NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = R.Neuhausen Found 57 matches. 2013SP05 Eur.Phys.J. A 49, 136 (2013) N.Sparveris, S.Stave, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stiliaris, Th.Walcher, M.Weis Measurements of the γ*p → Δ reaction at low Q2 NUCLEAR REACTIONS 1H(polarized e, e'p)π0, E(cm)=1205-1240 MeV; measured Ep, Ip(θ); deduced three unpolarized σ. Compared with published calculations.
doi: 10.1140/epja/i2013-13136-2
2008BO32 Phys.Rev. C 78, 054001 (2008) W.U.Boeglin, H.Arenhovel, K.I.Blomqvist, R.Bohm, M.Distler, R.Edelhoff, I.Ewald, R.Florizone, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, A.Wagner, Th.Walcher, S.Wolf, J.Jourdan, I.Sick, M.Kuss, M.Potokar, A.Rokavec, B.Vodenik, S.Sirca fLT response function of 2H(e, e'p)n at Q2=0.33 GeV/c)2 NUCLEAR REACTIONS 2H(e, e'p), E=855.11 MeV; measured σ, missing momentum, kinematic variables; deduced interference response function. Comparison with Coupled Channels Calculations.
doi: 10.1103/PhysRevC.78.054001
2008SP05 Phys.Rev. C 78, 018201 (2008) N.F.Sparveris, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, B.Pasquini, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stave, S.Stiliaris, Th.Walcher, M.Weis Virtual Compton scattering measurements in the γ* N → Δ transition NUCLEAR REACTIONS 1H(e, e'p), E=855 MeV; measured virtual Compton scattering σ, missing mass spectra; deduced magnetic dipole amplitude.
doi: 10.1103/PhysRevC.78.018201
2008ST16 Phys.Rev. C 78, 025209 (2008) S.Stave, N.Sparveris, M.O.Distler, I.Nakagawa, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stiliaris, Th.Walcher, M.Weis, for the A1 Collaboration Measurements of the γ*p → Δ reaction at low Q2: Probing the mesonic contribution NUCLEAR REACTIONS p(polarized e, e'p)π, E=705, 795, 855 MeV; measured σ, σ(θ).Comparison with model calculations.
doi: 10.1103/PhysRevC.78.025209
2008WE11 Eur.Phys.J. A 38, 27 (2008) M.Weis, P.Bartsch, D.Baumann, J.Bermuth, A.M.Bernstein, K.Bohinc, R.Bohm, M.Ding, M.O.Distler, I.Ewald, J.M.Friedrich, J.Friedrich, M.Kahrau, M.Kohl, K.W.Krygier, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.M.Pavan, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, M.Seimetz, S.Sirca, A.Wagner, Th.Walcher, for The A1 Collaboration Separated cross-sections in π0 electroproduction at threshold at Q2 = 0.05 GeV2/c2 NUCLEAR REACTIONS 1H(e, e'p), E=854.49 MeV; measured neutral pion production σ(θ), missing mass spectra. 1H(polarized e, e'p), E=854.49 MeV; measured beam helicity asymmetry. Comparison with model calculations.
doi: 10.1140/epja/i2008-10644-6
2007SP06 Phys.Lett. B 651, 102 (2007) N.F.Sparveris, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stave, S.Stiliaris, Th.Walcher, M.Weis Determination of quadrupole strengths in the γ*p → Δ(1232) transition at Q2 = 0.20 (GeV/c)2
doi: 10.1016/j.physletb.2007.04.056
2006EL02 Eur.Phys.J. A 27, 91 (2006) D.Elsner, A.Sule, P.Barneo, P.Bartsch, D.Baumann, J.Bermuth, R.Bohm, D.Bosnar, M.Ding, M.Distler, D.Drechsel, I.Ewald, J.Friedrich, J.M.Friedrich, S.Grozinger, P.Jennewein, S.Kamalov, F.H.Klein, M.Kohl, K.W.Krygier, H.Merkel, P.Merle, U.Muller, R.Neuhausen, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, M.Seimetz, O.Strahle, L.Tiator, Th.Walcher, M.Weis Measurement of the LT-asymmetry in π0 electroproduction at the energy of the Δ(1232)-resonance NUCLEAR REACTIONS 1H(polarized e, e'π0), E=855 MeV; measured longitudinal-transverse asymmetry at forward and backward angles; deduced multipole ratios. Comparison with model predictions and other data.
