NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.B.Barbaro Found 73 matches. 2024FR03 Phys.Rev. D 109, 013004 (2024) J.M.Franco-Patino, S.Dolan, R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, G.D.Megias New model comparison for semi-inclusive charged-current electron and muon neutrino scattering by 40Ar in the energy range of the MicroBooNE experiment NUCLEAR REACTIONS 40Ar(ν, X), E<1.5 GeV; measured reaction products, En, In; deduced missing energy profile of neutrons, σ(θ). Comparison with the relativistic distorted wave impulse approximation (RDWIA) calculations using ED-RMF and ROP FSI models, and the SuSAν2 model implemented in GENIE.
doi: 10.1103/PhysRevD.109.013004
2022GO04 Phys.Rev. C 105, 025502 (2022) R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, N.Jachowicz, G.D.Megias, K.Niewczas, A.Nikolakopoulos, J.W.Van Orden, J.M.Udias Neutrino energy reconstruction from semi-inclusive samples NUCLEAR REACTIONS 16O(ν, μ-p)E<4061 MeV; calculated σ(θ, E) with DUNE and T2K neutrino fluxes, missing energy-missing momentum trajectories. Discussing the usefulness of semi-inclusive charged-current neutrino scattering in extracting the neutrino spectrum.
doi: 10.1103/PhysRevC.105.025502
2021FR09 Phys.Rev. D 104, 073008 (2021) J.M.Franco-Patino, M.B.Barbaro, J.A.Caballero, G.D.Megias Theoretical description of semi-inclusive T2K, MINERνA and MicroBooNE neutrino-nucleus data in the relativistic plane wave impulse approximation NUCLEAR REACTIONS 40Ar(ν, X), E not given; calculated σ. MicroBooNE data sets.
doi: 10.1103/PhysRevD.104.073008
2020AM06 J.Phys.(London) G46, 124001 (2020) J.E.Amaro, M.B.Barbaro, J.A.Caballero, R.Gonzalez-Jimenez, G.D.Megias, I.Ruiz Simo Electron- versus neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, μ-), (e-, e-'), E=1, 1.5 GeV; calculated σ(θ, E).
doi: 10.1088/1361-6471/abb128
2020FR14 Phys.Rev. C 102, 064626 (2020) J.M.Franco-Patino, J.Gonzalez-Rosa, J.A.Caballero, M.B.Barbaro Semi-inclusive charged-current neutrino-nucleus cross sections in the relativistic plane-wave impulse approximation NUCLEAR REACTIONS 12C, 40Ar(ν, ν), (ν-bar, ν-bar), E<6 GeV; calculated momentum distributions, semi-inclusive cross sections, flux-averaged single-differential and double-differential inclusive cross sections for quasielastic neutrino-nucleus scattering and corresponding to experimental data from DUNE for 40Ar and T2K for 12C. Plane-wave impulse approximation using three nuclear models: relativistic Fermi gas (RFG), independent-particle shell model (IPSM), and the natural orbitals (NO) model with Lorentzian dependence of the excitation energy. Discussed off-shell effects.
doi: 10.1103/PhysRevC.102.064626
2020GO01 Phys.Rev. C 101, 015503 (2020) R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, N.Jachowicz, G.D.Megias, K.Niewczas, A.Nikolakopoulos, J.M.Udias Constraints in modeling the quasielastic response in inclusive lepton-nucleus scattering NUCLEAR REACTIONS 12C, 40Ar, 48Ti(e, e'), momentum transfer q=100, 200, 600, 1000, 1500 MeV; calculated vector and scalar potentials as a function of the position in the nucleus, quasielastic (QE) scaling functions, differential σ(E) by superscaling approach (SuSAv2) model and relativistic mean-field models. Comparison with the recent Jefferson Laboratory (JLab) data.
doi: 10.1103/PhysRevC.101.015503
2020ME03 Phys.Rev. C 101, 025501 (2020) G.D.Megias, S.Bolognesi, M.B.Barbaro, E.Tomasi-Gustafsson New evaluation of the axial nucleon form factor from electron- and neutrino-scattering data and impact on neutrino-nucleus cross sections NUCLEAR REACTIONS 12C(ν, X), (ν-bar, X), E=0.1-100 GeV; analyzed experimental double-differential cross section data from T2K and MINERvA for nucleon form factors in the two-component model; evaluated charged-current quasielastic (CCQE) neutrino-nucleus cross-sections in the SuSAv2 nuclear model based on the relativistic mean field; discussed impact of the uncertainties on the nucleon axial form factor from pion electroproduction and neutrino-scattering data.
