NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Giusti Found 97 matches. 2024VO02 Phys.Rev. C 109, 034613 (2024) M.Vorabbi, C.Barbieri, V.Soma, P.Finelli, C.Giusti Microscopic optical potentials for medium-mass isotopes derived at the first order of Watson multiple-scattering theory
doi: 10.1103/PhysRevC.109.034613
2022VO02 Phys.Rev. C 105, 014621 (2022) M.Vorabbi, M.Gennari, P.Finelli, C.Giusti, P.Navratil, R.Machleidt Elastic proton scattering off nonzero spin nuclei NUCLEAR REACTIONS 6,7Li, 13C(polarized p, p), E=200 MeV; 10B(polarized p, p), E=197 MeV; 1H(9C, p), E=290 MeV; calculated σ(θ) and analyzing powers Ay(θ) using microscopic optical potential (OP) and chiral theories for the nucleon-nucleon (NN) interaction, extended to include the spin of the target nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.105.014621
2021VO03 Phys.Rev. C 103, 024604 (2021) M.Vorabbi, M.Gennari, P.Finelli, C.Giusti, P.Navratil, R.Machleidt Impact of three-body forces on elastic nucleon-nucleus scattering observables NUCLEAR REACTIONS 12C(polarized p, p), E=122, 160, 200, 300 MeV; 16O(p, p), (polarized p, p), E=100, 135, 200, 318 MeV; 12C(n, n), E=108, 128, 155, 185, 225 MeV; calculated differential σ(E, θ), and analyzing power Ay(Ε, θ) using nonrelativistic optical model potentials obtained from the no-core shell model densities using two- and three-nucleon chiral interactions; deduced that contribution of the 3N force in the tNN matrix is small for the differential cross section and sizable for the spin observables such as analyzing power. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.024604
2020GI10 J.Phys.(London) G47, 024001 (2020) Neutral current neutrino-nucleus scattering: theory NUCLEAR REACTIONS 12C(ν, X), E=500, 1000, 2000 MeV; calculated differential σ, σ. Comparison with available data.
doi: 10.1088/1361-6471/ab5251
2020VO04 Phys.Rev.Lett. 124, 162501 (2020) M.Vorabbi, M.Gennari, P.Finelli, C.Giusti, P.Navratil Elastic Antiproton-Nucleus Scattering from Chiral Forces
doi: 10.1103/PhysRevLett.124.162501
2018VO16 Phys.Rev. C 98, 064602 (2018) M.Vorabbi, P.Finelli, C.Giusti Proton-nucleus elastic scattering: Comparison between phenomenological and microscopic optical potentials NUCLEAR REACTIONS 16O, 40,42,44,48Ca(p, p), (polarized p, p), E=200, 318 MeV; 58Ni(p, p), (polarized p, p), E=192, 295, 333 MeV; 60Ni(p, p), (polarized p, p), E=178 MeV; 62Ni(p, p), E=156 MeV; 116,118,120,122,124Sn(p, p), (polarized p, p), E=295 MeV; 120Sn, 208Pb(p, p), (polarized p, p), E=200 MeV; 204,206,208Pb(p, p), E=295 MeV; 56Ni(p, p), E(cm)=400 MeV/nucleon; calculated differential σ(θ) relative to Rutherford σ, and analyzing power Ay using nonrelativistic optical model potentials, and compared with experimental data.
doi: 10.1103/PhysRevC.98.064602
2017VO09 Phys.Rev. C 96, 044001 (2017) M.Vorabbi, P.Finelli, C.Giusti Optical potentials derived from nucleon-nucleon chiral potentials at N4 LO NUCLEAR REACTIONS 12C, 16O, 40Ca(p, p), (polarized p, p), E=200 MeV; calculated pp and np Wolfenstein amplitudes, cross sections, analyzing powers, and spin rotations; deduced Optical potentials using use NN chiral potentials at fifth order (N4LO). Comparison with experimental data.
doi: 10.1103/PhysRevC.96.044001
2016IV03 Phys.Rev. C 94, 014608 (2016) M.V.Ivanov, J.R.Vignote, R.Alvarez-Rodriguez, A.Meucci, C.Giusti, J.M.Udias Global relativistic folding optical potential and the relativistic Green's function model NUCLEAR REACTIONS 12C(p, p), E=20-1040 MeV; analyzed σ(θ, E) data using global relativistic folding optical potential (GRFOP) fits; deduced differential cross sections, analyzing powers, and the spin rotation parameter. 12C(e, e), E=150-747 MeV; 12C(ν, μ-), (ν-bar, μ-), E=3-100 GeV muon neutrinos; 12C(ν, ν), (ν-bar, ν-bar), E=0.2-2.5 GeV; analyzed σ(E) and σ(θ) data from MiniBooNE collaboration using new GRFOP potential within the relativistic Green's function model.
doi: 10.1103/PhysRevC.94.014608
2016MA64 Eur.Phys.J. A 52, 298 (2016) M.Makek, P.Achenbach, C.Ayerbe Gayoso, C.Barbieri, J.C.Bernauer, R.Bohm, D.Bosnar, A.Denig, M.O.Distler, I.Friscic, C.Giusti, H.Merkel, U.Muller, L.Nungesser, J.Pochodzalla, S.Sanches Majos, B.S.Schlimme, M.Schwamb, Th.Walcher, for the A1 Collaboration Differential cross section measurement of the 12C(e, e'pp)10Beg.s. reaction NUCLEAR REACTIONS 12C(e, e'pp)10Begs, E=163 MeV; measured Ep, Ip using Si detectors and Ie, Ip using high-resolution magnetic spectrometers, pp-coin, ep-coin; deduced σ(E, θ). 10Be deduced excitation energy spectrum after triple coin; calculated σ(E, θ) using Pavia reaction code.
