NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = S.Boffi Found 77 matches. 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
2007PA12 Nucl.Phys. A782, 86c (2007) Generalized parton distributions in a meson cloud model
doi: 10.1016/j.nuclphysa.2006.10.006
2006PA21 Phys.Rev. D 73, 094001 (2006) Virtual meson cloud of the nucleon and generalized parton distributions NUCLEAR STRUCTURE 1H; calculated generalized parton distributions. Convolution model, virtual meson cloud.
doi: 10.1103/PhysRevD.73.094001
2005BO23 Nucl.Phys. A755, 549c (2005) Generalized parton distributions of the nucleon in constituent quark models
doi: 10.1016/j.nuclphysa.2005.03.099
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
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.
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
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
2003WA30 Eur.Phys.J. A 18, 155 (2003) R.F.Wagenbrunn, S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici Relativistic study of nucleon electroweak properties in a constituent-quark model NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Constituent-quark model.
doi: 10.1140/epja/i2002-10291-5
2002BO23 Eur.Phys.J. A 14, 17 (2002) S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici, R.F.Wagenbrunn Covariant Electroweak Nucleon Form Factors in a Chiral Constituent-Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic and pseudoscalar form factors, charge radii. Chiral constituent-quark model.
doi: 10.1007/s10050-002-8784-3
2002PL01 Nucl.Phys. A699, 312c (2002) W.Plessas, S.Boffi, L.Ya.Glozman, W.Klink, M.Radici, R.F.Wagenbrunn Nucleon Properties in a Semirelativistic Chiral Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Goldstone-boson-exchange constituent quark model, comparison with data.
doi: 10.1016/S0375-9474(01)01509-3
2002SC46 Nucl.Phys. A711, 207c (2002) P.Schweitzer, S.Boffi, M.Radici Polynomiality of off-forward distribution functions in the chiral quark soliton model
doi: 10.1016/S0375-9474(02)01218-6
2001BO02 Nucl.Phys. A680, 80c (2001) S.Boffi, P.Demetriou, M.Radici, R.F.Wagenbrunn Electromagnetic Properties of Hadrons in a Chiral Constituent-Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated μ. 1H; calculated magnetic form factor vs momentum transfer. Chiral constituent quark model, comparisons with data.
doi: 10.1016/S0375-9474(00)00393-6
2001GL08 Phys.Lett. 516B, 183 (2001) L.Ya.Glozman, M.Radici, R.F.Wagenbrunn, S.Boffi, W.Klink, W.Plessas Covariant Axial Form Factor of the Nucleon in a Chiral Constituent Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated axial form factor. Chiral constituent quark model.
doi: 10.1016/S0370-2693(01)00915-7
2001WA30 Phys.Lett. 511B, 33 (2001) R.F.Wagenbrunn, S.Boffi, W.Klink, W.Plessas, M.Radici Covariant Nucleon Electromagnetic Form Factors from the Goldstone-Boson-Exchange Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated electric and magnetic form factors. Constituent quark model, point-form approach, comparison with data.
doi: 10.1016/S0370-2693(01)00622-0
2000BA95 Eur.Phys.J. A 9, 131 (2000) Semi-Inclusive Structure Functions in the Spectator Model
doi: 10.1007/s100500070063
2000WA30 Eur.Phys.J. A 8, 385 (2000) R.F.Wagenbrunn, M.Radici, S.Boffi, P.Demetriou Nucleon Magnetic Moments in an Extended Chiral Constituent Quark Model NUCLEAR STRUCTURE 1H, 1n; calculated magnetic moment. Goldstone boson exchange model. Comparison with data.
doi: 10.1007/s100530050048
1999BO30 Phys.Rev. C60, 025206 (1999) S.Boffi, P.Demetriou, M.Radici, R.F.Wagenbrunn Nucleon Form Factors in a Chiral Constituent-Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors. Chiral constituent-quark model.
doi: 10.1103/PhysRevC.60.025206
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
1999DO30 Phys.Rev. C60, 064622 (1999) S.M.Dolfini, R.O.Alarcon, H.Arenhovel, R.Beck, A.M.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, J.R.Comfort, D.Dale, G.Dodson, K.Dow, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, J.Mandeville, D.J.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, C.E.Vellidis, L.Weinstein, S.Williamson Out-of-Plane Measurements of the Fifth Response Function of the Exclusive Electronuclear Response NUCLEAR REACTIONS 2H, 12C(polarized e, e'p), E=560 MeV; measured coincidence yields, σ(θ), beam asymmetry; deduced unpolarized σ, fifth response function f'(LT). Magnetic spectrometers, out-of-plane measurements. DWIA calculations.