doi: 10.1103/PhysRevC.101.025501
2019BA15 Phys.Rev. C 99, 042501 (2019) M.B.Barbaro, J.A.Caballero, A.De Pace, T.W.Donnelly, R.Gonzalez-Jimenez, G.D.Megias Mean-field and two-body nuclear effects in inclusive electron scattering on argon, carbon, and titanium: The superscaling approach NUCLEAR REACTIONS 12C, 40Ar, 48Ti(E, E'), E=2.222 GeV; calculated double differential σ(E, θ) for quasielastic scattering, and superscaling function extracted from JLab data using superscaling (SuSAv2-MEC) model, including two-particle two-hole meson-exchange currents. Application to experimental data from MINERνA, MicroBooNE and J-PARC (T2K) collaborations.
doi: 10.1103/PhysRevC.99.042501
2019IV02 Phys.Rev. C 99, 014610 (2019) M.V.Ivanov, A.N.Antonov, G.D.Megias, J.A.Caballero, M.B.Barbaro, J.E.Amaro, I.Ruiz Simo, T.W.Donnelly, J.M.Udias Realistic spectral function model for charged-current quasielastic-like neutrino and antineutrino scattering cross sections on 12C NUCLEAR REACTIONS 12C(ν, X), (ν-bar, X), E=0-1.6 GeV muon neutrinos and antineutrinos; analyzed experimental data for double-differential, single-differential, and total integrated cross sections of charged current quasielastic (CCQE) scattering, fluxes of νμ and ν-barμ for MiniBooNE, T2K and Minerva experiments using spectral functions with and without nucleon-nucleon short-range correlations through the Jastrow method. Three different theoretical calculations using harmonic oscillator (HO), natural orbitals (NO), both including final-state interactions (FSI), and SuSAv2 based on the relativistic meanfield (RMF) model.
doi: 10.1103/PhysRevC.99.014610
2018AL24 Prog.Part.Nucl.Phys. 100, 1 (2018) L.Alvarez-Ruso, M.Sajjad Athar, M.B.Barbaro, D.Cherdack, M.E.Christy, P.Coloma, T.W.Donnelly, S.Dytman, A.de Gouvea, R.J.Hill, P.Huber, N.Jachowicz, T.Katori, A.S.Kronfeld, K.Mahn, M.Martini, J.G.Morfin, J.Nieves, G.N.Perdue, R.Petti, D.G.Richards, F.Sanchez, T.Sato, J.T.Sobczyk, G.P.Zeller NuSTEC1 White Paper: Status and challenges of neutrino-nucleus scattering
doi: 10.1016/j.ppnp.2018.01.006
2018BA35 Phys.Rev. C 98, 035501 (2018) M.B.Barbaro, A.De Pace, T.W.Donnelly, J.A.Caballero, G.D.Megias, J.W.Van Orden Asymmetric relativistic Fermi gas model for quasielastic lepton-nucleus scattering NUCLEAR REACTIONS 40Ar, 208Pb(e, e'), (ν, ν'), (ν-bar, ν-bar'), 12C, 40Ar, 208Pb(ν, μ-), (ν-bar, μ+), E(transfer)=0-500 MeV; calculated longitudinal and transverse electromagnetic, weak neutral-current, and weak charged current response functions using symmetric and asymmetric relativistic Fermi gas (SRFG and ARFG) models. Relevance to analysis of neutrino oscillation experiments.
doi: 10.1103/PhysRevC.98.035501
2017AM03 Phys.Rev. C 95, 065502 (2017) J.E.Amaro, M.B.Barbaro, J.A.Caballero, A.De Pace, T.W.Donnelly, G.D.Megias, I.Ruiz Simo Density dependence of 2p-2h meson-exchange currents
doi: 10.1103/PhysRevC.95.065502
2016SI25 Phys.Rev. C 94, 054610 (2016) I.Ruiz Simo, J.E.Amaro, M.B.Barbaro, A.De Pace, J.A.Caballero, G.D.Megias, T.W.Donnelly Emission of neutron-proton and proton-proton pairs in electron scattering induced by meson-exchange currents NUCLEAR REACTIONS 12C(e, e'np), (e, e'pp), E=961, 3595, 4621 MeV; calculated differential cross sections, transverse and longitudinal electromagnetic response functions for np and pp pair emissions using relativistic Fermi gas model with relativistic model of meson exchange currents (MECs).