doi: 10.1140/epja/i2016-16298-3
2016VO02 Phys.Rev. C 93, 034619 (2016) M.Vorabbi, P.Finelli, C.Giusti Theoretical optical potential derived from nucleon-nucleon chiral potentials NUCLEAR REACTIONS 16O(p, p), (polarized p, p), E=100, 200, 450-600 MeV; calculated real and imaginary parts of pp and pn Wolfenstein amplitudes using two different chiral potentials (EM and EGM), σ(θ) and analyzing powers Ay(θ); deduced new microscopic optical potential for elastic proton-nucleus scattering. Chiral perturbation theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034619
2015AN10 Phys.Rev. C 92, 025501 (2015) A.M.Ankowski, M.B.Barbaro, O.Benhar, J.A.Caballero, C.Giusti, R.Gonzalez-Jimenez, G.D.Megias, A.Meucci Estimate of the theoretical uncertainty of the cross sections for nucleon knockout in neutral-current neutrino-oxygen interactions NUCLEAR REACTIONS 16O(ν, ν')n, (ν, ν')p, (ν-bar, ν'-bar)n, (ν-bar, ν'-bar)p, E<2.0 GeV; calculated σ(E) for neutron and proton knockouts induced by neutral-current (NC) quasielastic (QE) scattering of atmospheric neutrinos and antineutrinos using relativistic plane-wave impulse approximation (RPWIA), relativistic mean-field (RMF), relativistic Green's function (RGF), and superscaling (SuSA) approaches and comparison with realistic nuclear spectral functions (SF). Relevance to ongoing and future experiments at the Super- and Hyper-Kamiokande including searches of diffuse supernova neutrinos (DSN) and sterile neutrinos in the beam of T2K experiment.
doi: 10.1103/PhysRevC.92.025501
2015IV03 Phys.Rev. C 91, 034607 (2015) M.V.Ivanov, A.N.Antonov, M.B.Barbaro, C.Giusti, A.Meucci, J.A.Caballero, R.Gonzalez-Jimenez, E.Moya de Guerra, J.M.Udias Neutral current quasielastic (anti)neutrino scattering beyond the Fermi gas model at MiniBooNE and BNL kinematics
doi: 10.1103/PhysRevC.91.034607
2014ME03 Phys.Rev. C 89, 034604 (2014) A.Meucci, M.Vorabbi, C.Giusti, F.D.Pacati, P.Finelli Elastic and quasi-elastic electron scattering on the N=14, 20, and 28 isotonic chains NUCLEAR REACTIONS 22,28O, 24,30Ne, 26,32,40Mg, 28,34,42Si, 30,36,44S, 32,38,46Ar, 34,40,42,44,48Ca, 42,48,50Ti, 44,50,52,54Cr, 46,54Fe, 56Ni(e, e), (e, e'), E=250, 850, 1080 MeV; calculated differential σ(θ) for elastic and quasi-elastic scattering, proton and neutron density distributions, parity-violating asymmetry parameter, differential RPWIA and RGF σ for (e, e') for selected isotones of N=14, 20 and 28. Distorted-wave Born approximation (DWBA) and relativistic Hartree-Bogoliubov (RHB) approach with density dependent meson-exchange interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.034604
2014ME12 Phys.Rev. C 90, 027301 (2014) A.Meucci, M.Vorabbi, C.Giusti, P.Finelli Neutron density distribution and neutron skin thickness of 208Pb NUCLEAR STRUCTURE 208Pb; calculated neutron density distribution and neutron thickness using various nonrelativistic and relativistic mean-field models. Comparison with experimental data from (γ, π0) at Mainz, and parity-violating asymmetry parameter for elastic electron scattering and neutron thickeners data for PREX experiment at JLab.
doi: 10.1103/PhysRevC.90.027301
2013GO13 Phys.Rev. C 88, 025502 (2013) R.Gonzalez-Jimenez, J.A.Caballero, A.Meucci, C.Giusti, M.B.Barbaro, M.V.Ivanov, J.M.Udias Relativistic description of final-state interactions in neutral-current neutrino and antineutrino cross sections
doi: 10.1103/PhysRevC.88.025502
2013ME06 Phys.Rev. C 87, 054620 (2013) A.Meucci, M.Vorabbi, C.Giusti, F.D.Pacati, P.Finelli Elastic and quasi-elastic electron scattering off nuclei with neutron excess NUCLEAR REACTIONS 14,16,18,20,22,24,26,28O(e, e), (e, e'), E=374.5, 850, 1080 MeV; 36,38,40,42,44,46,48,50,52,54,56Ca(e, e), (e, e'), E=496.8, 560, 850 MeV; 48Ca(e, e), E=2.2 GeV; calculated differential σ(θ, ω), differential RPWIA and RGF σ(ω), parity-violating asymmetry parameters for elastic and inelastic scattering. 208Pb(e, e), (e, e'), E=1.063 GeV; calculated weak charge density and asymmetry parameter compared with measurements by PREX Collaboration. Distorted-wave Born approximation approach with proton and neutron density distributions from relativistic Dirac-Hartree model. Comparison with experimental data. NUCLEAR STRUCTURE 14,16,18,20,22,24,26,28O, 36,38,40,42,44,46,48,50,52,54,56Ca; evaluated neutron and proton distributions using relativistic Dirac-Hartree model.
doi: 10.1103/PhysRevC.87.054620
2012CO04 Phys.Rev. C 85, 024322 (2012) G.Co, V.De Donno, P.Finelli, M.Grasso, M.Anguiano, A.M.Lallena, C.Giusti, A.Meucci, F.D.Pacati Mean-field calculations of the ground states of exotic nuclei NUCLEAR STRUCTURE 16,22,24,28O, 40,48,52,60Ca, 48,56,68,78Ni, 100,114,116,132Sn; calculated binding energies, single particle energies, rms charge radii, neutron skin thickness. Mean-field approach, nonrelativistic Hartree-Fock, relativistic Hartree calculations. Comparison with experimental data. NUCLEAR REACTIONS 40,48,52,60Ca(e, e'p), (e, e), E=483.2 MeV; calculated reduced cross sections, elastic scattering cross sections, neutron, proton and matter distributions, Mean-field approach, nonrelativistic Hartree-Fock, relativistic Hartree calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.024322
2012GI06 J.Phys.:Conf.Ser. 366, 012019 (2012) C.Giusti, A.Meucci, F.D.Pacati, G.Co, V.De Donno Electron-induced proton knockout from neutron rich nuclei NUCLEAR REACTIONS 40,48,52,60Ca(e, e'p), E=483.2 MeV; calculated (reduced) σ vs missing momentum using RDWIA, DWIA-HF and DIWA-WS. Two lighter isotopes compared with published data.
doi: 10.1088/1742-6596/366/1/012019
2011GI07 Phys.Rev. C 84, 024615 (2011) C.Giusti, A.Meucci, F.D.Pacati, G.Co, V.De Donno Quasifree (e, e' p) reactions on nuclei with neutron excess NUCLEAR REACTIONS 16,22,24,28O, 40,48,52,60Ca(e, e'p), E at 0-300 MeV/c; calculated σ(E), rms radii, S(p), proton and neutron density functions, single-particle wave functions. Distorted wave impulse approximation calculations with nonrelativistic and relativistic models. Comparison with experimental data. Dependence on the neutron to proton asymmetry.
