NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.F.Arellano Found 31 matches. 2022AR09 Eur.Phys.J. A 58, 119 (2022) On the separability of microscopic optical model potentials and emerging bell-shape Perey-Buck nonlocality
doi: 10.1140/epja/s10050-022-00777-9
2021AR04 Eur.Phys.J. A 57, 27 (2021) Ultraviolet suppression and nonlocality in optical model potentials for nucleon-nucleus scattering NUCLEAR REACTIONS 4He, 16O, 40Ca, 90Zr, 208Pb(p, p), E<1 GeV; analyzed available data; deduced σ, momenta using microscopic optical model potentials were constructed in momentum space using Bruckner-Hartree-Fock g matrices based on AV18 and N3LO chiral potentials.
doi: 10.1140/epja/s10050-020-00328-0
2021BL03 Eur.Phys.J. A 57, 13 (2021) G.Blanchon, M.Dupuis, H.F.Arellano, R.N.Bernard, B.Morillon, P.Romain Diving into Raynal's DWBA code
doi: 10.1140/epja/s10050-020-00331-5
2021NA24 Eur.Phys.J. A 57, 279 (2021) A.Nasri, M.Dupuis, G.Blanchon, H.F.Arellano, P.Tamagno Following J. Raynal's DWBA and ECIS codes: coupled channels with microscopic non-local potential
doi: 10.1140/epja/s10050-021-00585-7
2018AR07 Phys.Rev. C 98, 054616 (2018) Irreducible nonlocality of optical model potentials based on realistic NN interactions NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p)E=30-800 MeV; calculated real and imaginary s-wave central optical potential in momentum space and coordinate space, nonlocal behaviour of the s-wave, differential σ(θ), Ay(θ), reaction σ(E), and volume integral per nucleon using AV18 and N3LO interactions; deduced nonlocal structure of optical model potentials based on microscopic approaches. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.054616
2017BL05 Eur.Phys.J. A 53, 88 (2017) G.Blanchon, M.Dupuis, R.N.Bernard, H.F.Arellano Asymmetry dependence of Gogny-based optical potential NUCLEAR REACTIONS 40,48Ca(n, n'), (p, p'), E=0-36 MeV; calculated σ(θ), analyzing power, inelastic σ using potentials generated by NSM (Nuclear Structure Method) with Gogny effective interaction. 40,48Ca(p, p), E=0-36 MeV; calculated σ(θ) using Perey-Buck equivalent potential and NSM.
doi: 10.1140/epja/i2017-12268-7
2016AR11 Eur.Phys.J. A 52, 299 (2016) H.F.Arellano, F.Isaule, A.Rios Di-nucleon structures in homogeneous nuclear matter based on two- and three-nucleon interactions
doi: 10.1140/epja/i2016-16299-2
2016IS09 Phys.Rev. C 94, 034004 (2016) F.Isaule, H.F.Arellano, A.Rios Di-neutrons in neutron matter within a Brueckner-Hartree-Fock approach NUCLEAR STRUCTURE 2n; calculated self-consistent single-particle potentials, effective-to-bare-mass ratio, binding energy, radial probability density, mean radius for di-neutron in pure neutron matter. Brueckner-Hartree-Fock (BHF) approach at zero temperature, with Argonne V18, Paris bare interactions, and chiral two- and three-nucleon forces N3LO2N2NF, and N3LO2N+N2LO3N3NF; deduced that di-neutrons are loosely bound, by less than 700 keV.
doi: 10.1103/PhysRevC.94.034004
2015AR04 Eur.Phys.J. A 51, 7 (2015) Low-density homogeneous symmetric nuclear matter: Disclosing dinucleons in coexisting phases
doi: 10.1140/epja/i2015-15007-2
2015BL01 Phys.Rev. C 91, 014612 (2015) G.Blanchon, M.Dupuis, H.F.Arellano, N.Vinh Mau Microscopic positive-energy potential based on the Gogny interaction NUCLEAR REACTIONS 40Ca(p, p), E=9.86, 10.37, 13.49, 14.51, 15.97, 18.57, 19.57, 21, 23.5, 25, 26.3, 27.5, 30.3, 40 MeV; 40Ca(n, n), E=2.06, 3.29, 5.3, 5.88, 6.5, 7.91, 9.91, 13.9, 16.9, 19, 21.7, 25.5, 30.3, 40 MeV; 40Ca(polarized p, p), E=14.51, 15.97, 18.57, 40 MeV; 40Ca(polarized n, n), E=9.91, 11, 13.9, 16.9 MeV; analyzed differential σ(E, θ), integral σ(E), and analyzing power Ay(θ, E). Calculation based on Greens function formalism in the random-phase approximation with the finite-range Gogny effective interaction, and including effects of intermediate single-particle resonances.