doi: 10.1103/PhysRevC.60.064622
1998BO24 Nucl.Phys. A637, 585 (1998) S.Boffi, F.Capuzzi, P.Demetriou, M.Radici Semi-Relativistic Charge-Current Density Operator
doi: 10.1016/S0375-9474(98)00417-5
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
1998GO08 Phys.Rev. C57, 2618 (1998) Ye.S.Golubeva, L.A.Kondratyuk, A.Bianconi, S.Boffi, M.Radici Nuclear Transparency in Quasielastic A(e, e'p): Intranuclear cascade versus eikonal approximation NUCLEAR REACTIONS C, Ca, Fe, 197Au(e, e'p), E=high; calculated nuclear transparency, related features; deduced Pauli blocking role. Comparison of intranuclear cascade, Eikonal models.
doi: 10.1103/PhysRevC.57.2618
1997BO22 Yad.Fiz. 60, No 7, 1320 (1997); Phys.Atomic Nuclei 60, 1193 (1997) S.Boffi, Ye.S.Golubeva, L.A.Kondratyuk, M.I.Krivoruchenko, E.Perazzi Density Dependence of Resonance Broadening and Shadowing Effects in Nuclear Photoabsorption NUCLEAR REACTIONS, ICPND 12C, 63Cu, 208Pb(γ, X), E ≈ 0.3-1.2 GeV; analyzed total photoabsorption σ(E); deduced Δ-mass shift mass dependence. Resonance broadening, shadowing mechanisms density dependence.
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
1997PE01 Nucl.Phys. A614, 346 (1997) Photocouplings of Nucleon Resonances with Gluon and Pion Exchange Currents NUCLEAR REACTIONS 1n, 1H(γ, π0), E=resonance; calculated photoproduction σ. Constituent quark model.
doi: 10.1016/S0375-9474(96)00433-2
1997PO01 Phys.Rev. C55, 810 (1997) A.Polls, M.Radici, S.Boffi, W.H.Dickhoff, H.Muther High-Momentum Proton Removal from 16O and the (e, e'p) Cross Section NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum. Single-hole spectral function evaluated with short-range, tensor correlations.
doi: 10.1103/PhysRevC.55.810
1996BO20 Nucl.Phys. A606, 421 (1996) S.Boffi, Ye.Golubeva, L.A.Kondratyuk, M.I.Krivoruchenko Generalized Photonuclear Sum Rule, Resonance Broadening and Shadowing Effects NUCLEAR REACTIONS U(γ, X), E ≤ 12 GeV; calculated A(effective)/A vs E, ρ, ω, φ contributions included; deduced resonance broadening, shadowing effects consistency related features.
doi: 10.1016/0375-9474(96)00193-5
1996PA06 Nucl.Phys. A598, 485 (1996) Nuclear Compton Scattering in the Δ-Resonance Region with Polarized Photons NUCLEAR REACTIONS 12C, 4He(γ, γ), E=200-500 MeV; calculated Compton scattering σ(θ) vs E, photon asymmetry. Framework of Δ-hole model.
doi: 10.1016/0375-9474(95)00502-1
1996PA32 Phys.Lett. 386B, 29 (1996) Virtual Compton Scattering Off Nuclei in the Δ-Resonance Region RADIOACTIVITY 4He; calculated virtual photon Compton scattering associated structure functions vs θγ.
doi: 10.1016/0370-2693(96)00910-0
1995BI07 Phys.Lett. 348B, 7 (1995) Quantum Interference Effects in (e, e'p) Reactions NUCLEAR REACTIONS 12C(polarized e, e'p), E not given; calculated transparency coefficient, helicity asymmetry vs momentum transfer. Longitudinally polarized beam.
doi: 10.1016/0370-2693(95)00109-X
1994BI02 Phys.Rev. C49, R1243 (1994) A.Bianconi, S.Boffi, D.E.Kharzeev Quantum Interference Effects in N(*) Electroproduction and Propagation in Nuclei NUCLEAR REACTIONS 27Al(e, e'p), E not given; calculated effective amplitudes squared vs missing momentum. Quantum interference effects in N(*) electroproduction discussed.
doi: 10.1103/PhysRevC.49.R1243
1994BI05 Phys.Lett. 325B, 294 (1994) A.Bianconi, S.Boffi, D.E.Kharzeev Asymmetry of the Missing Momentum Distribution in (e, e'p) Reactions and Color Transparency NUCLEAR REACTIONS 12C(e, e'p), E not given; calculated missing momentum distribution asymmetry vs 3-momentum transfer; deduced color transparency implications.
doi: 10.1016/0370-2693(94)90013-2
1994BI14 Yad.Fiz. 57, No 10, 1732 (1994); Phys.Atomic Nuclei 57, 1661 (1994) A.Bianconi, S.Boffi, D.E.Kharzeev Color Transparency NUCLEAR REACTIONS 27Al(e, e'p), E not given; calculated transparency coefficient vs three-momentum transfer, missing momentum. Quark-hadron duality framework.