doi: 10.1103/PhysRevC.84.024615
2011ME07 Phys.Rev. C 83, 064614 (2011) A.Meucci, J.A.Caballero, C.Giusti, J.M.Udias Relativistic descriptions of quasielastic charged-current neutrino-nucleus scattering: Application to scaling and superscaling ideas NUCLEAR REACTIONS 12C(ν, μ-), E=1000, 1500, 2000 MeV for νμ; calculated inclusive quasielastic differential cross sections and scaling function using relativistic impulse approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064614
2011ME14 Phys.Rev.Lett. 107, 172501 (2011) A.Meucci, M.B.Barbaro, J.A.Caballero, C.Giusti, J.M.Udias Relativistic Descriptions of Final-State Interactions in Charged-Current Quasielastic Neutrino-Nucleus Scattering at MiniBooNE Kinematics
doi: 10.1103/PhysRevLett.107.172501
2010MI11 Eur.Phys.J. A 43, 137 (2010) D.G.Middleton, J.R.M.Annand, C.Barbieri, C.Giusti, P.Grabmayr, T.Hehl, I.J.D.MacGregor, I.Martin, J.C.McGeorge, F.Moschini, F.D.Pacati, M.Schwamb, D.Watts Knockout of proton-neutron pairs from 16O with electromagnetic probes NUCLEAR REACTIONS 16O(e, e'np)14N, E=215 MeV; 16O(γ, pn)14N, E=100-800 MeV; measured reaction products; deduced σ. Comparison with Pavia model of two-nucleon knockout predictions.
doi: 10.1140/epja/i2009-10902-7
2009ME07 Phys.Rev. C 80, 024605 (2009) A.Meucci, J.A.Caballero, C.Giusti, F.D.Pacati, J.M.Udias Relativistic descriptions of inclusive quasielastic electron scattering: Application to scaling and superscaling ideas NUCLEAR REACTIONS 12C(e, e'), E=620, 1000, 1299, 2020 MeV; calculated σ(θ), scaling functions using the relativistic impulse approximations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024605
2009TA34 Phys.Rev. C 80, 064601 (2009) T.Tamae, Y.Sato, T.Yokokawa, Y.Asano, M.Kawabata, O.Konno, I.Nakagawa, I.Nishikawa, K.Hirota, H.Yamazaki, R.Kimura, H.Miyase, H.Tsubota, C.Giusti, A.Meucci Comparison of the 12C(e, e'p) cross section at low momentum transfer with a relativistic calculation NUCLEAR REACTIONS 12C(e, e'p), E=197.5 MeV; measured Ep, Ip, σ, σ(θ), and reduced cross sections. Comparison with relativistic distorted-wave impulse approximation calculations and the 12C(γ, p) reaction.
doi: 10.1103/PhysRevC.80.064601
2008ME03 Phys.Rev. C 77, 034606 (2008) A.Meucci, C.Giusti, F.D.Pacati Spin effects in quasi-elastic neutrino-nucleus reactions NUCLEAR REACTIONS 12C(ν, n), (ν-bar, n), (ν, p), (ν-bar, p), (ν, ν), (ν-bar, ν-bar), E=500, 700, 1000, 2000 MeV; calculated polarization asymmetry. Relativistic DWIA calculation.
doi: 10.1103/PhysRevC.77.034606
2007GI01 Eur.Phys.J. A 31, 155 (2007) C.Giusti, F.D.Pacati, M.Schwamb, S.Boffi Center-of-mass effects in electromagnetic two-proton knockout reactions NUCLEAR REACTIONS 16O(e, e'2p), E=855 MeV; 16O(γ, 2p), E=400 MeV; calculated σ(E, θ), center-of-mass effects.
doi: 10.1140/epja/i2007-10001-y
2007GI14 Eur.Phys.J. A 33, 29 (2007) C.Giusti, F.D.Pacati, M.Schwamb, S.Boffi Electromagnetic proton-neutron knockout off 16O: New achievements in theory
doi: 10.1140/epja/i2007-10418-2
2006ME17 Nucl.Phys. A773, 250 (2006) A.Meucci, C.Giusti, F.D.Pacati Neutrino-nucleus quasi-elastic scattering and strange quark effects NUCLEAR REACTIONS 12C(ν, ν'p), (ν, ν'n), (ν-bar, ν-bar'p), (ν-bar, ν-bar'n), E=500, 1000 MeV; calculated quasielastic scattering σ(En), σ(Ep), final state interaction, strange-quark contribution and nuclear structure effects. Relativistic DWIA model, comparison with data.
doi: 10.1016/j.nuclphysa.2006.05.005
2006ME24 Acta Phys.Pol. B37, 2279 (2006) A.Meucci, C.Giusti, F.D.Pacati Relativistic approach to quasi-elastic neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, ν'p), (ν, ν'n), E=500 MeV; calculated En, Ep, σ(E), final state interaction effects, strangeness contribution.
2006MI22 Eur.Phys.J. A 29, 261 (2006); Erratum Eur.Phys.J. A 30, 469 (2006) D.G.Middleton, J.R.M.Annand, C.Barbieri, P.Barneo, P.Bartsch, D.Baumann, J.Bermuth, D.Bosnar, H.P.Blok, R.Bohm, M.Ding, M.O.Distler, D.Elsner, J.Friedrich, C.Giusti, D.I.Glazier, P.Grabmayr, S.Grozinger, T.Hehl, J.Heim, W.H.A.Hesselink, E.Jans, F.Klein, M.Kohl, L.Lapikas, I.J.D.MacGregor, I.Martin, J.C.McGeorge, H.Merkel, P.Merle, F.Moschini, U.Muller, Th.Pospischil, G.Rosner, H.Schmieden, M.Seimetz, A.Sule, H.de Vries, Th.Walcher, D.P.Watts, M.Weis, B.Zihlmann First measurements of the 16O(e, e'pn)14N reaction NUCLEAR REACTIONS 2H, 16O(e, e'np), E=855 MeV; measured particle spectra. 14N deduced excited states.
doi: 10.1140/epja/i2005-10314-9
2005CA24 Ann.Phys.(New York) 317, 492 (2005) F.Capuzzi, C.Giusti, F.D.Pacati, D.N.Kadrev Antisymmetrized Green's function approach to (e, e') reactions with a realistic nuclear density NUCLEAR REACTIONS 16O, 40Ca(e, e'), E ≈ 50-3000 MeV; calculated longitudinal and transverse response functions. Antisymmetrized Green's function approach.
