NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Radici Found 39 matches. 2016PI09 Eur.Phys.J. A 52, 155 (2016) Di-hadron fragmentation and mapping of the nucleon structure
doi: 10.1140/epja/i2016-16155-5
2010BA50 Eur.Phys.J. A 45, 373 (2010) A.Bacchetta, M.Radici, F.Conti, M.Guagnelli Weighted azimuthal asymmetries in a diquark spectator model
doi: 10.1140/epja/i2010-11016-y
2006BI02 Phys.Rev. D 73, 034018 (2006) Monte Carlo simulation of the Sivers effect in high-energy proton-proton collisions NUCLEAR REACTIONS 1H(polarized p, μ+μ-X), E(cm)=200 GeV; calculated muon pair invariant mass spectra, σ, polarization observables. Monte Carlo simulation, Sivers effect.
doi: 10.1103/PhysRevD.73.034018
2006BI07 Phys.Rev. D 73, 114002 (2006) Monte Carlo simulation of single spin asymmetries in pion-proton collisions NUCLEAR REACTIONS 1H(π+, μ+μ-X), (π-, μ+μ-X), E(cm) ≈ 10, 14 GeV; calculated asymmetries for polarized target, Sivers and Boer-Mulders effects. Monte Carlo approach.
doi: 10.1103/PhysRevD.73.114002
2006BI12 Phys.Rev. D 74, 034009 (2006) A.Bianconi, B.Pasquini, M.Radici Extraction of proton form factors in the timelike region from unpolarized e+e- → p(p-bar) events
doi: 10.1103/PhysRevD.74.034009
2006BI15 Phys.Rev. D 74, 074012 (2006) A.Bianconi, B.Pasquini, M.Radici Extraction of proton form factors in the timelike region from single-polarized e+ e- → p(pol) p-bar events
doi: 10.1103/PhysRevD.74.074012
2005BI13 J.Phys.(London) G31, 645 (2005) Azimuthal asymmetries in unpolarized Drell-Yan events on nuclear targets
doi: 10.1088/0954-3899/31/7/010
2003RA16 Eur.Phys.J. A 17, 65 (2003) M.Radici, A.Meucci, W.H.Dickhoff Spectroscopic information from different theoretical descriptions of (un)polarized (e, e'p) reactions NUCLEAR REACTIONS 16O(e, e'p), (polarized e, e'p), E=high; analyzed σ(E, θ), polarization observables; deduced spectroscopic parameters. Two theoretical approaches considered.
doi: 10.1140/epja/i2002-10137-2
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
2002RA06 Nucl.Phys. A699, 144c (2002) T-Odd Fragmentation Functions
doi: 10.1016/S0375-9474(01)01483-X
2002RA35 Phys.Rev. C66, 014613 (2002) M.Radici, W.H.Dickhoff, E.Roth Stoddard Consistency of Spectroscopic Factors from (e, e'p) Reactions at Different Momentum Transfers NUCLEAR REACTIONS 16O(e, e'p), E=90 MeV; analyzed σ(E, θ), asymmetry, structure functions; deduced spectroscopic factors.
doi: 10.1103/PhysRevC.66.014613
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
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
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
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
1997BI06 Phys.Rev. C56, 1002 (1997) Helicity Asymmetry for Proton Emission from Polarized Electrons in the Eikonal Regime NUCLEAR REACTIONS 12C(polarized e, e'p), E=high; calculated helicity asymmetry vs momentum transfer; deduced nuclear response components, scaling behaviour at large momentum transfer.
doi: 10.1103/PhysRevC.56.1002
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
1996BI01 Phys.Rev. C53, R563 (1996) (e, e'p) Reaction and the Transition to the Eikonal Regime NUCLEAR REACTIONS 12C(e, e'p), E not given; analyzed distorted spectral density; deduced models reliability related features.
doi: 10.1103/PhysRevC.53.R563
1996BI21 Phys.Rev. C54, 3117 (1996) Angular Distributions for Knockout and Scattering of Protons in the Eikonal Approximation NUCLEAR REACTIONS 12C(e, e'p), E not given; calculated distorted spectral density. Eikonal approximation.
doi: 10.1103/PhysRevC.54.3117
1995BI19 Phys.Lett. 363B, 24 (1995) A Test of the Eikonal Approximation in High-Energy (e, e'p) Scattering NUCLEAR REACTIONS 12C(e, e'p), E not given; calculated distorted spectral density vs proton momentum. Eikonal approximation test.
doi: 10.1016/0370-2693(95)01219-G
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
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
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
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
1991PA06 Phys.Lett. 257B, 263 (1991) Polarization Observables and Asymmetry in Electromagnetic Quasi-Free Proton Knockout NUCLEAR REACTIONS 16O(e, e'p), E=700 MeV; calculated ep-coin, polarized proton. Unpolarized target, one photon exchange approximation.
doi: 10.1016/0370-2693(91)91890-8
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
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
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
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