1994MA26 Phys.Rev.Lett. 72, 3325 (1994) J.Mandeville, R.Alarcon, R.Beck, A.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, L.Cardman, J.Comfort, D.Dale, G.Dodson, S.Dolfini, K.Dow, M.Epstein, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, D.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, L.Weinstein, S.Williamson First Measurement of the Imaginary Part of the Transverse-Longitudinal Nuclear Response NUCLEAR REACTIONS 12C(polarized e, e'p), E=560 MeV; measured asymmetry, differential σ, fifth structure function; deduced direct knockout, rescattering amplitudes interference.
doi: 10.1103/PhysRevLett.72.3325
1994RA22 Phys.Rev. C50, 3010 (1994) M.Radici, S.Boffi, S.C.Pieper, V.R.Pandharipande Many-Body Effects in 16O(e, e'p) NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum. Many-body variational wave functions.
doi: 10.1103/PhysRevC.50.3010
1993BI08 Phys.Lett. 305B, 1 (1993) A.Bianconi, S.Boffi, D.E.Kharzeev Colour Transparency in Hard Nuclear Reactions. Quark versus Hadronic Dynamics NUCLEAR REACTIONS 27Al(p, 2p), E at ≤ 28 GeV/c; calculated transparency coefficients. Hadron eigenstate expansion technique.
doi: 10.1016/0370-2693(93)91095-5
1993BI18 Nucl.Phys. A565, 767 (1993) A.Bianconi, S.Boffi, D.E.Kharzeev Hadronic Dynamics of Colour Transparency NUCLEAR REACTIONS 27Al(e, e'p), E not given; calculated transparency coefficient vs momentum transfer, missing momentum. Hadronic expansion of hard scattering operator correlator.
doi: 10.1016/0375-9474(93)90003-G
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
1992BO07 Nucl.Phys. A539, 597 (1992) S.Boffi, M.Radici, J.J.Kelly, T.M.Payerle Neutron Knockout and Isobar Excitation in Quasi-Free Electron Scattering NUCLEAR REACTIONS 17O(e, e'n), (polarized e, e'n), E not given; calculated σ(θ), polarization transfer coefficient vs missing momentum; deduced two-body currents, isobar excitation roles. Neutron knockout.
doi: 10.1016/0375-9474(92)90128-7
1992GO11 Nucl.Phys. A547, 633 (1992) Mean Square Radii of Hyperons in the Bound-State Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic mean square radii. Bound state soliton model.
doi: 10.1016/0375-9474(92)90655-4
1991BO10 Nucl.Phys. A526, 602 (1991) Nuclear Response in Electromagnetic Quasi-Free Knockout Including Two-Body Currents NUCLEAR REACTIONS 16O(e, e'p), (e, e'n), E not given; calculated longitudinal, transverse structure functions. Quasifree knockout, two-body currents.
doi: 10.1016/0375-9474(91)90435-9
1991BO26 Nuovo Cim. 104A, 843 (1991) S.Boffi, L.Bracci, P.Christillin Coherent (γ, π0) on Nuclei NUCLEAR REACTIONS 12C, 40Ca, 208Pb(γ, π0), E ≈ 130-180 MeV; 16O, 40Ca, 90Zr, 208Pb(γ, π0), E=160-400 MeV; calculated coherent production σ(E). 16O(γ, π0), E=180-320 MeV; calculated σ(θ); deduced pion distortion, medium effects role.
doi: 10.1007/BF02820558
1991BO29 Nucl.Phys. A533, 441 (1991) Distortion in Two-Nucleon Photoemission NUCLEAR REACTIONS 16O(γ, np), E=200 MeV; calculated σ(θ1, θ2, E1); deduced distortions role. Final state interactions, factorized approximation.
doi: 10.1016/0375-9474(91)90527-D
1990BO17 Phys.Lett. 242B, 151 (1990) Quasi-Elastic Electron Scattering at High Momenta Beyond the Impulse Approximation NUCLEAR REACTIONS 40Ca(e, e'p), E not given; analyzed data; deduced meson exchange current, isobar configuration role.
doi: 10.1016/0370-2693(90)91452-H
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
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
1988BO40 Nucl.Phys. A490, 585 (1988) S.Boffi, O.Nicrosini, M.Radici Nuclear Charge Form Factor in the Topological Soliton Model NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated charge form factors. Topological soliton model.
doi: 10.1016/0375-9474(88)90015-2
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.