doi: 10.1016/j.aop.2004.12.005
2005GI02 Nucl.Phys. B(Proc.Supp.) S139, 105 (2005) The (e, e'p) reaction on nuclei NUCLEAR REACTIONS 16O(e, e'p), E=520.6 MeV; calculated σ(E), spectroscopic factors, relativistic effects. DWIA approach, comparison with data.
doi: 10.1016/j.nuclphysbps.2004.11.231
2005GI20 Eur.Phys.J. A 26, 209 (2005) C.Giusti, F.D.Pacati, M.Schwamb, S.Boffi On the treatment of the Δ-contributions in electromagnetic pp-knockout reactions NUCLEAR REACTIONS 16O(e, e'2p), E=855 MeV; 16O(γ, 2p), E=120, 400 MeV; calculated σ(E, θ), Δ-current contributions. Comparisons with data.
doi: 10.1140/epja/i2005-10162-7
2005ME10 Nucl.Phys. A756, 359 (2005) A.Meucci, C.Giusti, F.D.Pacati Relativistic Green's function approach to parity-violating quasielastic electron scattering NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E=high; calculated response functions, parity-violating asymmetry, strange quark contribution. Relativistic Green's function approach.
doi: 10.1016/j.nuclphysa.2005.04.007
2004BA61 Phys.Rev. C 70, 014606 (2004) C.Barbieri, C.Giusti, F.D.Pacati, W.H.Dickhoff Effects of nuclear correlations on the 16O(e, e'pN) reactions to discrete final states NUCLEAR REACTIONS 16O(e, e'np), (e, e'2p), E=855 MeV; calculated σ(E, θ); deduced sensitivity to short-range and long-range correlations.
doi: 10.1103/PhysRevC.70.014606
2004BO46 Fizika(Zagreb) B 13, 1 (2004) S.Boffi, C.Giusti, F.D.Pacati, M.Schwamb NN correlations and final-state interactions in (e, e'NN) reactions NUCLEAR REACTIONS 16O(e, e'2p), (e, e'np), E=855 MeV; calculated σ(E, θ), final-state interaction effects.
2004ME12 Nucl.Phys. A739, 277 (2004) A.Meucci, C.Giusti, F.D.Pacati Relativistic Green's function approach to charged-current neutrino-nucleus quasielastic scattering NUCLEAR REACTIONS 16O(ν, μ-), E200-1000 MeV; calculated σ, σ(θ). 12C(ν, μ+), E not given; calculated muon spectrum. Relativistic Green's function approach, comparison with data.
doi: 10.1016/j.nuclphysa.2004.04.108
2004ME18 Nucl.Phys. A744, 307 (2004) A.Meucci, C.Giusti, F.D.Pacati Neutral-current neutrino-nucleus quasielastic scattering NUCLEAR REACTIONS 12C(ν, ν'p), (ν, ν'n), E=500, 700, 1000 MeV; calculated quasielastic scattering σ(En), σ(Ep), σ(Q2), final state interaction and nuclear structure effects. Comparison with data.
doi: 10.1016/j.nuclphysa.2004.08.023
2004SC17 Eur.Phys.J. A 20, 233 (2004) M.Schwamb, S.Boffi, C.Giusti, F.D.Pacati NN final-state interaction in two-nucleon knockout from 16O NUCLEAR REACTIONS 16O(e, e'2p), (e, e'np), E=855 MeV; 16O(γ, 2p), (γ, np), E=215 MeV; calculated σ(E, θ), final-state interaction effects.
doi: 10.1140/epja/i2003-10139-6
2003GI03 Phys.Rev. C 67, 044601 (2003) Meson exchange currents in electromagnetic one-nucleon emission NUCLEAR REACTIONS 16O(e, e'p), E=520, 2000 MeV; 16O(γ, p), E=60, 100, 196 MeV; calculated σ(θ), proton momentum; deduced role of meson exchange currents. Comparisons with data.
doi: 10.1103/PhysRevC.67.044601
2003GI08 Eur.Phys.J. A 17, 419 (2003) Theoretical aspects of (e, e'NN) reactions NUCLEAR REACTIONS 16O(e, e'2p), E=855 MeV; calculated σ(E, θ); deduced role of short-range correlations.
doi: 10.1140/epja/i2002-10185-6
2003KA31 Phys.Rev. C 68, 014617 (2003) D.N.Kadrev, M.V.Ivanov, A.N.Antonov, C.Giusti, F.D.Pacati Two-proton overlap functions in the Jastrow correlation method and cross section of the 160(e, e'pp)14C reaction NUCLEAR REACTIONS 16O(e, e'2p), E=584, 855 MeV; calculated two-proton overlap function, σ(E, θ). Jastrow correlation method, comparison with other model predictions.
doi: 10.1103/PhysRevC.68.014617
2003ME09 Phys.Rev. C 67, 054601 (2003) A.Meucci, F.Capuzzi, C.Giusti, F.D.Pacati Inclusive electron scattering in a relativistic Green's function approach NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E=high; calculated σ, response functions vs momentum transfer. Green's function approach, comparison with data.
doi: 10.1103/PhysRevC.67.054601
2003SC10 Eur.Phys.J. A 17, 7 (2003) M.Schwamb, S.Boffi, C.Giusti, F.D.Pacati On the NN final-state interaction in the 16O(e, e'pp) reaction NUCLEAR REACTIONS 16O(e, e'2p), E=855 MeV; calculated σ(E, θ), final-state interaction effects.
doi: 10.1140/epja/i2002-10148-y
2002GA48 Phys.Rev. C 66, 064308 (2002) M.K.Gaidarov, K.A.Pavlova, A.N.Antonov, C.Giusti, S.E.Massen, C.Moustakidis, K.Spasova Jastrow-type calculations of one-nucleon removal reactions on open s-d shell nuclei NUCLEAR STRUCTURE 24Mg, 28Si, 32S, 40Ca; calculated neutron and proton spectroscopic factors, separation energies. One-body density matrices. NUCLEAR REACTIONS 24Mg, 28Si, 32S(p, d), E=185 MeV; calculated σ(E, θ). 32S(e, e'p), E not given; calculated missing momentum spectrum. One-body density matrices, comparison with data.
doi: 10.1103/PhysRevC.66.064308
2002GI01 Nucl.Phys. A699, 57c (2002) Polarization in Electromagnetic Two-Nucleon Emission NUCLEAR REACTIONS 16O(polarized e, e'2p), (polarized e, e'np), E=855 MeV; 16O(polarized γ, np), (polarized γ, 2p), E=120 MeV; calculated polarization observables, correlation effects.