doi: 10.1103/PhysRevC.94.054610
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
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
2014GO21 Phys.Rev. C 90, 035501 (2014) R.Gonzalez-Jimenez, G.D.Megias, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Extensions of superscaling from relativistic mean field theory: The SuSAv2 model
doi: 10.1103/PhysRevC.90.035501
2014IV01 Phys.Rev. C 89, 014607 (2014) M.V.Ivanov, A.N.Antonov, J.A.Caballero, G.D.Megias, M.B.Barbaro, E.Moya de Guerra, J.M.Udias Charged-current quasielastic neutrino scattering cross sections on 12C with realistic spectral and scaling functions NUCLEAR REACTIONS 12C(ν, ν), (ν-bar, ν-bar), E=0.1-100 GeV; calculated differential σ(E) for quasielastic neutrino scattering based on impulse approximation, and realistic spectral and scaling functions. Comparison with MiniBooNE and NOMAD experimental data. Discussed role of the final-state interactions.
doi: 10.1103/PhysRevC.89.014607
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
2012AM04 Phys.Rev.Lett. 108, 152501 (2012) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Meson-Exchange Currents and Quasielastic Antineutrino Cross Sections in the Superscaling Approximation
doi: 10.1103/PhysRevLett.108.152501
2012CA43 J.Phys.:Conf.Ser. 366, 012006 (2012) J.A.Caballero, J.E.Amaro, M.B.Barbaro, T.W.Donnelly, J.M.Udias Scaling ideas in neutrino scattering reactions: application to the MiniBooNE experiment NUCLEAR REACTIONS 12C(ν, μ), E=0.2-2 GeV; calculated CCQE (Charged-Current QuasiElastic) σ using RIA (Relativistic Impulse Approximation). Compared with RFG (Relativistic Fermi Gas), SuSA, SuSA+MEC and MiniBoone data.
doi: 10.1088/1742-6596/366/1/012006
2011AN09 Phys.Rev. C 83, 045504 (2011) A.N.Antonov, M.V.Ivanov, J.A.Caballero, M.B.Barbaro, J.M.Udias, E.Moya de Guerra, T.W.Donnelly Scaling function, spectral function, and nucleon momentum distribution in nuclei NUCLEAR REACTIONS 12C, 16O(e, e'), E at 1 GeV/c; analyzed σ, spectral function and momentum distribution, scaling function using different nuclear models based on the independent particle shell model with short-range nucleon correlations through the use of natural orbits (NOs) within the Jastrow method.
doi: 10.1103/PhysRevC.83.045504
2011BE45 Phys.Rev. C 84, 054315 (2011) D.Berardo, M.B.Barbaro, R.Cenni, T.W.Donnelly, A.Molinari Connecting scaling with short-range correlations
doi: 10.1103/PhysRevC.84.054315
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
2010AM01 Phys.Rev. C 81, 014606 (2010) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.Maieron, J.M.Udias Meson-exchange currents and final-state interactions in quasielastic electron scattering at high momentum transfers NUCLEAR REACTIONS 12C(e, e'), E at 1, 1.3, 1.5 GeV/c; calculated transverse response function, and effects of meson-exchange currents (MEC) using continuum semirelativistic (SR) shell model and the Dirac equation based (DEB) potential for the final states.
doi: 10.1103/PhysRevC.81.014606
2010AM06 Phys.Rev. C 82, 044601 (2010) J.E.Amaro, C.Maieron, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Pionic correlations and meson-exchange currents in two-particle emission induced by electron scattering NUCLEAR REACTIONS 56Fe(e, e'), E at 370, 410, 550, 1140 MeV/c; calculated 2p-2h transverse and longitudinal response and structure functions using relativistic Fermi gas (RFG) model. Pionic correlations.
doi: 10.1103/PhysRevC.82.044601
2010BA54 J.Phys.:Conf.Ser. 205, 012015 (2010) Nuclear effects in neutrino-nucleus interactions NUCLEAR REACTIONS 12C(ν, μ), E at 1000 MeV/c; calculated σ using charged current SuSA (superscaling approximation) and RFG (relativistic Fermi gas) with quasielastic and resonance components. 12C(ν, ν'), E=0.4-2 GeV; calculated quasielastic σ using different charged current models. 12C(ν, p), (ν, n), (ν-bar, p), (ν-bar, n), E=100-800 MeV; calculated neutral current σ(Ep, θ), σ(En, θ).
