NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.W.Van Orden Found 36 matches. 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
2020JE03 Phys.Rev. C 101, 064621 (2020) S.Jeschonnek, J.W.Van Orden, T.W.Donnelly Neutral-current neutrino scattering from the deuteron NUCLEAR REACTIONS 2H(ν, ν), E=few GeV; calculated double-differential σ(E) for neutral current neutrino scattering off both single and both nucleons in deuterium, isospin asymmetry Aν; deduced final hadronic states containing only a proton and neutron, sensitivity of cross sections to the isoscalar axial-vector form factor and magnetic strangeness form factor. Lorentz covariant model with relativistic dynamics. Relevance to new ways of testing the standard model by comparisons with other reactions, such as charge-changing neutrino reactions and parity-conserving and parity-violating electron scattering reactions.
doi: 10.1103/PhysRevC.101.064621
2019VA11 Phys.Rev. C 100, 044620 (2019) Nuclear theory and event generators for charge-changing neutrino reactions NUCLEAR REACTIONS 16O(ν, μ)16F, E=0-3 GeV; calculated charge-changing muon neutrino (CCν) cross sections for spectral function models arising from simple independent-particle shell-model calculation, the relativistic Fermi gas, a local density approximation based on the RFG, and the realistic Rome spectral function. Results indicate that there may be simple kinematical descriptions of the average neutrino energy which is common to all of these models.
doi: 10.1103/PhysRevC.100.044620
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
2017JE02 Phys.Rev. C 95, 044001 (2017) Factorization breaking of ATd for polarized deuteron targets in a relativistic framework NUCLEAR REACTIONS 2H(e, e'p), Q2=2.4, 4.25 GeV2; calculated factorization of the tensor asymmetry ATd measured for polarized deuteron targets within a relativistic framework; discussed differences between PWIA and PWBA calculations.
doi: 10.1103/PhysRevC.95.044001
2017VA32 Phys.Rev. D 96, 113008 (2017) J.W.Van Orden, T.W.Donnelly, O.Moreno Coincidence charged-current neutrino-induced deuteron disintegration for 2H2 16O
doi: 10.1103/PhysRevD.96.113008
2016MA09 J.Phys.(London) G43, 023002 (2016) L.E.Marcucci, F.Gross, M.T.Pena, M.Piarulli, R.Schiavilla, I.Sick, A.Stadler, J.W.Van Orden, M.Viviani Electromagnetic structure of few-nucleon ground states NUCLEAR REACTIONS 2,3H, 3,4He(E, E), E not given; analyzed available data; deduced experimental form factors of the hydrogen and helium isotopes, extracted from an up-to-date global analysis of σ and polarization observables measured in elastic electron scattering from these systems.
doi: 10.1088/0954-3899/43/2/023002
2014FO08 Phys.Rev. C 89, 034004 (2014) W.P.Ford, R.Schiavilla, J.W.Van Orden The 3He(e, e'p) 2H and 4He(e, e'p)3H reactions at high momentum transfer NUCLEAR REACTIONS 3He(e, e'p), 4He(e, e'p), (polarized e, e'p), at 0-1200 MeV/c; calculated differential σ(momentum transfer), longitudinal transverse asymmetry, induced polarization for 4He in (polarized e, e' polarized proton). Plane-wave impulse approximation (PWIA) with the full single and double rescattering Glauber approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.034004
2014FO19 Phys.Rev. C 90, 064006 (2014) W.P.Ford, S.Jeschonnek, J.W.Van Orden Momentum distributions for 2H(e, e'p) NUCLEAR REACTIONS 2H(e, e'p), Q2=4.25 GeV2; calculated momentum density distributions, comparison of three different parametrizations of electric and magnetic form factors of the proton and neutron, plane wave impulse approximation (PWIA) cross sections, Ratio of final state interactions (FSI) to PWIA cross sections. Bethe-Salpeter-like formalism with a wide variety of bound state wave functions, form factors, and final state interactions.