doi: 10.1016/S0375-9474(01)01470-1
2002IV02 Nucl.Phys. A699, 336c (2002) M.V.Ivanov, M.K.Gaidarov, A.N.Antonov, C.Giusti Effects of Nucleon Correlations Studied within the Generator Coordinate Method NUCLEAR REACTIONS 40Ca(e, e'p), E not given; 40Ca(γ, p), E=60 MeV; calculated σ(E), σ(θ); deduced nuclear correlation effects. Generator coordinate method.
doi: 10.1016/S0375-9474(01)01515-9
2002ME17 Phys.Rev. C66, 034610 (2002) A.Meucci, C.Giusti, F.D.Pacati Meson Exchange Currents in a Relativistic Model for Electromagnetic One Nucleon Emission NUCLEAR REACTIONS 16O(γ, p), E=60-196 MeV; 12C(γ, p), E=58.4 MeV; 16O(γ, n), E=60 MeV; calculated σ(θ), photon asymmetry; deduced role of meson exchange currents. Relativistic model.
doi: 10.1103/PhysRevC.66.034610
2001GI16 Eur.Phys.J. A 12, 69 (2001) Polarization Observables in (γ(pol), N(pol)N) Reactions NUCLEAR REACTIONS 16O(polarized γ, np), (polarized γ, 2p), E=100, 120, 400 MeV; calculated σ(θ), polarization observables; deduced nuclear structure effects.
doi: 10.1007/s100500170040
2001IV04 Phys.Rev. C64, 014605 (2001) M.V.Ivanov, M.K.Gaidarov, A.N.Antonov, C.Giusti Generator Coordinate Method Calculations of One-Nucleon Removal Reactions on 40Ca NUCLEAR REACTIONS 40Ca(e, e'p), E=460, 483 MeV; calculated σ(E). 40Ca(γ, p), E=60 MeV; 40Ca(p, d), E=65 MeV; calculated σ(θ). Generator coordinate method, comparisons with data. NUCLEAR STRUCTURE 40Ca; calculated neutron and proton separation energies, single-particle overlap functions. Generator coordinate method.
doi: 10.1103/PhysRevC.64.014605
2001ME14 Phys.Rev. C64, 014604 (2001) A.Meucci, C.Giusti, F.D.Pacati Relativistic Corrections in (e, e'p) Knockout Reactions NUCLEAR REACTIONS 16O(e, e'p), E=2000 MeV; calculated σ(E), structure functions vs proton energy, recoil momentum; deduced relativistic effects.
doi: 10.1103/PhysRevC.64.014604
2001ME29 Phys.Rev. C64, 064615 (2001) A.Meucci, C.Giusti, F.D.Pacati Relativistic Corrections in (γ, N) Knockout Reactions NUCLEAR REACTIONS 16O(γ, p), E=609-257 MeV; calculated σ(θ), photon asymmetry. 16O(γ, n), E=60-250 MeV; 12C(γ, p), E=58.4, 78.5 MeV; calculated σ(θ). Relativistic DWIA, comparison with data.
doi: 10.1103/PhysRevC.64.064615
2000GA01 Phys.Rev. C61, 014306 (2000) M.K.Gaidarov, K.A.Pavlova, A.N.Antonov, M.V.Stoitsov, S.S.Dimitrova, M.V.Ivanov, C.Giusti Overlap Functions in Correlation Methods and Quasifree Nucleon Knockout from 16O NUCLEAR REACTIONS 16O(e, e'n), (e, e'p), E=521 MeV; calculated σ, missing mass spectra; deduced nucleon-nucleon correlation effects. 16O(γ, p), E=72 MeV; calculated σ(E, θ); deduced meson exchange current contributions. Comparisons with data.
doi: 10.1103/PhysRevC.61.014306
2000GA42 Trans.Bulg.Nucl.Soc. 5, 188 (2000) M.K.Gaidarov, K.A.Pavlova, A.N.Antonov, S.S.Dimitrova, M.V.Stoitsov, C.Giusti, D.Van Neck, H.Muther New Theoretical Treatment of One-Nucleon Transfer Reactions NUCLEAR REACTIONS 16O(p, d), E=31.8, 45.3, 65 MeV; 16O(e, e'p), E=520.6 MeV; 16O(γ, p), E=60 MeV; calculated single-particle overlap functions, σ(θ). comparisons with data.
2000GI08 Phys.Rev. C61, 054617 (2000) Proton Recoil Polarization in Exclusive (e, e'pp) Reactions NUCLEAR REACTIONS 16O(polarized e, e'2p), E=855 MeV; calculated σ(θ), outgoing proton polarization, polarization transfer coefficients; deduced role of short-range nuclear correlations.
doi: 10.1103/PhysRevC.61.054617
2000ST02 Phys.Lett. 474B, 33 (2000) R.Starink, M.F.van Batenburg, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, C.Giusti, D.L.Groep, P.Heimberg, W.H.A.Hesselink, M.Iodice, E.Jans, L.Lapikas, R.De Leo, C.J.G.Onderwater, F.D.Pacati, R.Perrino, J.Ryckebusch, M.F.M.Steenbakkers, J.A.Templon, G.-M.Urciuoli, L.B.Weinstein Evidence for Short-Range Correlations in 16O NUCLEAR REACTIONS 16O(e, e'2p), E=580-585 MeV; measured σ(E), missing momentum spectra. 16O deduced short-range correlations.
doi: 10.1016/S0370-2693(99)01510-5
1999DE08 Nucl.Phys. A650, 199 (1999) P.Demetriou, A.Gil, S.Boffi, C.Giusti, E.Oset, F.D.Pacati Comparison of Monte Carlo Simulation and Direct Multistep Scattering Theory in (e, e'p) Nuclear Reactions NUCLEAR REACTIONS 40Ca(e, e'p), E=497 MeV; calculated σ(Ep, θ). Comparison of Monte Carlo, direct multistep methods for final state interaction.
doi: 10.1016/S0375-9474(99)00108-6
1999GI15 Phys.Rev. C60, 054608 (1999) C.Giusti, H.Muther, F.D.Pacati, M.Stauf Short-Range and Tensor Correlations in the 16O(e, e'pn) Reaction NUCLEAR REACTIONS 16O(e, e'np), E=855 MeV; calculated σ(E, θ) vs recoil momentum; deduced role of nucleon-nucleon correlations, two-body meson exchange currents.