doi: 10.1088/1742-6596/205/1/012015
2010CA14 Phys.Rev. C 81, 055502 (2010) J.A.Caballero, M.B.Barbaro, A.N.Antonov, M.V.Ivanov, T.W.Donnelly Scaling function and nucleon momentum distribution NUCLEAR REACTIONS 12C(e, e'), E at 0.5-1.0 GeV/c; calculated superscaling function and nucleon momentum distribution using relativistic Fermi gas (RFG) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.055502
2009AN06 Phys.Rev. C 79, 044602 (2009) A.N.Antonov, M.V.Ivanov, M.B.Barbaro, J.A.Caballero, E.Moya de Guerra Longitudinal and transverse scaling functions within the coherent density fluctuation model. NUCLEAR REACTIONS 12C, 16O, 27Al, 56Fe, 197Au, 208Pb(e, e'), E not given; calculated longitudinal and transverse scaling functions, quasielastic scaling functions, and differential cross sections as function of energy loss in the framework of coherent density fluctuation model (CDFM). Comparison with experimental data. 12C(ν, μ-), (ν-bar, μ-), E=1 GeV; calculated differential σ using the SDFM approach.
doi: 10.1103/PhysRevC.79.044602
2009BA55 Phys.Rev. C 80, 064320 (2009) M.B.Barbaro, D.Berardo, R.Cenni, T.W.Donnelly, A.Molinari Fermion propagators in space-time
doi: 10.1103/PhysRevC.80.064320
2009MA57 Phys.Rev. C 80, 035504 (2009) C.Maieron, J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.F.Williamson Superscaling of non-quasielastic electron-nucleus scattering NUCLEAR REACTIONS 12C(e, e'), E not given; analyzed differential σ and superscaling function using superscaling model for quasielastic scattering (SSM-QE).
doi: 10.1103/PhysRevC.80.035504
2008BA33 Phys.Rev. C 78, 024602 (2008) M.B.Barbaro, R.Cenni, T.W.Donnelly, A.Molinari Model for BCS-type correlations in superscaling
doi: 10.1103/PhysRevC.78.024602
2008IV01 Phys.Rev. C 77, 034612 (2008) M.V.Ivanov, M.B.Barbaro, J.A.Caballero, A.N.Antonov, E.Moya de Guerra, M.K.Gaidarov Superscaling and charge-changing neutrino scattering from nuclei in the Δ region beyond the relativistic Fermi gas model NUCLEAR REACTIONS 12C(ν, μ-), E=1, 1.5 GeV; 12C(ν-bar, μ+), E=1 GeV; calculated coherent density fluctuation model scaling functions, σ.
doi: 10.1103/PhysRevC.77.034612
2007AM01 Phys.Rev. C 75, 034613 (2007) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, J.M.Udias Final-state interactions and superscaling in the semi-relativistic approach to quasielastic electron and neutrino scattering NUCLEAR REACTIONS 12C(e, e'), E=high; calculated longitudinal and transverse scaling functions, final state interaction effects. 12C(ν, μ), E=1, 1.5 GeV; calculated σ(E, θ). Semi-relativistic approach.
doi: 10.1103/PhysRevC.75.034613
2007AM05 Phys.Rev.Lett. 98, 242501 (2007) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Quasielastic Charged-Current Neutrino-Nucleus Scattering NUCLEAR REACTIONS 12C(ν, μ-), E=0.5, 1.0, 1.5 GeV; calculated integrated cross sections for quasielastic charged-current neutrino-nucleus scattering.
doi: 10.1103/PhysRevLett.98.242501
2007AN17 Phys.Rev. C 75, 064617 (2007) A.N.Antonov, M.V.Ivanov, M.B.Barbaro, J.A.Caballero, E.Moya de Guerra, M.K.Gaidarov Superscaling and neutral current quasielastic neutrino-nucleus scattering beyond the relativistic Fermi gas model
doi: 10.1103/PhysRevC.75.064617
2006AM02 Phys.Rev. C 73, 035503 (2006) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Superscaling and neutral current quasielastic neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, ν'pX), (ν, ν'nX), E=1 GeV; calculated σ(E, θ), response functions, strangeness contribution.
