NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = F.D.Pacati Found 78 matches. 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
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
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
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.
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
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
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
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
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
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
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
1991PA06 Phys.Lett. 257B, 263 (1991) Polarization Observables and Asymmetry in Electromagnetic Quasi-Free Proton Knockout NUCLEAR REACTIONS 16O(e, e'p), E=700 MeV; calculated ep-coin, polarized proton. Unpolarized target, one photon exchange approximation.
doi: 10.1016/0370-2693(91)91890-8
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
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
1973BO18 Nucl.Phys. A204, 485 (1973) Realistic One-Particle Density Matrix and Single-Particle Description of Nuclei NUCLEAR STRUCTURE 16O, 40Ca calculated one particle density matrix; deduced single particle energies.
doi: 10.1016/0375-9474(73)90389-8
1973BO34 Nucl.Phys. A210, 477 (1973) Self-Consistent Center-of-Mass Correction and the Charge Form Factor of 4He NUCLEAR STRUCTURE 4He; calculated charge form factors.
doi: 10.1016/0375-9474(73)90287-X
1973PA19 Lett.Nuovo Cim. 7, 621 (1973) Variational Approach to 4He with Separation of Centre-of-Mass Motion NUCLEAR STRUCTURE 4He; calculated binding energy, single particle wave functions.
doi: 10.1007/BF02728038
1971BO55 Nuovo Cim. 6A, 465 (1971) Parity Projection in Spherical Nuclei NUCLEAR STRUCTURE 4He; calculated binding energy, charge form factor. 16O; calculated levels, binding energy. Variational formalism, parity projection.
doi: 10.1007/BF02723380
1970PA26 Phys.Rev. C2, 1205 (1970) Slater Determinants, Parity Projection, and Hartree-Fock Calculations NUCLEAR STRUCTURE 3H, 3He; calculated binding energy. Hartree-Fock method, Slater determinants.
doi: 10.1103/PhysRevC.2.1205
1967BO34 Nuovo Cimento 52B, 244 (1967) S.Boffi, F.D.Pacati, J.Sawicki A Simple Model of 9Be and the Reaction 9Be(γ, n)8Be NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF02710670
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