doi: 10.1103/PhysRevC.60.054608
1998DE22 Nucl.Phys. A634, 57 (1998) P.Demetriou, S.Boffi, C.Giusti, F.D.Pacati Charge-Exchange and Multi-Scattering Effects in (e, e'n) Knockout NUCLEAR REACTIONS 40Ca(e, e'n), E not given; calculated σ(E, θ); deduced two-, three-step charge exchange processes contributions. Multistep direct theory.
doi: 10.1016/S0375-9474(98)00149-3
1998GI05 Phys.Rev. C57, 1691 (1998) C.Giusti, F.D.Pacati, K.Allaart, W.J.W.Geurts, W.H.Dickhoff, H.Muther Selectivity of the 16O(e, e'pp) Reaction to Discrete Final States NUCLEAR REACTIONS 16O(e, e'2p), E=475, 584, 855 MeV; calculated σ(E, θ); deduced final state selectivity.
doi: 10.1103/PhysRevC.57.1691
1998GI14 Nucl.Phys. A641, 297 (1998) Photon-Induced Two-Nucleon Knockout Reactions to Discrete Final States NUCLEAR REACTIONS 16O(γ, np), (γ, 2p), (polarized γ, np), (polarized γ, 2p), E=45-105 MeV; calculated σ(Ex, θ), asymmetries; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(98)00468-0
1998ON02 Phys.Rev.Lett. 81, 2213 (1998) C.J.G.Onderwater, K.Allaart, E.C.Aschenauer, Th.S.Bauer, D.J.Boersma, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, W.J.W.Geurts, C.Giusti, D.L.Groep, W.H.A.Hesselink, M.Iodice, E.Jans, N.Kalantar-Nayestanaki, W.-J.Kasdorp, C.Kormanyos, L.Lapikas, J.J.van Leeuwe, R.De Leo, A.Misiejuk, H.Muther, F.D.Pacati, A.R.Pellegrino, R.Perrino, R.Starink, M.Steenbakkers, G.van der Steenhoven, J.J.M.Steijger, M.A.van Uden, G.M.Urciuoli, L.B.Weinstein, H.W.Willering Signatures for Short-Range Correlations in 16O Observed in the Reaction 16O(e, e'pp)14C NUCLEAR REACTIONS 16O(e, e'2p), E=584 MeV; measured σ(Ee, θ(e), Ep, θ(p)), missing momentum; deduced short-range correlations role.
doi: 10.1103/PhysRevLett.81.2213
1997DE47 Nucl.Phys. A625, 513 (1997) P.Demetriou, S.Boffi, C.Giusti, F.D.Pacati Multi-Scattering Effects in (e, e'p) Knockout NUCLEAR REACTIONS 40Ca(e, e'p), E=497 MeV; calculated σ(θ, Ee, Ep); deduced multistep processes role. Comparisons with experiment.
doi: 10.1016/S0375-9474(97)00406-5
1997GI03 Nucl.Phys. A615, 373 (1997) Exclusive (e, e'pp) Knockout Reactions NUCLEAR REACTIONS 16O(e, e'2p), E not given; calculated exclusive differential σ; deduced initial proton pair cm orbital angular momentum dependence. Short-range correlations, two-body currents, Δ-excitation, final state interactions.
doi: 10.1016/S0375-9474(97)00006-7
1997WI26 Z.Phys. A359, 467 (1997) P.Wilhelm, H.Arenhovel, C.Giusti, F.D.Pacati Treatment of the Δ Current in Electromagnetic Two-Nucleon Knockout Reactions NUCLEAR REACTIONS 16O(γ, 2p), E=50-400 MeV; calculated σ(E, θ); deduced Δ-current dependence.
doi: 10.1007/s002180050428
1995GI06 Nucl.Phys. A585, 618 (1995) Charge Exchange in Final-State Interactions of (e, e'pp) Reactions NUCLEAR REACTIONS 16O(e, e'2p), E=500 MeV; calculated differential σ. Charge exchange plus direct one-step knockout mechanism.
doi: 10.1016/0375-9474(94)00799-S
1995KE06 Phys.Rev.Lett. 74, 1712 (1995) L.J.H.M.Kester, W.H.A.Hesselink, N.Kalantar-Nayestanaki, J.H.Mitchell, A.Pellegrino, E.Jans, J.Konijn, J.J.M.Steijger, J.L.Visschers, A.Zondervan, J.R.Calarco, D.DeAngelis, F.W.Hersman, W.Kim, Th.S.Bauer, M.W.Kelder, Z.Papandreou, C.Giusti, F.D.Pacati Short-Range Nucleon-Nucleon Correlations Investigated with the Reaction 12C(e, e'pp) NUCLEAR REACTIONS 12C(e, e'2p), E=475 MeV; measured σ(E(e'), (θp)1, (θp)2, θ(e'), (Ep1), (Ep2)); deduced short range nucleon-nucleon correlations role in two-nucleon knockout.
doi: 10.1103/PhysRevLett.74.1712
1995ZO01 Nucl.Phys. A587, 697 (1995) A.Zondervan, L.J.de Bever, E.Jans, J.Konijn, M.Kruijer, J.J.M.Steijger, J.L.Visschers, P.J.Countryman, W.H.A.Hesselink, N.Kalantar-Nayestanaki, L.J.H.M.Kester, J.H.Mitchell, A.Pellegrino, J.R.Calarco, F.W.Hersman, M.Leuschner, T.P.Smith, Th.S.Bauer, M.W.Kelder, C.Giusti, F.D.Pacati, J.Ryckebusch, M.Vanderhaeghen The 12C(e, e'p) and 12C(e, e'pp) Reactions in the Δ-Resonance Region NUCLEAR REACTIONS 12C(e, e'p), (e, e'2p), E ≈ Δ resonance; measured six-fold, ninefold differential σ; deduced reaction mechanism. Model comparison.
doi: 10.1016/0375-9474(95)00044-2
1994BE19 Nucl.Phys. A574, 716 (1994) G.Benenti, C.Giusti, F.D.Pacati Meson-Exchange Current Effects in Nucleon Photoemission NUCLEAR REACTIONS 16O(γ, p), (γ, n), E=60, 150 MeV; calculated σ(θ); deduced meson exchange currents role. Direct knockout model.
doi: 10.1016/0375-9474(94)90956-3
1994GI04 Nucl.Phys. A571, 694 (1994) One- and Two-Nucleon Knockout in Electron Scattering NUCLEAR REACTIONS 16O(e, e'np), (e, e'2p), E=700 MeV; calculated σ(θ, E(e'), θ1, θ2). Two nucleon emission model.
