 44.7, 52.8 GeV; ⁴H(p, p), E(cm)=88, 89 GeV; analyzed σ(θ); deduced quark-quark scattering effects. Glauber multiple-scattering theory.

doi: 10.1140/epja/i2004-10127-4
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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
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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
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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
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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
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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.

Note: The following list of authors and aliases matches the search parameter A.Y.Ellithi: , A.Y.ELLITHI