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NSR database version of May 21, 2024.

Search: Author = F.D.Pacati

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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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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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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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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.


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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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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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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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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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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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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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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1991PA06      Phys.Lett. 257B, 263 (1991)

F.D.Pacati, M.Radici

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
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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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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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1973BO18      Nucl.Phys. A204, 485 (1973)

S.Boffi, F.D.Pacati

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
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1973BO34      Nucl.Phys. A210, 477 (1973)

S.Boffi, F.D.Pacati

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
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1973PA19      Lett.Nuovo Cim. 7, 621 (1973)

F.D.Pacati, S.Boffi

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
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1971BO55      Nuovo Cim. 6A, 465 (1971)

S.Boffi, F.D.Pacati

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
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1970PA26      Phys.Rev. C2, 1205 (1970)

F.D.Pacati, S.Boffi

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
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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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