doi: 10.1016/0375-9474(94)90716-1
1993BO35 Nucl.Phys. A564, 473 (1993) S.Boffi, C.Giusti, F.D.Pacati, M.Radici Dynamics of Direct Photoemission of Proton-Neutron Pairs NUCLEAR REACTIONS 16O(γ, np), E=80-350 MeV; calculated σ(θp, θn). 9Be(γ, np), E=247 MeV; calculated σ(θn); deduced direct photoemission features. Unfactorized approach.
doi: 10.1016/0375-9474(93)90209-G
1992GI05 Nucl.Phys. A546, 607 (1992) C.Giusti, F.D.Pacati, M.Radici Two-Proton Emission Induced by Real and Virtual Photons NUCLEAR REACTIONS 16O(e, e'2p), E=400, 700 MeV; 16O(γ, 2p), E=200 MeV; calculated σ(θ1, θ2, E1) vs model parameter. Coplanar symmetrical kinematics, unfactorized approach.
doi: 10.1016/0375-9474(92)90547-W
1991CA09 Nucl.Phys. A524, 681 (1991) F.Capuzzi, C.Giusti, F.D.Pacati Final-State Interaction in Electromagnetic Response Functions NUCLEAR REACTIONS 12C, 40Ca(e, e'p), E not given; calculated longitudinal, transverse response functions.
doi: 10.1016/0375-9474(91)90269-C
1991GI07 Nucl.Phys. A535, 573 (1991) Two-Proton Emission Induced by Electron Scattering NUCLEAR REACTIONS 16O(e, e'2p), E=700 MeV; calculated σ(θ(e'), θ1, θ2); deduced short range correlations, outgoing particle distortions role.
doi: 10.1016/0375-9474(91)90476-M
1990BO31 Nucl.Phys. A518, 639 (1990) S.Boffi, C.Giusti, F.D.Pacati, M.Radici Nucleon Recoil Polarization in Electromagnetic Quasi-Free Knockout Including Two-Body Currents NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated structure function vs missing momentum for polarized emitted proton. One photon exchange approximation.
doi: 10.1016/0375-9474(90)90183-M
1989GI09 Nucl.Phys. A504, 685 (1989) Complete Determination of Scattering Amplitudes and Nucleon Polarization in Electromagnetic Knockout Reactions NUCLEAR REACTIONS 90Zr, 16O, 12C(e, e'p), E=700 MeV; 12C(e, e'n), E=500 MeV; calculated outgoing nucleon polarization observables vs momentum. DWIA, knockout mechanism.
doi: 10.1016/0375-9474(89)90003-1
1988BO05 Nucl.Phys. A476, 617 (1988) Quasi-Free (e(pol), e'N) Reactions on Polarized Targets NUCLEAR REACTIONS 7Li(polarized e, e'p), (e, e'p), E=700 MeV; 39K(polarized e, e'p), (e, e'p), E=500 MeV; calculated σ(θ(e')) vs proton recoil momentum, electron asymmetry. Quasifree scattering, nonrelativistic DWIA. Polarized target.
doi: 10.1016/0375-9474(88)90327-2
1988GI07 Nucl.Phys. A485, 461 (1988) Separation of Structure Functions and Electron Distortion in Quasifree (e, e'p) Reactions NUCLEAR REACTIONS 40Ca, 208Pb(e, e'p), E=410 MeV; calculated longitudinal, transverse structure functions. One photon exchange approximation.
doi: 10.1016/0375-9474(88)90548-9
1988RE01 Phys.Rev.Lett. 60, 776 (1988) D.Reffay-Pikeroen, M.Bernheim, S.Boffi, G.P.Capitani, E.De Sanctis, S.Frullani, F.Garibaldi, A.Gerard, C.Giusti, H.Jackson, A.Magnon, C.Marchand, J.Mougey, J.Morgenstern, F.D.Pacati, J.Picard, S.Turck-Chieze, P.Vernin Bound-Nucleon Response Functions from the Reaction 40Ca(e, e'p)39K(*) and Nuclear-Medium Effects NUCLEAR REACTIONS 40Ca(e, e'p), E=52, 121, 146 MeV/c; measured σ(θ(e'), E(e'), θp', Ep'); deduced longitudinal, transverse structure functions.
doi: 10.1103/PhysRevLett.60.776
1987BO54 Nuovo Cim. 98A, 291 (1987) S.Boffi, C.Giusti, F.D.Pacati, F.Cannata Missing Strength in (e, e'p) Reactions and Nonlocality in Final-State Interactions NUCLEAR REACTIONS 12C, 16O, 40Ca, 51V, 90Zr(e, e'p), E not given; calculated occupation number damping factor.
1987GI07 Nucl.Phys. A473, 717 (1987) Electron Distortion in Quasifree (e, e'p) Reactions NUCLEAR REACTIONS 40Ca(e, e'p), E=400, 640 MeV; 63Cu(e, e'p), E=500 MeV; 208Pb(e, e'p), E=410, 710 MeV; calculated reduced σ vs momentum transfer. Coulomb distortion effects.
doi: 10.1016/0375-9474(87)90276-4
1987VA08 Phys.Rev.Lett. 58, 1727 (1987) G.van der Steenhoven, A.M.van den Berg, H.P.Blok, S.Boffi, J.F.J.van den Brand, R.Ent, T.de Forest, Jr., C.Giusti, J.W.A.den Herder, E.Jans, G.J.Kramer, J.B.J.M.Lanen, L.Lapikas, J.Mougey, P.J.Mulders, F.D.Pacati, E.N.M.Quint, P.K.A.de Witt Huberts Nuclear-Density Dependence of the Electron-Proton Coupling NUCLEAR REACTIONS 6Li(e, e'p), E=322, 479.9 MeV; measured reduced σ ratios; deduced electron-proton coupling nuclear density dependence. Enriched target. DWIA analyses.
doi: 10.1103/PhysRevLett.58.1727
1986VA17 Phys.Rev.Lett. 57, 182 (1986) G.van der Steenhoven, H.P.Blok, J.F.J.van den Brand, T.de Forest, Jr., J.W.A.den Herder, E.Jans, P.H.M.Keizer, L.Lapikas, P.J.Mulders, E.N.M.Quint, P.K.A.de Witt Huberts, J.Mougey, S.Boffi, C.Giusti, F.D.Pacati Effect of Nuclear Medium on the Proton Investigated with Reaction 12C(e, e'p)11B NUCLEAR REACTIONS 12C(e, e'p), E=312.8, 443.3 MeV; measured σ(E(e'), θ(e'), Ep', θp); deduced longitudinal, transverse response functions, medium effects.