doi: 10.1103/PhysRevC.90.064006
2013FO02 Phys.Rev. C 87, 014004 (2013) Regge model for nucleon-nucleon spin-dependent amplitudes
doi: 10.1103/PhysRevC.87.014004
2013FO15 Phys.Rev. C 87, 054006 (2013) W.P.Ford, S.Jeschonnek, J.W.Van Orden 2H(e, e'p) observables using a Regge model parametrization of final-state interactions
doi: 10.1103/PhysRevC.87.054006
2013FO28 Phys.Rev. C 88, 054004 (2013) Off-shell extrapolation of Regge-model NN-scattering amplitudes describing final-state interactions in 2H(e, e'p)
doi: 10.1103/PhysRevC.88.054004
2011JE01 Few-Body Systems 49, 65 (2011) Exclusive Scattering from Unpolarized and Polarized Deuteron
doi: 10.1007/s00601-010-0109-5
2010JE01 Phys.Rev. C 81, 014008 (2010) Ejectile polarization for 2H(e, e'p(pol))n at GeV energies NUCLEAR REACTIONS 2H(e, e'p)n, E=5.5 GeV; calculated asymmetries relevant to a polarized ejectile proton in various frames using fully relativistic calculation in impulse approximation.
doi: 10.1103/PhysRevC.81.014008
2009JE04 Phys.Rev. C 80, 054001 (2009) Target polarization for 2H(pol)(e, e'p)n at GeV energies
doi: 10.1103/PhysRevC.80.054001
2008JE04 Phys.Rev. C 78, 014007 (2008) New calculation for 2H(e, e'p)n at GeV energies NUCLEAR REACTIONS 2H(e, e'p)n, E=1.0, 1.1, 1.2, 5.5 GeV; calculated σ(θ), asymmetry. Impulse equation.
doi: 10.1103/PhysRevC.78.014007
2006VA14 Phys.Rev. C 74, 034607 (2006) Conserved electromagnetic currents in a relativistic optical model
doi: 10.1103/PhysRevC.74.034607
2005AD07 Phys.Rev. C 71, 034003 (2005) Comprehensive treatment of electromagnetic interactions and three-body spectator equations
doi: 10.1103/PhysRevC.71.034003
2003VA09 Eur.Phys.J. A 17, 391 (2003) Energy-weighted sum rules, y-scaling and duality
doi: 10.1140/epja/i2002-10182-9
2002AD26 Phys.Rev. C66, 044003 (2002) J.Adam, Jr., F.Gross, S.Jeschonnek, P.Ulmer, J.W.Van Orden Covariant description of inelastic electron-deuteron scattering: Predictions of the relativistic impulse approximation NUCLEAR REACTIONS 2H(e, e'p), E=high; calculated coincidence σ(E, θ), asymmetry. Covariant spectator theory, transversity formalism, relativistic impulse approximation.
doi: 10.1103/PhysRevC.66.044003
2000JE12 Phys.Rev. C62, 044613 (2000) Origin of Relativistic Effects in the Reaction 2H(e, e'p)n at GeV Energies NUCLEAR REACTIONS 2H(e, e'p), E=high; calculated σ(E, θ); deduced origin of relativistic effects.
doi: 10.1103/PhysRevC.62.044613
1998AD22 Nucl.Phys. A640, 391 (1998) J.Adam, Jr., J.W.Van Orden, F.Gross Electromagnetic Interactions for the Two-Body Spectator Equations
doi: 10.1016/S0375-9474(98)00430-8
1997AD10 Phys.Rev. C56, 641 (1997) J.Adam, Jr., F.Gross, C.Savkli, J.W.Van Orden Normalization of the Covariant Three-Body Bound State Vertex Function
doi: 10.1103/PhysRevC.56.641
1995VA28 Phys.Rev.Lett. 75, 4369 (1995) J.W.Van Orden, N.Devine, F.Gross Elastic Electron Scattering from the Deuteron Using the Gross Equation NUCLEAR REACTIONS 2H(e, e), E not given; calculated electromagnetic form factors. Gross, spectator equation, one-boson exchange model.
doi: 10.1103/PhysRevLett.75.4369
1992GR05 Phys.Rev. C45, 2094 (1992) F.Gross, J.W.Van Orden, K.Holinde Relativistic One-Boson-Exchange Model for the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(n, n), E ≤ 300 MeV; calculated phase shifts vs E. Relativistic one-boson exchange model. NUCLEAR STRUCTURE 2H; calculated S-, D-wave functions. Relativistic one-boson exchange model.