doi: 10.1140/epja/i2005-10212-2
2005GL03 Eur.Phys.J. A 24, 101 (2005) D.I.Glazier, M.Seimetz, J.R.M.Annand, H.Arenhovel, M.A.Antelo, C.Ayerbe, P.Bartsch, D.Baumann, J.Bermuth, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, D.Elsner, J.Friedrich, S.Hedicke, P.Jennewein, G.J.Manas, F.H.Klein, F.Klein, M.Kohl, K.W.Krygier, K.Livingston, I.J.D.MacGregor, M.Makek, H.Merkel, P.Merle, D.Middleton, U.Muller, R.Neuhausen, L.Nungesser, M.Ostrick, R.Perez Benito, J.Pochodzalla, Th.Pospischil, M.Potokar, A.Reiter, G.Rosner, J.Sanner, H.Schmieden, A.Sule, Th.Walcher, D.P.Watts, M.Weis, and the A1 Collaboration Measurement of the electric form factor of the neutron at Q2 = 0.3-0.8 (GeV/c)2 NUCLEAR REACTIONS 2H(polarized e, e'n), E=660, 855, 883 MeV; measured asymmetry, polarization transfer. 1n deduced electric form factor.
doi: 10.1140/epja/i2004-10115-8
2004AN27 Eur.Phys.J. A 22, 449 (2004) K.A.Aniol, M.B.Epstein, E.Gama, D.J.Margaziotis, W.Bertozzi, J.P.Chen, D.Dale, R.E.J.Florizone, S.Gilad, A.J.Sarty, J.A.Templon, S.P.Van Verst, J.Zhao, Z.-L.Zhou, P.Bartsch, W.U.Boeglin, R.Boehm, M.O.Distler, I.Ewald, J.M.Friedrich, J.M.Friedrich, R.Geiges, P.Jennewein, M.Kahrau, K.W.Krygier, A.Liesenfeld, H.Merkel, K.Merle, U.Muller, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, G.Rosner, H.Schmieden, A.Wagner, Th.Walcher, M.Kuss, A.Richter, G.Schrieder, K.Bohinc, M.Potokar, S.Sirca, J.M.Udias, J.R.Vignote, R.Schiavilla Measurement of RLT and ATL in the 4He(e, e'p)3H reaction at pmiss of 130-300 MeV/c NUCLEAR REACTIONS 4He(e, e'p), E=675, 855 MeV; measured σ(E, θ), transverse-longitudinal asymmetry, response function. Comparison with model predictions.
doi: 10.1140/epja/i2004-10040-x
2003BE39 Phys.Lett. B 564, 199 (2003) J.Bermuth, P.Merle, C.Carasco, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, B.Krusche, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier The neutron charge from factor and target analyzing powers from 3He(pol)(e(pol), e'n) scattering NUCLEAR REACTIONS 3He(polarized e, e'n), E=854.5 MeV; measured particle spectra, asymmetries, analyzing power; deduced final state interaction effects. 1n deduced charge form factor. Polarized target.
doi: 10.1016/S0370-2693(03)00725-1
2003CA09 Phys.Lett. B 559, 41 (2003) C.Carasco, J.Bermuth, P.Merle, P.Bartsch, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier Final state interaction effects in 3He(pol)(e(pol), e'p) NUCLEAR REACTIONS 3He(polarized e, e'p), E=854.5 MeV; measured Ep, σ(θ), asymmetries; deduced final-state interaction effects. Polarized target, comparison with model predictions.
doi: 10.1016/S0370-2693(03)00306-X
2003KO32 Phys.Rev. C 67, 065204 (2003) M.Kohl, M.A.Antelo, C.Ayerbe, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.Garcia Llongo, P.Jennewein, G.J.Manas, H.Merkel, P.Merle, U.Muller, R.Neuhausen, L.Nungesser, R.Perez Benito, J.Pochodzalla, M.Potokar, C.Rangacharyulu, A.Richter, G.Schrieder, M.Seimetz, Th.Walcher, M.Weis Search for narrow nucleon resonances below pion threshold in the H(e, e'π+)X and 2H(e, e'p)X reactions NUCLEAR REACTIONS 1H(e, e'π+X), E=660, 855 MeV; 2H(e, e'pX), E=660, 883 MeV; measured missing mass spectra; deduced nucleon resonance features.