doi: 10.1103/PhysRevC.91.014612
2015BL08 Eur.Phys.J. A 51, 165 (2015) G.Blanchon, M.Dupuis, H.F.Arellano Prospective study on microscopic potential with Gogny interaction
doi: 10.1140/epja/i2015-15165-1
2011AR02 Phys.Rev. C 83, 044306 (2011) Toward an actual account for the angular dependence of the Brueckner-Bethe-Goldstone propagator in nuclear matter
doi: 10.1103/PhysRevC.83.044306
2011AR13 Phys.Rev. C 84, 034606 (2011) 7D-folding integral in a density-dependent microscopic optical model potential for nucleon-nucleus scattering NUCLEAR REACTIONS 16O, 90Zr(polarized p, p), E=30-65; calculated σ(θ), analyzing powers. Density-dependent microscopic optical potential model with seven dimension folding integral. Comparison with experimental data, and with other models.
doi: 10.1103/PhysRevC.84.034606
2008AG12 Phys.Rev. C 78, 014608 (2008) Surface-peaked medium effects in the interaction of nucleons with finite nuclei NUCLEAR REACTIONS 16O, 90Zr(p, p), E=30-100 MeV; calculated σ(θ), analyzing powers. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.014608
2007AR19 Phys.Rev. C 76, 014613 (2007) Functional medium dependence of the nonrelativistic optical model potential
doi: 10.1103/PhysRevC.76.014613
2007AR20 Phys.Rev. C 76, 014616 (2007) In-medium full-folding model approach to quasielastic (p, n) charge-exchange reactions NUCLEAR REACTIONS 14C, 48Ca, 90Zr(p, n), E=120, 135 MeV; calculated σ and angular distributions using a coupled-channel extension of the full-folding optical model approach.
doi: 10.1103/PhysRevC.76.014616
2007AR25 Phys.Rev. C 76, 034602 (2007) Reaction cross sections for proton scattering from stable and unstable nuclei based on a microscopic approach NUCLEAR REACTIONS 12C, 16O, 40Ca, 58,60Ni, 90Zr, 208Pb(p, X), (n, X), E 10-1000 MeV; calculated total reaction cross sections using a non-relativistic microscopic approach. Compared results to available data.
doi: 10.1103/PhysRevC.76.034602
2005AR16 Nucl.Phys. A755, 527c (2005) Nuclear halo structure from quasielastic charge-exchange reactions NUCLEAR REACTIONS 48Ca(p, n), E=160 MeV; calculated σ(θ), nuclear density dependence.
doi: 10.1016/j.nuclphysa.2005.03.069
2005AR20 Phys.Rev. C 72, 025203 (2005) Microscopic analysis of K+-nucleus elastic scattering based on K+-nucleon phase shifts NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, K+), E at 400-1000 MeV/c; analyzed kaon-nucleon phase shifts; calculated σ(θ). Microscopic optical model approach, comparison with data.
doi: 10.1103/PhysRevC.72.025203
2002AR14 Phys.Rev. C66, 024602 (2002) Extension of the full-folding optical model for nucleon-nucleus scattering with applications up to 1.5 GeV NUCLEAR REACTIONS 16O, 40Ca, 90Zr, 208Pb(n, n), (p, p), E=100-1500 MeV; calculated total σ. 40Ca, 208Pb(p, p), E=300-1040 MeV; calculated σ(θ), analyzing power vs momentum transfer. Relativistic full-folding optical model approach, comparisons with data.