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
1986BO03 Nucl.Phys. A448, 637 (1986) Coherent π0 Photoproduction near Threshold on Closed-Shell Nuclei NUCLEAR REACTIONS 12C, 40Ca(γ, π0), E=135-185 MeV; calculated coherent pion photoproduction σ(E). 40Ca(γ, π0), E=180 MeV; 16O(γ, π0), E=150 MeV; calculated coherent pion photoproduction σ(θ).
doi: 10.1016/0375-9474(86)90434-3
1986BO44 Europhys.Lett. 2, 941 (1986) Phenomenology of (γ, π0) Reaction on Nuclei NUCLEAR REACTIONS 40Ca(γ, π0), E=180 MeV; 40Ca(π-, π-), E=44.5 MeV; calculated σ(θ). DWBA.
doi: 10.1209/0295-5075/2/12/009
1986VA17 Phys.Rev.Lett. 57, 182 (1986) G.van der Steenhoven, H.P.Blok, J.F.J.van den Brand, T.de Forest, Jr., J.W.A.den Herder, E.Jans, P.H.M.Keizer, L.Lapikas, P.J.Mulders, E.N.M.Quint, P.K.A.de Witt Huberts, J.Mougey, S.Boffi, C.Giusti, F.D.Pacati Effect of Nuclear Medium on the Proton Investigated with Reaction 12C(e, e'p)11B NUCLEAR REACTIONS 12C(e, e'p), E=312.8, 443.3 MeV; measured σ(E(e'), θ(e'), Ep', θp); deduced longitudinal, transverse response functions, medium effects.
doi: 10.1103/PhysRevLett.57.182
1985BO12 Nucl.Phys. A436, 438 (1985) S.Boffi, F.Capuzzi, C.Giusti, F.D.Pacati Charge Exchange in the Final State of Direct (γ, n) Reactions NUCLEAR REACTIONS 12C(γ, n), E=60, 80 MeV; 40Ca(γ, n), E=80 MeV; calculated σ(θ); deduced charge exchange mechanism role.
doi: 10.1016/0375-9474(85)90078-8
1985BO13 Nucl.Phys. A435, 697 (1985) Structure Functions in Nucleon Emission by Polarized Electrons NUCLEAR REACTIONS 16O(polarized e, e'p), E=500 MeV; calculated σ(θ(e'), θp); deduced fifth structure function existence possibility. Quasifree nucleon knockout.
doi: 10.1016/0375-9474(85)90182-4
1984BO18 Nucl.Phys. A420, 38 (1984) S.Boffi, R.Cenni, C.Giusti, F.D.Pacati Orthogonality, Antisymmetry and c.m. Effects in Direct Photoreactions NUCLEAR REACTIONS 12C(γ, p), (γ, n), E=40, 60, 80, 100 MeV; calculated σ(θ); deduced orthogonality, antisymmetrization, recoil effect role. PWIA, DWIA analyses.
doi: 10.1016/0375-9474(84)90655-9
1983BO28 Nuovo Cim. 76A, 685 (1983) S.Boffi, C.Giusti, F.D.Pacati, M.Rosa-Clot A Sum Rule Approach to Effective Charges in Electromagnetic Knock-Out Reactions NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E not given; calculated squared neutron, proton effective charges, ratios vs momentum transfer, θ. Quasielastic knockout, sum rule approach.
doi: 10.1007/BF02904601
1982BE02 Nucl.Phys. A375, 381 (1982) M.Bernheim, A.Bussiere, J.Mougey, D.Royer, D.Tarnowski, S.Turck-Chieze, S.Frullani, S.Boffi, C.Giusti, F.D.Pacati, G.P.Capitani, E.De Sanctis, G.J.Wagner The Influence of Bound States and Optical Potentials on 1p Momentum Distributions Obtained from 12C and 16O(e, e'p) Reactions NUCLEAR REACTIONS 12C, 16O(e, e'p), E=500 MeV; measured σ(missing energy, recoil momentum); deduced proton-hole spectral functions. Unfactorized DWIA analysis.
