NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Jeschonnek Found 26 matches. 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
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
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
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
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
2008EL08 Phys.Rev. C 78, 034002 (2008) Ch.Elster, T.Lin, W.Glockle, S.Jeschonnek Faddeev and Glauber calculations at intermediate energies in a model for n+d scattering NUCLEAR REACTIONS 2H(n, n), E=100-2000 MeV; calculated elastic scattering σ. Fadeev Glauber calculations.
doi: 10.1103/PhysRevC.78.034002
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
2006HU09 Phys.Rev. C 73, 064004 (2006) B.Hu, M.K.Jones, P.E.Ulmer, H.Arenhovel, O.K.Baker, W.Bertozzi, E.J.Brash, J.Calarco, J.-P.Chen, E.Chudakov, A.Cochran, S.Dumalski, R.Ent, J.M.Finn, F.Garibaldi, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, J.Hovdebo, C.W.de Jager, S.Jeschonnek, X.Jiang, C.Keppel, A.Klein, A.Kozlov, S.Kuhn, G.Kumbartzki, M.Kuss, J.J.LeRose, M.Liang, N.Liyanage, G.J.Lolos, P.E.C.Markowitz, D.Meekins, R.Michaels, J.Mitchell, Z.Papandreou, C.F.Perdrisat, V.Punjabi, R.Roche, D.Rowntree, A.Saha, S.Strauch, L.Todor, G.Urciuoli, L.B.Weinstein, K.Wijesooriya, B.B.Wojtsekhowski, R.Woo Polarization transfer in the 2H(e(pol), e'p(pol))n reaction up to Q2 = 1.61 (GeV/c)2 NUCLEAR REACTIONS 1,2H(polarized e, e'p), E=1.669 GeV; measured recoil proton polarization vs momentum transfer, missing momentum; deduced form factor ratios. Comparison with model predictions.
doi: 10.1103/PhysRevC.73.064004
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
2002UL01 Phys.Rev.Lett. 89, 062301 (2002) P.E.Ulmer, K.A.Aniol, H.Arenhovel, J.-P.Chen, E.Chudakov, D.Crovelli, J.M.Finn, K.G.Fissum, O.Gayou, J.Gomez, J.-O.Hansen, C.W.de Jager, S.Jeschonnek, M.K.Jones, M.Kuss, J.J.LeRose, M.Liang, R.A.Lindgren, S.Malov, D.Meekins, R.Michaels, J.Mitchell, C.F.Perdrisat, V.Punjabi, R.Roche, F.Sabatie, A.Saha, R.Suleiman, L.Todor, B.B.Wojtsekhowski 2H(e, e'p)n Reaction at High Recoil Momenta NUCLEAR REACTIONS 2H(e, e'p), E=3.110 GeV; measured Ep, σ vs recoil momentum. Comparison with model predictions.
doi: 10.1103/PhysRevLett.89.062301
2001JE02 Phys.Rev. C63, 034609 (2001) Unfactorized versus Factorized Calculations for 2H(e, e'p) Reactions at GeV Energies NUCLEAR REACTIONS 2H(e, e'p), E=high; calculated σ vs missing momentum, energy transfer. Comparison of factorized and unfactorized calculations.
doi: 10.1103/PhysRevC.63.034609
2000JE07 Prog.Part.Nucl.Phys. 44, 59 (2000) The Fifth Response Function and Spin-Orbit Final-State Interaction in the Framework of Glauber Theory for (e, e'p) Reaction
doi: 10.1016/S0146-6410(00)00057-0
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
1999JE04 Phys.Rev. C59, 2676 (1999) Spin-Orbit Final-State Interaction in the Framework of Glauber Theory for (e, e'p) Reactions NUCLEAR REACTIONS 2H(e, e'p), (polarized e, e'p), E=6 GeV; calculated σ(E, θ), polarization observables, response functions; deduced role of spin-orbit final state interaction.
doi: 10.1103/PhysRevC.59.2676
1998JE02 Phys.Rev. C57, 2438 (1998) Relativistic Effects in the Electromagnetic Current at GeV Energies NUCLEAR REACTIONS 2H(e, e'p), (polarized e, e'p), E not given; calculated response functions; deduced relativistic effects.
doi: 10.1103/PhysRevC.57.2438
1996BI02 Phys.Rev. C53, 576 (1996) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Quadrupole Deformation of Deuterons and Final-State Interaction in 2H(pol)(e, e'p) Scattering on Tensor-Polarized Deuterons at GeV Energies NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated tensor analyzing power vs θ, missing momentum; deduced final state interactions role, 2H quadrupole deformation effect. Polarized target, Glauber theory.
doi: 10.1103/PhysRevC.53.576
1996BI15 Nucl.Phys. A608, 437 (1996); Erratum Nucl.Phys. A616, 680 (1997) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Do Final-State Interactions Obscure Short-Range Correlation Effects in Quasielastic A(e, e'p) Scattering ( Question ) NUCLEAR REACTIONS 4He(e, e'p), E not given; calculated missing momentum distribution, inclusive scattering, realistic model functions; deduced final state interactions, initial state two-nucleon correlations interplay, quantum mechanical interference roles.
doi: 10.1016/S0375-9474(96)00248-5
1996JE04 Phys.Rev. C54, 2066 (1996) S.Jeschonnek, S.Krewald, A.Szczurek Final State Charge Exchange Interactions in the 12C(e, e'p) Reaction NUCLEAR REACTIONS 12C(e, e'p), E=855.1 MeV; analyzed spectral function data; deduced final state interaction, off-shell effects role. Continuum RPA, channel coupling, direct, Pauli exchange diagrams.
doi: 10.1103/PhysRevC.54.2066
1995BI04 Phys.Rev. C51, 1584 (1995) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Apparent Coulomb Reacceleration of Neutrons in Electrodissociation of the Deuteron NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated average neutron velocity shift relative to that of deuteron; deduced relation to missing momentum distribution forward-backward asymmetry, final state interaction role.
doi: 10.1103/PhysRevC.51.1584
1995BI05 Phys.Lett. 343B, 13 (1995) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Final State Interaction Effects in D(e, e'p) Scattering NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated missing momentum distribution vs θ, anisotropy; deduced final state interaction effects related features.
doi: 10.1016/0370-2693(94)01436-G
1995BI26 Phys.Lett. 363B, 217 (1995) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Universal Pattern in (e, e'p) at Large Missing Momenta: Quasi-deuteron on diffractive final state interactions ( Question ) NUCLEAR REACTIONS 4He, 2H(e, e'p), E not given; calculated missing momentum distribution, forward-backward asymmetry; deduced universality related features.
doi: 10.1016/0370-2693(95)01218-4
1994BI11 Phys.Lett. 338B, 123 (1994) A.Bianconi, S.Jeschonnek, N.N.Nikolaev, B.G.Zakharov Simple Classification of Final State Interaction Effects in 4He(e, e'p) Scattering NUCLEAR REACTIONS 4He(e, e'p), E not given; calculated missing momentum distribution, components angular dependence; deduced phase space dominated by final state interactions.
doi: 10.1016/0370-2693(94)91354-4
1994JE04 Nucl.Phys. A570, 599 (1994) S.Jeschonnek, A.Szczurek, G.Co, S.Krewald Finite-State Interaction Effects in Exclusive and Inclusive Quasi-Elastic scattering from 12C NUCLEAR REACTIONS 12C(e, e'p), (e, e'n), E not given; calculated spectral function vs missing momentum. 12C(e, e'), E not given; calculated longitudinal, transverse response functions. Final state interactions.
doi: 10.1016/0375-9474(94)90075-2
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