doi: 10.1103/PhysRevC.73.035503
2006AN29 Phys.Rev. C 74, 054603 (2006) A.N.Antonov, M.V.Ivanov, M.K.Gaidarov, E.Moya de Guerra, J.A.Caballero, M.B.Barbaro, J.M.Udias, P.Sarriguren Superscaling analysis of inclusive electron scattering and its extension to charge-changing neutrino-nucleus cross sections beyond the relativistic Fermi gas approach NUCLEAR REACTIONS 12C(e, e'X), E ≈ 0.5-2 GeV; calculated σ(E, θ), scaling functions. Superscaling analysis, coherent density fluctuation model, relativistic Fermi gas model.
doi: 10.1103/PhysRevC.74.054603
2006BA17 Nucl.Phys. B(Proc.Supp.) S155, 257 (2006) M.B.Barbaro, J.E.Amaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Superscaling and Charge-changing Neutrino Cross Sections NUCLEAR REACTIONS 12C(ν, μ-), E at 1000 MeV/c; calculated σ(E, θ).
doi: 10.1016/j.nuclphysbps.2006.02.065
2006BA62 Nucl.Phys. B(Proc.Supp.) S159, 186 (2006) Superscaling in electron- and neutrino-nucleus scattering NUCLEAR REACTIONS 12C(e, e'), E=1299, 1500 MeV; 16O(e, e'), E=880 MeV; 12C(ν, μ-), (ν, pX), E=1 GeV; calculated σ(E, θ).
doi: 10.1016/j.nuclphysbps.2006.08.071
2005AM03 Phys.Rev. C 71, 015501 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Using electron scattering superscaling to predict charge-changing neutrino cross sections in nuclei NUCLEAR REACTIONS 12C(e, e'), E=1.3, 1.5 GeV; 16O(e, e'), E=0.88 GeV; analyzed σ(E, θ); deduced electromagnetic response. 12C(ν, μ), E=1 GeV; calculated σ(E, θ). Superscaling analysis.
doi: 10.1103/PhysRevC.71.015501
2005AM09 Phys.Rev. C 71, 065501 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.Maieron Semirelativistic description of quasielastic neutrino reactions and superscaling in a continuum shell model NUCLEAR REACTIONS 12C, 16O(ν, μ-), E=1, 1.5 GeV; calculated σ(E, θ), response functions, scaling and superscaling behaviors.
doi: 10.1103/PhysRevC.71.065501
2005AM10 Ann.Phys.(New York) 319, 123 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero Skewed recoil polarization in (e, e'p) reactions from polarized nuclei NUCLEAR REACTIONS 39K(polarized e, e'p), E not given; calculated polarization asymmetries, polarization transfer, related observables. Polarized target.
doi: 10.1016/j.aop.2005.03.004
2005BA79 Eur.Phys.J. A 25, 299 (2005) M.B.Barbaro, R.Cenni, M.R.Quaglia The generalised relativistic Lindhard functions
doi: 10.1140/epja/i2005-10105-4
2005CA54 Phys.Rev.Lett. 95, 252502 (2005) J.A.Caballero, J.E.Amaro, M.B.Barbaro, T.W.Donnelly, C.Maieron, J.M.Udias Superscaling in Charged Current Neutrino Quasielastic Scattering in the Relativistic Impulse Approximation NUCLEAR REACTIONS 12C, 16O(ν, μ-), E=1-2 GeV; calculated σ(E, θ), scaling functions. Relativistic impulse approximation.
doi: 10.1103/PhysRevLett.95.252502
2004BA82 Phys.Rev. C 70, 034309 (2004) M.B.Barbaro, A.Molinari, F.Palumbo, M.R.Quaglia Goldstone bosons in the pairing Hamiltonian: The path integral approach
doi: 10.1103/PhysRevC.70.034309
2004BB01 Eur.Phys.J. A 22, 377 (2004) M.B.Barbaro, R.Cenni, A.Molinari, M.R.Quaglia The many levels pairing Hamiltonian for two pairs
doi: 10.1140/epja/i2004-10043-7
2003AL20 Nucl.Phys. A724, 157 (2003) L.Alvarez-Ruso, M.B.Barbaro, T.W.Donnelly, A.Molinari Nuclear response functions for the N-N*(1440) transition NUCLEAR REACTIONS 12C(e, e'X), E=high; calculated parity-conserving and parity-violating response functions for resonance production.
