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NSR database version of May 1, 2024.

Search: Author = M.I.Jaghoub

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2024SA16      Phys.Rev. C 109, 034606 (2024)

A.Saleh, M.I.Jaghoub

Modeling α-nucleus elastic scattering using a velocity-dependent optical potential

doi: 10.1103/PhysRevC.109.034606
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2023MA08      Phys.Rev. C 107, 024616 (2023)

S.B.Masadeh, D.A.Abdallah, M.I.Jaghoub

Analysis of nucleon-nucleus scattering data using a density-dependent semi-microscopic optical model with channel coupling

NUCLEAR REACTIONS ⁷Li(n, n'), E=10-24 MeV; ¹²C(n, n'), E=10-95 MeV; ¹⁶O(n, n'), E=9-26 MeV; ⁴⁰Ca(n, n'), E=11-20 MeV; ⁵⁴Fe(n, n'), E=8.5-26 MeV; ⁵⁸Ni(n, n'), E=9.9-24 MeV; ¹²⁰Sn(n, n'), E=9.9-16.9 MeV; ²⁰⁸Pb(n, n'), E=9.9-26 MeV; ¹²C(p, p'), E=14-40 MeV;¹⁶O(p, p'), E=13-40 MeV;⁴⁰Ca(p, p'), E=14.6-55.0 MeV;⁵⁴Fe(p, p'), E=11-35 MeV;, ⁵⁸Ni(p, p'), E=10.9-39.8 MeV;¹²⁰Sn(p, p'), E=20.4-36.2 MeV;²⁰⁸Pb(p, p), E=30.8-61.2 MeV; calculated elastic and inelastic σ(θ), total σ, analyzing power. Density-dependent semi-microscopic optical model with channel-coupling and density-dependent BDM3Y1-Paris bare (NN) interaction. Comparison to experimental data and other theoretical calculations.

doi: 10.1103/PhysRevC.107.024616
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2022AL09      Nucl.Phys. A1024, 122461 (2022)

A.Albelleh, M.I.Jaghoub, W.S.Al-Rayashi

Comparing the effects of nonlocal sources on the neutron-nucleus elastic scattering process

NUCLEAR REACTIONS ⁶Li, ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁴Fe, ¹¹⁸Sn, ²⁰⁸Pb(n, n), (n, n'), E<25.7 MeV; analyzed available data; deduced Perey damping factors, the wave function of a nonlocal potential is reduced or enhanced in the nuclear interior where the potential acts.

doi: 10.1016/j.nuclphysa.2022.122461
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2022UT01      Can.J.Phys. 100, 309 (2022)

M.Utoom, M.I.Jaghoub, T.Aqel

Nonlocal optical model for deuteron elastic scattering

NUCLEAR REACTIONS ²H(¹⁰Be, d), ¹²C, ^16,18O, ²⁸Si, ⁵⁴Fe, ^58,60Ni, ⁹⁰Zr, ¹²⁰Sn(d, d), E=10-70 MeV; analyzed available data; deduced two sets of global nonlocal parameters, one for light 1p-shell nuclei and the other for intermediate and heavy ones using the nonlocal model of Perey and Buck, which explicitly includes a Gaussian nonlocality.

doi: 10.1139/cjp-2021-0380
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2020AQ01      Eur.Phys.J. A 56, 216 (2020)

T.Aqel, M.I.Jaghoub

A nonlocal optical potential with a Gaussian nonlocality for proton elastic scattering off light 1p-shell nuclei

NUCLEAR REACTIONS ⁹Be, ¹²C, ^16,18O(p, p), E=13-26.2 MeV; analyzed available data; calculated σ(θ).

doi: 10.1140/epja/s10050-020-00226-5
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2019AQ01      Nucl.Phys. A989, 145 (2019)

T.Aqel, M.I.Jaghoub

A nonlocal optical model for neutron scattering from light 1p-shell nuclei

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁶O, x), E=9-65 MeV;⁶Li(n, n), E=9-14 MeV;⁹Be(n, n), E=9-22 MeV;¹²C(n, n), E=9.6-35 MeV; ¹³C(n, n), E=9-16 MeV;¹⁶O(n, n), E=10.7-24 MeV/nucleon;¹⁸O(n, n), E=8.5-24 MeV; calculated elastic scattering σ(θ) MeV using nonlocal OMP; deduced potential parameters (dependent on target and energy), constant set of nonlocal parameters using fitting to the data.