doi: 10.1103/PhysRevC.67.065204
2002BA34 Phys.Rev.Lett. 88, 142001 (2002) P.Bartsch, D.Baumann, J.Bermuth, R.Bohm, K.Bohinc, D.Bosnar, M.Ding, M.Distler, D.Drechsel, D.Elsner, I.Ewald, J.Friedrich, J.M.Friedrich, S.Grozinger, S.Hedicke, P.Jennewein, M.Kahrau, S.S.Kamalov, F.Klein, K.W.Krygier, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, M.Seimetz, A.Sule, L.Tiator, A.Wagner, Th.Walcher, M.Weis Measurement of the Beam-Helicity Asymmetry in the p(e(pol), e'p)π0 Reaction at the Energy of the Δ(1232) Resonance NUCLEAR REACTIONS 1H(polarized e, e'π0), (polarized e, e'pX), E=854.5 MeV; measured missing mass, beam-helicity asymmetry. Comparison with model predictions.
doi: 10.1103/PhysRevLett.88.142001
2002KO16 Phys.Lett. 530B, 67 (2002) M.Kohl, P.Bartsch, D.Baumann, J.Bermuth, R.Bohm, K.Bohinc, S.Derber, M.Ding, M.O.Distler, I.Ewald, J.Friedrich, J.M.Friedrich, P.Jennewein, M.Kahrau, S.S.Kamalov, A.Kozlov, K.W.Krygier, M.Kuss, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, Th.Pospischil, M.Potokar, C.Rangacharyulu, A.Richter, D.Rohe, G.Rosner, H.Schmieden, G.Schrieder, M.Seimetz, S.Sirca, T.Suda, L.Tiator, M.Urban, A.Wagner, Th.Walcher, J.Wambach, M.Weis, A.Wirzba Self Energies of the Pion and the Δ Isobar from the 3He(e, e'π+)3H Reaction NUCLEAR REACTIONS 3He(e, e'π+), E=855 MeV; measured σ(θ, E), longitudinal and transverse σ(θ); deduced reduction in π+ mass. Chiral Perturbation Theory.
doi: 10.1016/S0370-2693(02)01345-X
2002KU01 Phys.Lett. 524B, 26 (2002) G.Kubon, H.Anklin, P.Bartsch, D.Baumann, W.U.Boeglin, K.Bohinc, R.Bohm, M.O.Distler, I.Ewald, J.Friedrich, J.M.Friedrich, M.Hauger, A.Honegger, P.Jennewein, J.Jourdan, M.Kahrau, K.W.Krygier, A.Liesenfeld, H.Merkel, U.Muller, R.Neuhausen, Ch.Normand, Th.Petitjean, Th.Pospischil, M.Potokar, D.Rohe, G.Rosner, H.Schmieden, I.Sick, S.Sirca, Ph.Trueb, A.Wagner, Th.Walcher, G.Warren, M.Weis, H.Wohrle, M.Zeier, J.Zhao, B.Zihlmann Precise Neutron Magnetic Form Factors NUCLEAR REACTIONS 2H(e, e'p), (e, e'n), E=555, 600, 855 MeV; measured relative σ(Q2). 1n deduced magnetic form factors.
doi: 10.1016/S0370-2693(01)01386-7
2001DI06 Phys.Lett. 500B, 47 (2001) S.Dieterich, P.Bartsch, D.Baumann, J.Bermuth, K.Bohinc, R.Bohm, D.Bosnar, S.Derber, M.Ding, M.Distler, I.Ewald, J.Friedrich, J.M.Friedrich, R.Gilman, C.Glashausser, M.Hauger, P.Jennewein, J.Jourdan, J.J.Kelly, M.Kohl, A.Kozlov, K.W.Krygier, G.Kumbartzki, J.Lac, A.Liesenfeld, H.Merkel, U.Muller, R.Neuhausen, Th.Pospischil, R.D.Ransome, D.Rohe, G.Rosner, H.Schmieden, M.Seimetz, I.Sick, S.Strauch, J.M.Udias, J.R.Vignote, A.Wagner, Th.Walcher, G.Warren, M.Weis Polarization Transfer in the 4He((pol)e, e'p(pol))3H Reaction NUCLEAR REACTIONS 4He(polarized e, e'p), E=854.5 MeV; measured polarization transfer vs missing momentum. Comparison with model predictions.
