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NSR database version of May 21, 2024.

Search: Author = C.Giusti

Found 98 matches.

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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
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2024VO04      Few-Body Systems 65, 47 (2024)

M.Vorabbi, P.Finelli, C.Giusti

Determination of Nuclear Matter Radii by Means of Microscopic Optical Potentials: The Case of 78Kr

NUCLEAR REACTIONS 78Kr(p, p), E=153 MeV; analyzed available data; deduced σ(θ), the matter radius and estimating the neutron skin, quantities that are both needed to determine the slope parameter L of the nuclear symmetry energy with microscopic Nucleon–Nucleus Optical Potentials (OP).

doi: 10.1007/s00601-024-01919-z
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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
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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
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2020GI10      J.Phys.(London) G47, 024001 (2020)

C.Giusti, M.V.Ivanov

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2005GI02      Nucl.Phys. B(Proc.Supp.) S139, 105 (2005)

C.Giusti

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
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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
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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
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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
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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
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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
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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
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2003GI03      Phys.Rev. C 67, 044601 (2003)

C.Giusti, F.D.Pacati

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
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2003GI08      Eur.Phys.J. A 17, 419 (2003)

C.Giusti

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
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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
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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
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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
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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
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2002GI01      Nucl.Phys. A699, 57c (2002)

C.Giusti, F.D.Pacati

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
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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
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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
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2001GI16      Eur.Phys.J. A 12, 69 (2001)

C.Giusti, F.D.Pacati

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
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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
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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
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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
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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
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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)

C.Giusti, F.D.Pacati

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
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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
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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
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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
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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
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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
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1998GI14      Nucl.Phys. A641, 297 (1998)

C.Giusti, F.D.Pacati

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
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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
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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
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1997GI03      Nucl.Phys. A615, 373 (1997)

C.Giusti, F.D.Pacati

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
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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
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1995GI06      Nucl.Phys. A585, 618 (1995)

C.Giusti, F.D.Pacati

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
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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
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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
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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
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1994GI04      Nucl.Phys. A571, 694 (1994)

C.Giusti, F.D.Pacati

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
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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
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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
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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
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1991GI07      Nucl.Phys. A535, 573 (1991)

C.Giusti, F.D.Pacati

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
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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
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1989GI09      Nucl.Phys. A504, 685 (1989)

C.Giusti, F.D.Pacati

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
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1988BO05      Nucl.Phys. A476, 617 (1988)

S.Boffi, C.Giusti, F.D.Pacati

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
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1988GI07      Nucl.Phys. A485, 461 (1988)

C.Giusti, F.D.Pacati

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
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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
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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)

C.Giusti, F.D.Pacati

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
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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
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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
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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
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1985BO13      Nucl.Phys. A435, 697 (1985)

S.Boffi, C.Giusti, F.D.Pacati

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
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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
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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
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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
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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
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1982BO28      Nucl.Phys. A386, 599 (1982)

S.Boffi, C.Giusti, F.D.Pacati

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
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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
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1981BO02      Phys.Lett. B98, 11 (1981)

S.Boffi, C.Giusti, F.D.Pacati

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
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1981BO14      Nucl.Phys. A359, 91 (1981)

S.Boffi, C.Giusti, F.D.Pacati

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
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1981BO38      Lett.Nuovo Cim. 32, 381 (1981)

S.Boffi, C.Giusti, F.D.Pacati

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
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1980BO08      Nucl.Phys. A336, 416 (1980)

S.Boffi, C.Giusti, F.D.Pacati

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
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1980BO09      Nucl.Phys. A336, 437 (1980)

S.Boffi, C.Giusti, F.D.Pacati

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
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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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