doi: 10.1016/j.nuclphysa.2019.06.005
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2019MA49      Phys.Rev. C 100, 014603 (2019)

S.B.Masadeh, M.I.Jaghoub

Semimicroscopic optical model with coupled-channel analysis for neutron scattering off nuclei with mass numbers 12 ≤ A ≤ 208

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁵⁴Fe, ⁵⁸Ni, ¹²⁰Sn, ²⁰⁸Pb(n, n), (n, n'), (n, X), E=9-28.2 MeV; analyzed experimental data for exclusive differential σ(θ, E), analyzing powers A_y(θ, E), and total reaction σ(E) using semimicroscopic optical model, based on M3Y-Paris bare nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.100.014603
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2018AL17      Eur.Phys.J. A 54, 62 (2018)

S.M.Al-Rawashdeh, M.I.Jaghoub

An optical potential for the statically deformed actinide nuclei derived from a global spherical potential

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^227,232Th, ^233,238U, ^239,240,242Pu, ²⁴⁴Cm, ²⁵⁰Cf; calculated quadrupole and hexadecapole deformation, radius correction.

NUCLEAR REACTIONS ²³²Th, ²³⁸U, ²³⁹Pu(n, x), E=0.005-200 MeV;²⁴⁴Cm(n, x), E=0.001-4 MeV; calculated total σ using CC and using global KD potential; compared with EXFOR data. ¹⁵⁰Nd(n, n), E=1.0, 1.2, 1.4, 1.8, 2.0 MeV;²³²Th(n, n), E=1.0, 1.5, 1.8, 2.2, 2.6, 3.0, 3.4, 3.5, 5.5, 7.5, 10.0 MeV;²³³U(n, n), E=2.3, 5.0, 6.0, 7.0, 8.0, 9.0 MeV;²³⁸U(n, n), (n, n'), E=1.5, 1.9, 2.5, 3.0, 3.4, 5.0, 7.0, 10.0, 14.0 MeV;²⁴²Pu(n, n), (n, n'), E=1.0, 1.5, 2.0, 2.5 MeV;²⁵⁰Cf(n, n), E=1.6, 2.7, 3.5, 5.0, 7.0 MeV; calculated σ(θ) using CC; compared with ENDF data. ²³²Th(n, n), (n, n'), E=0.70, 1.50, 2.50, 3.40 MeV; calculated σ(θ) using CC and using Fitted CC model; compared with data.

doi: 10.1140/epja/i2018-12497-2
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2018JA14      Phys.Rev. C 98, 024609 (2018)

M.I.Jaghoub, A.E.Lovell, F.M.Nunes

Exploration of the energy dependence of proton nonlocal optical potentials

NUCLEAR REACTIONS ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb(p, p), E=10-45 MeV; analyzed σ(θ, E); deduced best fit for angular distributions over the whole mass range using both the energy dependent and energy independent Tian, Pang, and Ma nonlocal interactions. ³²S, ⁶⁸Zn, ⁸⁹Y, ¹⁰⁰Mo, ¹¹⁰Pd(p, p), E=10-65 MeV; calculated σ(θ, E) using global interaction parametrization. Comparison with experimental values.

doi: 10.1103/PhysRevC.98.024609
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2016AL14      Phys.Rev. C 93, 064311 (2016)

W.S.Al-Rayashi, M.I.Jaghoub

Effect of coupled channels on the energy dependence of phenomenological optical potential parameters

NUCLEAR REACTIONS ⁶Li, ¹²C, ¹⁶O, ⁵⁴Fe, ¹²⁰Sn, ²⁰⁸Pb(n, n), (n, n'), E=9.94-28 MeV; ¹²C²⁴Mg(p, p), (p, p'), E=11.6-69.5 MeV; ²⁴Mg(polarized p, p), E=17.8 MeV; ⁵⁴Fe(polarized n, n), E=9.94, 13.92, 16.93 MeV; analyzed σ(θ) and A_y(θ) data by variations of the phenomenological optical potential parameters with incident energy in the coupled channel method using the FRESCO and SFRESCO computer codes.