doi: 10.1016/S0370-2693(01)00052-1
2001EW01 Phys.Lett. 499B, 238 (2001) I.Ewald, P.Bartsch, D.Baumann, J.Bermuth, A.M.Bernstein, K.Bohinc, R.Bohm, N.Clawiter, S.Derber, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, M.Kahrau, M.Kohl, A.Kozlov, K.W.Krygier, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.Pavan, Th.Pospischil, M.Potokar, D.Rohe, G.Rosner, H.Schmieden, S.Sirca, A.Wagner, Th.Walcher, M.Weis Coherent π0 Threshold Production from the Deuteron at Q2 = 0.1 GeV2/c2 NUCLEAR REACTIONS 2H(e, e'π0), E=345, 435, 720 MeV; measured missing mass distributions, σ(θ), σ; deduced partial wave contributions. Comparison with Chiral Perturbation theory.
doi: 10.1016/S0370-2693(00)01396-4
2001KO24 Nucl.Phys. A684, 460c (2001) A.Kozlov, K.A.Aniol, P.Bartsch, D.Baumann, W.Bertozzi, R.Bohm, K.Bohinc, J.P.Chen, D.Dale, L.Dennis, S.Derber, M.Ding, M.O.Distler, P.Dragovitsch, I.Ewald, K.G.Fissum, R.E.J.Florizone, J.Friedrich, J.M.Friedrich, R.Geiges, S.Gilad, P.Jennewein, M.Kahrau, M.Kohl, K.W.Krygier, A.Liesenfeld, D.J.Margaziotis, H.Merkel, P.Merle, U.Muller, R.Neuhausen, T.Pospischil, G.Riccardi, R.Roche, G.Rosner, D.Rowntree, A.J.Sarty, H.Schmieden, S.Sirca, J.A.Templon, M.N.Thompson, A.Wagner, Th.Walcher, M.Weis, J.Zhao, Z.Zhou The Longitudinal and Transverse Response of the 4He(e, e'p) Reaction in the Dip Region NUCLEAR REACTIONS 4He(e, e'p), E=570, 675, 855 MeV; measured σ(E, θ), momentum distributions; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)00504-8
2001PO08 Phys.Rev.Lett. 86, 2959 (2001) Th.Pospischil, P.Bartsch, D.Baumann, J.Bermuth, R.Bohm, K.Bohinc, S.Derber, M.Ding, M.Distler, D.Drechsel, D.Elsner, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, S.Hedicke, P.Jennewein, M.Kahrau, S.S.Kamalov, F.Klein, K.W.Krygier, J.Lac, A.Liesenfeld, J.McIntyre, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.Potokar, R.D.Ransome, D.Rohe, G.Rosner, H.Schmieden, M.Seimetz, S.Sirca, I.Sick, A.Sule, L.Tiator, A.Wagner, Th.Walcher, G.A.Warren, M.Weis Measurement of the Recoil Polarization in the p(e(pol), e'p(pol)π0 Reaction at the Δ(1232) Resonance NUCLEAR REACTIONS 1H(polarized e, e'π0), E=854.4 MeV; measured recoil proton polarization components; deduced Coulomb quadrupole to magnetic dipole ratio. Mainz unitary isobar model.
doi: 10.1103/PhysRevLett.86.2959
2001PO27 Eur.Phys.J. A 12, 125 (2001) Th.Pospischil, P.Bartsch, D.Baumann, R.Bohm, K.Bohinc, M.Ding, S.Derber, M.O.Distler, D.Elsner, I.Ewald, J.Friedrich, J.M.Friedrich, S.Grozinger, S.Hedicke, P.Jennewein, J.Jourdan, M.Kahrau, F.Klein, K.W.Krygier, J.Lac, A.Liesenfeld, S.Malov, J.McIntyre, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.Potokar, R.D.Ransome, D.Rohe, G.Rosner, J.Sanner, H.Schmieden, M.Seimetz, S.Sirca, I.Sick, O.Strahle, A.Sule, A.Wagner, Th.Walcher, M.Weis Measurement of GEp/GMp via Polarization Transfer at Q2 = 0.4 GeV/c2 NUCLEAR REACTIONS 1H(polarized e, e), E=854.4 MeV; measured polarization transfer; deduced form factor ratio.
doi: 10.1007/s100500170046
2000FR07 Nucl.Phys. A663-664, 389c (2000) J.M.Friedrich, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, J.Roche, D.Rohe, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher The First Dedicated Virtual Compton Scattering Experiment at MAMI NUCLEAR REACTIONS 1H(e, e'γ), E not given; measured ep-coin, σ(E, θ(e), θ(p)); deduced structure function.