doi: 10.1016/S0375-9474(03)01480-5
2003AM05 Nucl.Phys. A723, 181 (2003) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Delta-isobar relativistic meson exchange currents in quasielastic electron scattering
doi: 10.1016/S0375-9474(03)01269-7
2003AM06 Phys.Rev. C 68, 014604 (2003) J.E.Amaro, M.B.Barbaro, J.A.Caballero, F.K.Tabatabaei Semirelativistic meson-exchange currents in (e, e') and (e, e'p) reactions NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions, asymmetries. Semirelativistic meson-exchange currents.
doi: 10.1103/PhysRevC.68.014604
2002AM01 Nucl.Phys. A697, 388 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Pionic Effects in Quasielastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated transverse and longitudinal response functions; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01253-2
2002AM09 Eur.Phys.J. A 15, 421 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Momentum distribution of relativistic nuclei with Hartree-Fock mesonic correlations
doi: 10.1140/epja/i2002-10080-2
2002AM12 Phys.Rep. 368, 317 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Gauge and Lorentz invariant one-pion exchange currents in electron scattering from a relativistic Fermi gas
doi: 10.1016/S0370-1573(02)00195-3
2001AL05 Phys.Lett. 497B, 214 (2001) L.Alvarez-Ruso, M.B.Barbaro, T.W.Donnelly, A.Molinari Influence of Nucleonic Motion in Relativistic Fermi Gas Inclusive Responses NUCLEAR STRUCTURE 12C; calculated response functions for electron scattering. Relativistic Fermi gas.
doi: 10.1016/S0370-2693(00)01332-0
2001BA56 Phys.Rev. C64, 011302 (2001) M.B.Barbaro, L.Fortunato, A.Molinari, M.R.Quaglia Pairing Hamiltonian for One Pair of Identical Nucleons Bound in a Potential Well
doi: 10.1103/PhysRevC.64.011302
1999AL16 Nucl.Phys. A651, 277 (1999) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias Strange Form Factors of the Proton: A new analysis of the ν(ν-bar) data of the BNL-734 experiment
doi: 10.1016/S0375-9474(99)00142-6
1999AM10 Nucl.Phys. A657, 161 (1999) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Nuclear Responses in the Quasi-Elastic Delta Region NUCLEAR REACTIONS 1H(e, e'), E(cm)=1100-1400 MeV; calculated transverse σ. 12C(e, e'X), E=620, 1108 MeV; calculated σ(θ), electromagnetic response functions; deduced resonance role. Relativistic Fermi Gas model.
doi: 10.1016/S0375-9474(99)00334-6
1998AL28 Phys.Lett. 438B, 9 (1998) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias The Ratio of p and n Yields in NC ν(ν-bar) Nucleus Scattering and Strange Form Factors of the Nucleon
doi: 10.1016/S0370-2693(98)01043-0
1998AM11 Nucl.Phys. A643, 349 (1998) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Meson-Exchange Currents for One-Particle Emission Reactions
doi: 10.1016/S0375-9474(98)00569-7
1998BA94 Nucl.Phys. A643, 137 (1998) M.B.Barbaro, R.Cenni, A.De Pace, T.W.Donnelly, A.Molinari Relativistic y-Scaling and the Coulomb Sum Rule in Nuclei
doi: 10.1016/S0375-9474(98)00443-6
1997AL21 Nucl.Phys. A623, 471 (1997) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias Inelastic ν and (ν-bar) Scattering on Nuclei and ' Strangeness ' of the Nucleon NUCLEAR REACTIONS 12C(ν, ν'X), (ν-bar, ν-bar'X), E=200-1000 GeV; calculated differential σ vs ejected nucleon energy, proton to neutron production ratio, asymmetry related quantity; deduced nucleon strangeness role. Shell, Fermi gas models.
doi: 10.1016/S0375-9474(97)00416-8
1996AM03 Phys.Rev. C53, 2801 (1996) P.Amore, M.B.Barbaro, A.De Pace Relativistic Hamiltonians in Many-Body Theories
doi: 10.1103/PhysRevC.53.2801
1996BA07 Nucl.Phys. A596, 553 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari The Charge Response of a Meson-Correlated Relativistic Fermi Gas
doi: 10.1016/0375-9474(95)00424-6
1996BA09 Nucl.Phys. A598, 503 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari Parity-Violating Longitudinal Response NUCLEAR REACTIONS 12C(e, e'X), E not given; calculated longitudinal quasielastic parity-violating response. Anti-symmetrized RPA-HF correlations, relativistic Fermi gas basis.