doi: 10.1103/PhysRevC.45.2094
1991BO04 Phys.Rev. C43, 582 (1991) Many-Body Correlation Effects on the Longitudinal Response in the Quasielastic (e, e') Reaction NUCLEAR REACTIONS 40Ca(e, e'), E ≤ 500 MeV; calculated longitudinal response function; deduced many-body correlations role.
doi: 10.1103/PhysRevC.43.582
1989CH25 Phys.Rev. C40, 790 (1989) C.R.Chinn, A.Picklesimer, J.W.van Orden Final-State Interactions and Relativistic Effects in the Quasielastic (e, e') Reaction NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated longitudinal, transverse response functions. Final state interactions, relativistic effects.
doi: 10.1103/PhysRevC.40.790
1989CH33 Phys.Rev. C40, 1159 (1989) C.R.Chinn, A.Picklesimer, J.W.Van Orden Quasielastic (e, e') Sum Rule Saturation NUCLEAR REACTIONS 40Ca(e, e'X), E not given; calculated Coulomb sum rule saturation. Microscopic Green's function doorway formalism.
doi: 10.1103/PhysRevC.40.1159
1989DO05 Nucl.Phys. A494, 365 (1989) T.W.Donnelly, E.L.Kronenberg, J.W.Van Orden Models for Relativistic Coulomb Sum Rules: Expansions in moments of the nuclear momentum density NUCLEAR STRUCTURE 16O; calculated Coulomb sum rules. Relativistic models, different momentum distributions.
doi: 10.1016/0375-9474(89)90183-8
1989PI07 Phys.Rev. C40, 290 (1989) Polarization Response Functions and the (e(pol), e'p(pol)) Reaction NUCLEAR REACTIONS 16O(polarized e, e'p), E=135 MeV; calculated longitudinal, transverse response functions. Polarized nucleon, relativistic, nonrelativistic treatments.
doi: 10.1103/PhysRevC.40.290
1987CO26 Phys.Rev.Lett. 59, 1267 (1987) T.D.Cohen, J.W.Van Orden, A.Picklesimer Medium-Modified Form Factors, Relativistic Dynamics, and the (e, e'p) Reaction NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated transverse to longitudinal response function ratio. DWIA.
doi: 10.1103/PhysRevLett.59.1267
1987DO03 Phys.Rev. C35, 1637 (1987) G.Do Dang, M.L'Huillier, Nguyen Van Giai, J.W.Van Orden Coulomb Sum Rules in the Relativistic Fermi Gas Model NUCLEAR REACTIONS 40Ca(e, e'), E at 550 MeV/c; calculated longitudinal response function. Coulomb sum rule.
doi: 10.1103/PhysRevC.35.1637
1985PI10 Phys.Rev. C32, 1312 (1985) A.Picklesimer, J.W.Van Orden, S.J.Wallace Final State Interactions and Relativistic Effects in the (e(pol), e'p) Reaction NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions for Ep=135 MeV. Relativistic effects, final state interactions, DWIA.
doi: 10.1103/PhysRevC.32.1312
1981VA08 Ann.Phys.(New York) 131, 451 (1981) Mesonic Processes in Deep-Inelastic Electron Scattering from Nuclei NUCLEAR REACTIONS 12C, Ni, 208Pb(e, e'), E=500 MeV; calculated σ(θ, E(e')); 12C(e, π), E=500 MeV; calculated pion production σ. Meson exchange currents, deep inelastic scattering, Fermi gas model.
doi: 10.1016/0003-4916(81)90038-5
1980AL12 Phys.Rev.Lett. 44, 1579 (1980) Y.Alexander, J.W.Van Orden, E.F.Redish, S.J.Wallace Do Quasifree Reaction Mechanisms Explain Reaction Cross Sections in Intermediate-Energy Proton-Nucleus Scattering < Question > NUCLEAR REACTIONS 12C(p, p'), E=800 MeV; calculated inclusive proton spectra. PWIA, quasifree nucleon knockout, isobar production.
doi: 10.1103/PhysRevLett.44.1579
1980VA07 Phys.Rev. C21, 2628 (1980) J.W.Van Orden, W.Truex, M.K.Banerjee Short-Range Correlations and the Nuclear Momentum Density Distribution for 16O NUCLEAR STRUCTURE 16O; calculated momentum density distribution. Brueckner method, finite nuclei, Reid soft core, Sprung potentials.
doi: 10.1103/PhysRevC.21.2628
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