doi: 10.1103/PhysRevC.66.024602
2000NA02 Phys.Rev. C61, 024001 (2000) K.Nakayama, H.F.Arellano, J.W.Durso, J.Speth η' Meson Production in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, pX), E ≈ threshold; calculated pion, η-, η'-meson production σ; deduced contributions. Relativistic meson exchange model. Comparisons with data.
doi: 10.1103/PhysRevC.61.024001
1996AR13 Phys.Rev. C54, 2570 (1996) H.F.Arellano, F.A.Brieva, M.Sander, H.V.von Geramb Sensitivity of Nucleon-Nucleus Scattering to the Off-Shell Behavior of On-Shell Equivalent NN Potentials NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=40-500 MeV; 208Pb(polarized p, p), (p, p), E=400 MeV; analyzed σ(θ), analyzing power vs θ; deduced sensitivity to off-shell behavior of on-shell equivalent. NN-potentials.
doi: 10.1103/PhysRevC.54.2570
1995AR13 Phys.Rev. C52, 301 (1995) H.F.Arellano, F.A.Brieva, W.G.Love In-Medium Full-Folding Optical Model for Nucleon-Nucleus Elastic Scattering NUCLEAR REACTIONS 208Pb, 40Ca(polarized p, p), E=30.3-400 MeV; analyzed σ(θ), analyzing power, spin-rotation function vs θ. 40Ca, 90Zr, 208Pb(n, n), E=4-500 MeV; calculated σ(E). In-medium, full-folding optical model.
doi: 10.1103/PhysRevC.52.301
1994AR17 Phys.Rev. C50, 2480 (1994) H.F.Arellano, F.A.Brieva, W.G.Love Deuteron Effects in Nucleon-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=160-400 MeV; 208Pb(polarized p, p), E=98-400 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced medium effects, higher order corrections role. Full folding model.
doi: 10.1103/PhysRevC.50.2480
1992AR01 Phys.Rev. C45, 759 (1992) Coulomb-Exchange Contribution to Proton-Nucleus Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=19.57-153 MeV; calculated σ(θ). 40Ca(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Momentum space calculations, Coulomb exchange contribution.
doi: 10.1103/PhysRevC.45.759
1991AR03 Phys.Rev. C43, 1875 (1991) H.F.Arellano, F.A.Brieva, W.G.Love, K.Nakayama Comparison of Nucleon-Nucleon Potential Models in a Full-Folding Description of Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300, 400 MeV; analyzed σ(θ), polarization observables data; deduced effective nucleon-nucleon potential dependence. Nonrelativistic full-folding model analysis.
doi: 10.1103/PhysRevC.43.1875
1991AR11 Phys.Rev. C43, 2734 (1991) H.F.Arellano, W.G.Love, F.A.Brieva Starting Energy Dependence of Elastic Scattering Observables in a Full-Folding Model NUCLEAR REACTIONS 16O(polarized p, p), E=135 MeV; 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), polarization observables; deduced starting energy dependence.
doi: 10.1103/PhysRevC.43.2734
1990AR03 Phys.Rev. C41, 2188 (1990); Erratum Phys.Rev. C42, 1782 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Nonrelativistic Full-Folding Model of Nucleon Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=400, 200 MeV; calculated σ(θ), analyzing power, spin-rotation parameter vs momentum transfer. Nonrelativistic full-folding optical potentials.
doi: 10.1103/PhysRevC.41.2188
1990AR11 Phys.Rev. C42, 652 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Role of Nuclear Densities in Nucleon Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 400 MeV; 16O(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced scattering observables sensitivity to density. Full-folding model.
doi: 10.1103/PhysRevC.42.652
1990AR31 J.Phys.(Paris), Colloq.C-6, 603 (1990) H.F.Arellano, W.E.Love, K.Nakayama, F.A.Brieva Off-Shell Effects of Nucleon-Nucleon Potential Models on Proton-Nucleus Elastic Scattering Observables NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.
1989AR05 Phys.Rev.Lett. 63, 605 (1989) H.F.Arellano, F.A.Brieva, W.G.Love Full-Folding-Model Description of Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Full folding model analysis.
doi: 10.1103/PhysRevLett.63.605
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