NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Schwamb Found 24 matches. 2016MA64 Eur.Phys.J. A 52, 298 (2016) M.Makek, P.Achenbach, C.Ayerbe Gayoso, C.Barbieri, J.C.Bernauer, R.Bohm, D.Bosnar, A.Denig, M.O.Distler, I.Friscic, C.Giusti, H.Merkel, U.Muller, L.Nungesser, J.Pochodzalla, S.Sanches Majos, B.S.Schlimme, M.Schwamb, Th.Walcher, for the A1 Collaboration Differential cross section measurement of the 12C(e, e'pp)10Beg.s. reaction NUCLEAR REACTIONS 12C(e, e'pp)10Begs, E=163 MeV; measured Ep, Ip using Si detectors and Ie, Ip using high-resolution magnetic spectrometers, pp-coin, ep-coin; deduced σ(E, θ). 10Be deduced excitation energy spectrum after triple coin; calculated σ(E, θ) using Pavia reaction code.
doi: 10.1140/epja/i2016-16298-3
2010AH02 Eur.Phys.J. A 44, 189 (2010) J.Ahrens, S.Altieri, J.R.M.Annand, H.-J.Arends, R.Beck, M.A.Blackston, C.Bradtke, A.Braghieri, N.d'Hose, H.Dutz, A.Fix, E.Heid, O.Jahn, F.Klein, R.Kondratiev, M.Lang, V.Lisin, M.Martinez-Fabregate, J.C.McGeorge, W.Meyer, A.Panzeri, P.Pedroni, T.Pinelli, D.Protopopescu, G.Reicherz, Ch.Rohlof, G.Rosner, T.Rostomyan, D.Ryckbosch, M.Schwamb, G.Tamas, A.Thomas, H.R.Weller, Helicity dependence of the γd → πNN reactions in the Δ -resonance region NUCLEAR REACTIONS 2H(γ, πX), E=301-455 MeV; 2H(polarized γ, πX), E=307-451 MeV; measured yields, σ(θ), helicity-dependent σ(θ) with polarized beam; deduced reaction mechanism features. Comparison with other data and various models.
doi: 10.1140/epja/i2010-10946-6
2010MI11 Eur.Phys.J. A 43, 137 (2010) D.G.Middleton, J.R.M.Annand, C.Barbieri, C.Giusti, P.Grabmayr, T.Hehl, I.J.D.MacGregor, I.Martin, J.C.McGeorge, F.Moschini, F.D.Pacati, M.Schwamb, D.Watts Knockout of proton-neutron pairs from 16O with electromagnetic probes NUCLEAR REACTIONS 16O(e, e'np)14N, E=215 MeV; 16O(γ, pn)14N, E=100-800 MeV; measured reaction products; deduced σ. Comparison with Pavia model of two-nucleon knockout predictions.
doi: 10.1140/epja/i2009-10902-7
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
2006SC23 Eur.Phys.J. A 28, Supplement 1, 39 (2006) Few-nucleon systems (theory)
doi: 10.1140/epja/i2006-09-005-6
2005AN11 Eur.Phys.J. A 24, 361 (2005) D.Andreasi, W.Leidemann, C.Reiss, M.Schwamb New inversion methods for the Lorentz Integral Transform
doi: 10.1140/epja/i2005-10009-3
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
2005RE19 Eur.Phys.J. A 25, 171 (2005) C.Reiss, H.Arenhovel, M.Schwamb π0 photoproduction on the deuteron via Δ-excitation using the Lorentz Integral Transform NUCLEAR REACTIONS 2H(γ, π0X), E ≈ threshold; calculated pion photoproduction σ, Δ resonance contribution. Lorentz integral transform method, simple pure resonance model.
doi: 10.1140/epja/i2005-10110-7
2004AR26 Phys.Rev.Lett. 93, 202301 (2004) Spin Asymmetry and Gerasimov-Drell-Hearn Sum Rule for the Deuteron NUCLEAR REACTIONS 2H(γ, n), (γ, X), E ≈ 500-2000 MeV; analyzed photodisintegration and meson production associated σ, spin asymmetries, sum rule integral.
doi: 10.1103/PhysRevLett.93.202301
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
2004SC18 Phys.Lett. B 588, 49 (2004) Meson retardation in deuteron electrodisintegration NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated structure functions, σ(E, θ); deduced meson retardation effects.