doi: 10.1103/PhysRevLett.57.182
1985BO12 Nucl.Phys. A436, 438 (1985) S.Boffi, F.Capuzzi, C.Giusti, F.D.Pacati Charge Exchange in the Final State of Direct (γ, n) Reactions NUCLEAR REACTIONS 12C(γ, n), E=60, 80 MeV; 40Ca(γ, n), E=80 MeV; calculated σ(θ); deduced charge exchange mechanism role.
doi: 10.1016/0375-9474(85)90078-8
1985BO13 Nucl.Phys. A435, 697 (1985) Structure Functions in Nucleon Emission by Polarized Electrons NUCLEAR REACTIONS 16O(polarized e, e'p), E=500 MeV; calculated σ(θ(e'), θp); deduced fifth structure function existence possibility. Quasifree nucleon knockout.
doi: 10.1016/0375-9474(85)90182-4
1984BO18 Nucl.Phys. A420, 38 (1984) S.Boffi, R.Cenni, C.Giusti, F.D.Pacati Orthogonality, Antisymmetry and c.m. Effects in Direct Photoreactions NUCLEAR REACTIONS 12C(γ, p), (γ, n), E=40, 60, 80, 100 MeV; calculated σ(θ); deduced orthogonality, antisymmetrization, recoil effect role. PWIA, DWIA analyses.
doi: 10.1016/0375-9474(84)90655-9
1983BO28 Nuovo Cim. 76A, 685 (1983) S.Boffi, C.Giusti, F.D.Pacati, M.Rosa-Clot A Sum Rule Approach to Effective Charges in Electromagnetic Knock-Out Reactions NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E not given; calculated squared neutron, proton effective charges, ratios vs momentum transfer, θ. Quasielastic knockout, sum rule approach.
doi: 10.1007/BF02904601
1982BE02 Nucl.Phys. A375, 381 (1982) M.Bernheim, A.Bussiere, J.Mougey, D.Royer, D.Tarnowski, S.Turck-Chieze, S.Frullani, S.Boffi, C.Giusti, F.D.Pacati, G.P.Capitani, E.De Sanctis, G.J.Wagner The Influence of Bound States and Optical Potentials on 1p Momentum Distributions Obtained from 12C and 16O(e, e'p) Reactions NUCLEAR REACTIONS 12C, 16O(e, e'p), E=500 MeV; measured σ(missing energy, recoil momentum); deduced proton-hole spectral functions. Unfactorized DWIA analysis.
doi: 10.1016/0375-9474(82)90020-3
1982BO16 Nucl.Phys. A379, 509 (1982) S.Boffi, F.Cannata, F.Capuzzi, C.Giusti, F.D.Pacati Orthogonality and the Perey Factor in Knockout Reactions Induced by Electromagnetic Probes NUCLEAR REACTIONS 16O(γ, p), E=80 MeV; calculated σ(θ). Knockout reactions, channel orthogonality, optical potentials.
doi: 10.1016/0375-9474(82)90011-2
1982BO28 Nucl.Phys. A386, 599 (1982) Structure Functions in Quasi-free (e, e'p) Reactions NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated proton-hole structure functions. Quasifree scattering.
doi: 10.1016/0375-9474(82)90039-2
1981BA10 Nucl.Phys. A358, 371c (1981) P.Barreau, M.Bernheim, S.Boffi, A.Bussiere, G.P.Capitani, S.Frullani, C.Giusti, J.Mougey, J.Morgenstern, F.Pacati, D.Royer, E.De Sanctis, D.Tarnowski, S.Turck-Chieze, G.J.Wagner Improvements in the Interpretation of Quasi Free Scattering Coincidence Experiments NUCLEAR REACTIONS 16O(e, e'p), E not given; analyzed σ, e'p-coin data; calculated spectral function; deduced final state interaction effects, dependence on optical model absorption term. DWBA calculations, quasifree scattering.
doi: 10.1016/0375-9474(81)90341-9
1981BO02 Phys.Lett. B98, 11 (1981) Direct Nucleon Emission by Polarized Photons NUCLEAR REACTIONS 16O(polarized γ, p), (polarized γ, n), E=60, 80, 100 MeV; calculated σ(θ). Linearly polarized beam, direct knockout mechanism, final state distortion.
doi: 10.1016/0370-2693(81)90355-5
1981BO14 Nucl.Phys. A359, 91 (1981) Direct Mechanism in Medium Energy (γ, p0) Reactions NUCLEAR REACTIONS 16O, 12C(γ, p), E=60, 80, 100 MeV; 40Ca(γ, p), E=50-200 MeV; analyzed σ(θp, E); deduced optical potential dependence. Direct knockout mechanism.
doi: 10.1016/0375-9474(81)90213-X
1981BO38 Lett.Nuovo Cim. 32, 381 (1981) On Medium-Energy (γ, p0) Reactions at Foward Angles NUCLEAR REACTIONS 16O(γ, p), E=80 MeV; analyzed σ(θ) from different models; deduced one-body knockout mechanism validity.
doi: 10.1007/BF02745131
1980BO08 Nucl.Phys. A336, 416 (1980) Electron-Nucleon Interaction in Quasi-Free Scattering (I). Non-Relativistic Hamiltonian Through Second Order NUCLEAR REACTIONS 12C(e, e'p), (e, e'n), E=500 MeV; calculated σ(θ). Relativistic, nonrelativistic approach.
doi: 10.1016/0375-9474(80)90218-3
1980BO09 Nucl.Phys. A336, 437 (1980) Spin-Orbit Distortion of the Emerging Nucleon in Quasi-Free Electron Scattering NUCLEAR REACTIONS 12C(e, e'p), E=500 MeV; calculated σ(θ); deduced p spin-orbit distortion. Quasifree scattering.
doi: 10.1016/0375-9474(80)90220-1
1979BO07 Nucl.Phys. A319, 461 (1979) S.Boffi, C.Giusti, F.D.Pacati, S.Frullani Validity of the Factorized DWIA in (e, e'p) Reactions NUCLEAR REACTIONS 12C(e, e'p); calculated σ(θ) vs recoil momentum. Model without factorization into nondiagonal spectral function, off-shell two-body electron-nucleon scattering amplitude. Compared with DIWA.
doi: 10.1016/0375-9474(79)90526-8
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