doi: 10.1016/0375-9474(82)90020-3
1982BO16 Nucl.Phys. A379, 509 (1982) S.Boffi, F.Cannata, F.Capuzzi, C.Giusti, F.D.Pacati Orthogonality and the Perey Factor in Knockout Reactions Induced by Electromagnetic Probes NUCLEAR REACTIONS 16O(γ, p), E=80 MeV; calculated σ(θ). Knockout reactions, channel orthogonality, optical potentials.
doi: 10.1016/0375-9474(82)90011-2
1982BO28 Nucl.Phys. A386, 599 (1982) Structure Functions in Quasi-free (e, e'p) Reactions NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated proton-hole structure functions. Quasifree scattering.
doi: 10.1016/0375-9474(82)90039-2
1981BA10 Nucl.Phys. A358, 371c (1981) P.Barreau, M.Bernheim, S.Boffi, A.Bussiere, G.P.Capitani, S.Frullani, C.Giusti, J.Mougey, J.Morgenstern, F.Pacati, D.Royer, E.De Sanctis, D.Tarnowski, S.Turck-Chieze, G.J.Wagner Improvements in the Interpretation of Quasi Free Scattering Coincidence Experiments NUCLEAR REACTIONS 16O(e, e'p), E not given; analyzed σ, e'p-coin data; calculated spectral function; deduced final state interaction effects, dependence on optical model absorption term. DWBA calculations, quasifree scattering.
doi: 10.1016/0375-9474(81)90341-9
1981BO02 Phys.Lett. B98, 11 (1981) Direct Nucleon Emission by Polarized Photons NUCLEAR REACTIONS 16O(polarized γ, p), (polarized γ, n), E=60, 80, 100 MeV; calculated σ(θ). Linearly polarized beam, direct knockout mechanism, final state distortion.
doi: 10.1016/0370-2693(81)90355-5
1981BO14 Nucl.Phys. A359, 91 (1981) Direct Mechanism in Medium Energy (γ, p0) Reactions NUCLEAR REACTIONS 16O, 12C(γ, p), E=60, 80, 100 MeV; 40Ca(γ, p), E=50-200 MeV; analyzed σ(θp, E); deduced optical potential dependence. Direct knockout mechanism.
doi: 10.1016/0375-9474(81)90213-X
1981BO38 Lett.Nuovo Cim. 32, 381 (1981) On Medium-Energy (γ, p0) Reactions at Foward Angles NUCLEAR REACTIONS 16O(γ, p), E=80 MeV; analyzed σ(θ) from different models; deduced one-body knockout mechanism validity.
doi: 10.1007/BF02745131
1980BO08 Nucl.Phys. A336, 416 (1980) Electron-Nucleon Interaction in Quasi-Free Scattering (I). Non-Relativistic Hamiltonian Through Second Order NUCLEAR REACTIONS 12C(e, e'p), (e, e'n), E=500 MeV; calculated σ(θ). Relativistic, nonrelativistic approach.
doi: 10.1016/0375-9474(80)90218-3
1980BO09 Nucl.Phys. A336, 437 (1980) Spin-Orbit Distortion of the Emerging Nucleon in Quasi-Free Electron Scattering NUCLEAR REACTIONS 12C(e, e'p), E=500 MeV; calculated σ(θ); deduced p spin-orbit distortion. Quasifree scattering.
doi: 10.1016/0375-9474(80)90220-1
1979BO07 Nucl.Phys. A319, 461 (1979) S.Boffi, C.Giusti, F.D.Pacati, S.Frullani Validity of the Factorized DWIA in (e, e'p) Reactions NUCLEAR REACTIONS 12C(e, e'p); calculated σ(θ) vs recoil momentum. Model without factorization into nondiagonal spectral function, off-shell two-body electron-nucleon scattering amplitude. Compared with DIWA.
doi: 10.1016/0375-9474(79)90526-8
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
1971BO37 Lett.Nuovo Cim. 1, 931 (1971) On the One-Particle Nuclear-Density Matrix NUCLEAR STRUCTURE 4He; calculated ground-state properties. 1-particle density matrix approach.
doi: 10.1007/BF02770150
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
1970BO40 Lett.Nuovo Cim. 4, 988 (1970) Note on the Microscopic Description of the Charge Form Factor of 4He NUCLEAR STRUCTURE 4He; calculated charge form factor.
doi: 10.1007/BF02755259
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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