doi: 10.1103/PhysRevC.93.064311
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2015GH04      Phys.Rev. C 91, 064308 (2015)

I.N.Ghabar, M.I.Jaghoub

Velocity-dependent optical potential for neutron elastic scattering from 1p-shell nuclei

NUCLEAR REACTIONS ¹²C(n, n), E=9.6, 11.0, 12.0, 12.8, 14.0, 15.0, 17.0, 19.0, 20.0, 22.0, 30.0, 50.0, 80.0 MeV; ¹⁶O(n, n), E=12.0, 14.0, 17.0, 20.0, 22.0, 25.0, 27.0, 29.0, 30.0, 35.0, 50.0, 60.0, 70.0, 80.0, 90.0 MeV; analyzed σ(θ, E), total σ(E), A_y(θ, E) analyzing power data using a velocity-dependent optical potential that introduces real surface terms, and conventional optical potential; deduced potential parameters. Comparison with other models, and with experimental data.

doi: 10.1103/PhysRevC.91.064308
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2013ZU04      Nucl.Phys. A916, 183 (2013)

R.A.Zureikat, M.I.Jaghoub

Surface and volume term nonlocalities in the proton-nucleus elastic scattering process

NUCLEAR REACTIONS ¹²C(p, p), E=14.0, 17.8, 22.0, 30.4, 39.6 MeV;¹⁶O(p, p), E=10.5, 12.9, 24.5 MeV;⁴⁰Ca(p, p), E=12.4, 15.6, 20.6, 28.6, 30.3, 35.8, 28.6 MeV;⁵⁸Ni(p, p), E=16.0, 18.6, 30.3, 29.6 MeV; calculated σ(θ), σ, analyzing power, rms radii using optical potential with added new surface term and a gradient term for low and additional volume term for higher energies; deduced potential parameters. Compared with data.

doi: 10.1016/j.nuclphysa.2013.08.007
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2012JA03      Nucl.Phys. A877, 59 (2012)

M.I.Jaghoub, G.H.Rawitscher

Evidence of nonlocality due to a gradient term in the optical model

NUCLEAR REACTIONS ¹²C(n, n), E=12, 14, 16, 18, 20 MeV; calculated σ(θ) using optical model; deduced parameters, nonlocality. Comparison with data.

doi: 10.1016/j.nuclphysa.2011.12.004
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2012JA06      Phys.Rev. C 85, 024606 (2012)

M.I.Jaghoub

Surface term optical model nonlocality in the NA elastic scattering process

NUCLEAR REACTIONS ⁴⁰Ca(n, n), E=11, 14, 17, 20 MeV; analyzed σ(θ), and analyzing powers; deduced velocity-dependent optical potential parameters. Nonlocality in the optical model.

doi: 10.1103/PhysRevC.85.024606
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2011JA09      Phys.Rev. C 84, 034618 (2011)

M.I.Jaghoub, M.F.Hassan, G.H.Rawitscher

Novel source of nonlocality in the optical model

NUCLEAR REACTIONS ¹²C(n, n), E=12-20 MeV; analyzed σ(E, θ) data and analyzing powers using optical potential model with velocity dependent terms. Comparison with standard optical model calculations.

doi: 10.1103/PhysRevC.84.034618
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2006JA02      Eur.Phys.J. A 27, 99 (2006)

M.I.Jaghoub

Perturbation theory for isotropic velocity-dependent potentials: Bound-states case

doi: 10.1140/epja/i2005-10192-1
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2006JA14      Eur.Phys.J. A 28, 253 (2006)

M.I.Jaghoub

Effect of ordering ambiguity in constructing the Schrodinger equation on perturbation theory

doi: 10.1140/epja/i2006-10047-3
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2002JA08      Eur.Phys.J. A 13, 349 (2002)

M.I.Jaghoub

Bound and Scattering Wave Functions for a Velocity-Dependent Kisslinger Potential for l > 0

doi: 10.1007/s10050-002-8763-8
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2002JA21      Eur.Phys.J. A 15, 443 (2002)

M.I.Jaghoub

Perturbation theory for velocity-dependent potentials

doi: 10.1140/epja/i2002-10055-3
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