doi: 10.1016/S0375-9474(99)00624-7
2000RO21 Phys.Rev.Lett. 85, 708 (2000) J.Roche, J.M.Friedrich, D.Lhuillier, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.D'Hose, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, I.Ewald, H.Fonvieille, J.Friedrich, P.A.M.Guichon, H.Holvoet, Ch.E.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, K.W.Krygier, B.Lannoy, A.Liesenfeld, C.Marchand, D.Marchand, J.Marroncle, J.Martino, H.Merkel, P.Merle, G.De Meyer, J.Mougey, U.Muller, R.Neuhausen, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, D.Rohe, G.Rosner, D.Ryckbosch, H.Schmieden, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, M.Weiss First Determination of Generalized Polarizabilities of the Proton by a Virtual Compton Scattering Experiment NUCLEAR REACTIONS 1H(polarized e, e'γ), E=855 MeV; measured σ(E, θ(e), θ(p)). 1H deduced dynamic structure functions, generalized polarizibilities. High-resolution spectrometers, virtual Compton scattering.
doi: 10.1103/PhysRevLett.85.708
1999BA31 Eur.Phys.J. A 4, 209 (1999) P.Bartsch, D.Baumann, J.Bermuth, K.Bohinc, R.Bohm, D.Bosnar, N.Clawiter, S.Derber, M.Ding, M.O.Distler, A.Ebbes, I.Ewald, J.M.Friedrich, J.Friedrich, P.Jennewein, M.Kahrau, M.Kohl, A.Kozlov, K.W.Krygier, M.Kuss, A.Liesenfeld, H.Merkel, K.Merle, U.Muller, R.Neuhausen, T.Pospischil, M.Potokar, D.Rohe, G.Rosner, H.Schmieden, S.Sirca, A.Wagner, T.Walcher, M.Weis, S.Wolf Evidence for Narrow Δ0(1232) States in the 12C(e, e'pπ-)11C Reaction NUCLEAR REACTIONS 12C(e, e'pπ-), E=600, 855 MeV; measured missing momentum, excitation energy spectra. 12C deduced bound Δ0 resonance states, widths. Triple coincidence measurement. Weak coupling model analysis.
doi: 10.1007/s100500050220
1999FL02 Phys.Rev.Lett. 83, 2308 (1999) R.E.J.Florizone, W.Bertozzi, J.P.Chen, D.Dale, S.Gilad, A.J.Sarty, J.A.Templon, S.P.Van Verst, J.Zhao, Z.-L.Zhou, P.Bartsch, W.U.Boeglin, R.Bohm, M.O.Distler, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, P.Jennewein, M.Kahrau, K.W.Krygier, A.Liesenfeld, H.Merkel, K.Merle, U.Muller, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, G.Rosner, H.Schmieden, A.Wagner, Th.Walcher, K.A.Aniol, M.B.Epstein, D.J.Margaziotis, M.Kuss, A.Richter, G.Schrieder, K.Bohinc, M.Potokar, S.Sirca High-Precision Studies of the 3He(e, e'p) Reaction at the Quasielastic Peak NUCLEAR REACTIONS 3He(e, e'p), E=540, 675, 855 MeV; measured σ(E, θ(p), θ(e)); deduced two-body-breakup, continuum momentum distributions. Quasielastic kinematics.
doi: 10.1103/PhysRevLett.83.2308
1999LI41 Phys.Lett. 468B, 20 (1999) A.Liesenfeld, A.W.Richter, S.Sirca, K.I.Blomqvist, W.U.Boeglin, K.Bohinc, R.Bohm, M.Distler, D.Drechsel, R.Edelhoff, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, M.Kahrau, M.Korn, K.W.Krygier, V.Kunde, H.Merkel, K.Merle, U.Muller, R.Neuhausen, T.Pospischil, M.Potokar, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, H.Schmieden, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf A Measurement of the Axial Form Factor of the Nucleon by the p(e, e'π+)n Reaction at W = 1125 MeV NUCLEAR REACTIONS 1H(e, e'π+), E=405-855 MeV; measured longitudinal, transverse σ(θ); deduced axial mass parameter. Effective Lagrangian model.