doi: 10.1016/j.physletb.2004.03.032
2003AR34 Mod.Phys.Lett. A 18, 190 (2003) H.Arenhovel, E.M.Darwish, A.Fix, M.Schwamb Present status of electromagnetic reactions on the deuteron above pion threshold NUCLEAR REACTIONS 2H(γ, p), (γ, pX), E ≈ 200-440 MeV; compiled, analyzed σ, σ(θ), pion and η meson production data.
doi: 10.1142/S0217732303010235
2003DA02 Eur.Phys.J. A 16, 111 (2003) E.M.Darwish, H.Arenhovel, M.Schwamb Influence of final-state interaction on incoherent pion photoproduction on the deuteron in the region of the Δ-resonance NUCLEAR REACTIONS 2H(γ, π-p), (γ, π0p), (γ, π+n), E=150-480 MeV; calculated σ, σ(θ); deduced final-state interaction and rescattering effects. Comparisons with data.
doi: 10.1140/epja/i2002-10071-3
2003DA18 Eur.Phys.J. A 17, 513 (2003) E.M.Darwish, H.Arenhovel, M.Schwamb Final-state interaction in spin asymmetry and GDH sum rule for incoherent pion production on the deuteron NUCLEAR REACTIONS 2H(polarized γ, π+), (polarized γ, π0), (polarized γ, π-), E=150-550 MeV; calculated pion production σ, final state interaction effects, contribution to sum rule.
doi: 10.1140/epja/i2003-10023-5
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
2001AR20 Eur.Phys.J. A 12, 207 (2001) Construction of Consistent Meson Exchange Currents by Laplace Transform NUCLEAR REACTIONS 2H(e, e'n), E ≈ threshold; calculated σ(Q2). Laplace transformation for construction of meson exchange currents.
doi: 10.1007/s100500170029
2001SC30 Nucl.Phys. A690, 647 (2001) The Role of Meson Retardation in the NN Interaction above Pion Threshold NUCLEAR REACTIONS 1n, 1H(n, n), (p, p), E < 1000 MeV; calculated scattering phase shifts, inelasticities, mixing angles. Hadronic interaction model, meson retardation, comparisons with data.
doi: 10.1016/S0375-9474(01)00355-4
2001SC31 Nucl.Phys. A690, 682 (2001) The Role of Meson Retardation in Deuteron Photodisintegration above Pion Threshold NUCLEAR REACTIONS 2H(γ, n), E=140-440 MeV; calculated σ(θ), σ, nucleon polarization. Coupled channels approach, meson retardation.
doi: 10.1016/S0375-9474(01)00360-8
2001SC53 Nucl.Phys. A696, 556 (2001) Off-Shell Effects in Electromagnetic Reactions on the Deuteron NUCLEAR REACTIONS 2H(γ, n), E=100-500 MeV; calculated photodisintegration σ, σ(θ), off-shell effects. Comparisons with data.
doi: 10.1016/S0375-9474(01)01135-6
1998SC13 Nucl.Phys. A631, 583c (1998) M.Schwamb, H.Arenhovel, P.Wilhelm, Th.Wilbois Explicit Pionic Degrees of Freedom in Deuteron Photodisintegration in the Δ-Resonance Region NUCLEAR REACTIONS 2H(γ, p), E=200-440 MeV; calculated total σ, σ(θ), photon asymmetries. Retarded potentials, coupled channels approach. Comparison with data.
doi: 10.1016/S0375-9474(98)00071-2
1998SC17 Phys.Lett. 420B, 255 (1998) M.Schwamb, H.Arenhovel, P.Wilhelm, Th.Wilbois Meson Retardation in Deuteron Photodisintegration Above π-Threshold NUCLEAR REACTIONS 2H(γ, n), E=200-440 MeV; analyzed σ(θ), σ; deduced meson retardation role.
doi: 10.1016/S0370-2693(97)01532-3
1995SC58 Few-Body Systems 19, 121 (1995) M.Schwamb, H.Arenhovel, P.Wilhelm Role of the D13 and S11 Resonances in Deuteron Photodisintegration NUCLEAR REACTIONS 2H(γ, p), E ≤ 800 MeV; analyzed σ(θ), proton polarization vs θ; deduced D13, S11 resonances role.
doi: 10.1007/s006010050021
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