doi: 10.1016/S0375-9474(96)00010-3
1996BA59 Phys.Rev. C54, 1954 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari, M.J.Musolf Probing Nucleon Strangeness with Neutrinos: Nuclear model dependences
doi: 10.1103/PhysRevC.54.1954
1994BA14 Nucl.Phys. A569, 701 (1994) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari Parity-Violating Electron Scattering from the Pion-Correlated Relativistic Fermi Gas
doi: 10.1016/0375-9474(94)90381-6
1993AL05 J.Phys.(London) G19, 403 (1993) J.S.Al-Khalili, M.B.Barbaro, C.Wilkin An Analysis of Eta-Production via the p6Li → (Eta)7Be Reaction NUCLEAR REACTIONS 6Li(p, π+), E=201-800 MeV; 6Li(p, d), E=698 MeV; 7Li(p, d), E=800 MeV; analyzed data; deduced empirical form factors, extrapolation to eta-production point in 6Li+p reaction. Semi-phenomenological model.
doi: 10.1088/0954-3899/19/3/008
1993AL07 Phys.Lett. 303B, 5 (1993) W.M.Alberico, M.B.Barbaro, A.De Pace, A.Molinari Parity-Violating Experiments Using the Quasi-Elastic Electron and Positron Scattering NUCLEAR REACTIONS 12C(polarized e-, e-), (polarized e+, e+), E not given; calculated asymmetry vs energy transfer; deduced parity violation measurement feasibility conditions. Relativistic Fermi gas model.
doi: 10.1016/0370-2693(93)90034-F
1993AL20 Nucl.Phys. A563, 605 (1993) W.M.Alberico, M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari The Pion in Electromagnetic and Weak Neutral-Current Nuclear Response Functions NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal, transverse response functions; deduced pionic correlations, meson exchange current role. Weak neutral current, Hartree-Fock, RPA, infinite order summation schemes.
doi: 10.1016/0375-9474(93)90057-5
1992DO05 Nucl.Phys. A541, 525 (1992) T.W.Donnelly, M.J.Musolf, W.M.Alberico, M.B.Barbaro, A.De Pace, A.Molinari Parity-Violating Quasielastic Electron Scattering NUCLEAR REACTIONS 12C(e, e'X), E not given; calculated response functions, asymmetry. Parity-violating quasielastic electron scattering, relativistic Fermi gas model.
doi: 10.1016/0375-9474(92)90220-E
1991CA15 Nucl.Phys. A529, 653 (1991) J.Carbonell, M.B.Barbaro, C.Wilkin Deuteron Analysing Powers in the Charge Exchange Reaction d(pol)p → (pp)n NUCLEAR REACTIONS 1H(polarized d, 2p), E=200 MeV; calculated differential σ, analyzing power. Impulse approximation.
doi: 10.1016/0375-9474(91)90590-3
1989BA15 J.Phys.(London) G15, L69 (1989) Spin Correlation Parameters in the d(pol)p(pol) → (pp)n Reaction NUCLEAR REACTIONS 1H(polarized d, 2p), E=515 MeV; 1H(polarized n, n), E=515 MeV; calculated spin correlation parameter. Polarized target.
doi: 10.1088/0954-3899/15/5/002
1988AL34 Ann.Phys.(New York) 187, 79 (1988) W.M.Alberico, M.B.Barbaro, A.Bottino, A.Molinari The 2ν Double Beta Decay in Nuclear Matter RADIOACTIVITY 76Ge, 82Se, 130Te, 136Xe(2β); calculated 2ν-accompanied decay Gamow-Teller matrix element.
doi: 10.1016/0003-4916(88)90281-3
1987AL19 Europhys.Lett. 4, 415 (1987) On the Semi-Classical Charge Longitudinal Response in 12C and 40Ca NUCLEAR REACTIONS 12C, 40Ca(e, e'), E not given; calculated charge longitudinal response functions. Semi-classical RPA.
doi: 10.1209/0295-5075/4/4/006
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