doi: 10.1016/S0370-2693(99)01204-6
1999RO19 Phys.Rev.Lett. 83, 4257 (1999) D.Rohe, P.Bartsch, D.Baumann, J.Becker, J.Bermuth, K.Bohinc, R.Bohm, S.Buttazzoni, T.Caprano, N.Clawiter, A.Deninger, S.Derber, M.Ding, M.Distler, A.Ebbes, M.Ebert, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, T.Grossmann, M.Hauger, W.Heil, A.Honegger, P.Jennewein, J.Jourdan, M.Kahrau, A.Klein, M.Kohl, K.W.Krygier, G.Kubon, A.Liesenfeld, H.Merkel, K.Merle, P.Merle, M.Muhlbauer, U.Muller, R.Neuhausen, E.W.Otten, Th.Petitjean, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, I.Sick, S.Sirca, R.Surkau, A.Wagner, Th.Walcher, G.Warren, M.Weis, H.Wohrle, M.Zeier Measurement of the Neutron Electric Form Factor Gen at 0.67 (GeV/c)2 via 3He(pol)(e(pol), e'n) NUCLEAR REACTIONS 3He(polarized e, e'n), E=854 MeV; measured electron spectra, neutron spectra, asymmetries. 1n deduced electric form factor. Polarized target.
doi: 10.1103/PhysRevLett.83.4257
1999RO30 Nucl.Phys. (Supplement) A654, 547c (1999) J.Roche, P.Bartsch, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, J.M.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, S.Wolf Virtual Compton Scattering Under π0 Threshold at Q2 = 0.33 GeV2. Preliminary Results. NUCLEAR REACTIONS 1H(e, e'γ), E=750-855 MeV; measured ep-coin, photon polarization, σ(θ). Virtual Compton scattering.
doi: 10.1016/S0375-9474(00)88498-5
1998AN13 Phys.Lett. 428B, 248 (1998) H.Anklin, L.J.deBever, K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, D.Fritschi, R.Geiges, J.Gotz, A.Honegger, P.Jennewein, J.Jourdan, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, G.Kubon, V.Kunde, A.Liesenfeld, G.Masson, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Petitjean, Th.Pospischil, M.Potokar, L.M.Qin, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, I.Sick, S.Sirca, Ph.Trueb, M.Tuccillo, B.Vodenik, A.Wagner, Th.Walcher, G.Warren, S.Wolf, J.Zhao, M.Zeier, B.Zihlmann Precise Measurements of the Neutron Magnetic Form Factor NUCLEAR REACTIONS 2H(e, e'p), (e, e'n), E not given; measured σ ratios vs momentum transfer; deduced neutron magnetic form factor G(mn).
doi: 10.1016/S0370-2693(98)00442-0
1998BL06 Phys.Lett. 421B, 71 (1998) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.K.Jones, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, C.L.Morris, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, R.D.Ransome, A.W.Richter, B.G.Ritchie, A.Rokavec, G.Rosner, J.Ryckebusch, P.Sauer, S.Schardt, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf, M.K.Yadav Investigation of Short-Range Nucleon-Nucleon Correlations using the Reaction 12C(e, e'pp) in Close to 4π Geometry NUCLEAR REACTIONS 12C(e, e'2p), E=705 MeV; measured nine-fold σ(E, θ), missing momentum spectra; deduced short-range nucleon-nucleon correlations.
doi: 10.1016/S0370-2693(98)00024-0
1998BL07 Phys.Lett. 424B, 33 (1998) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, I.Ewald, R.Florizone, J.Friedrich, R.Geiges, J.Jourdan, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, B.Vodenik, I.Sick, S.Sirca, A.Wagner, Th.Walcher, S.Wolf Large Recoil Momenta in the D(e, e'p)n Reaction NUCLEAR REACTIONS 2H(e, e'p), E=855.11 MeV; measured σ(θ(e), θ(p)) vs missing momentum; deduced possible virtual nucleon excitation role. Model comparisons.
doi: 10.1016/S0370-2693(98)00151-8
1998DI03 Phys.Rev.Lett. 80, 2294 (1998) M.O.Distler, A.M.Bernstein, K.I.Blomqvist, W.U.Boeglin, R.Bohm, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, H.Merkel, K.Merle, R.Neuhausen, Th.Pospischil, M.Potokar, A.Rokavec, A.W.Richter, G.Rosner, P.Sauer, St.Schardt, H.Schmieden, S.Sirca, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Measurement of Separated Structure Functions in the p(e, e'p)π0 Reaction at Threshold and Chiral Perturbation Theory NUCLEAR REACTIONS 1H(e, e'π0), E=435, 555, 855 MeV; measured pion σ(E, θ); deduced structure functions. Comparison with chiral perturbation theory calculations.
doi: 10.1103/PhysRevLett.80.2294
1997BL13 Nucl.Phys. A626, 871 (1997) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, S.Kamalov, M.Kirchbach, M.Kohl, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.M.Laget, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, C.Rangacharyulu, A.Richter, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, St.Schardt, G.Schrieder, T.Suda, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Pion Electroproduction in the 3He(e, e'π+)3H Reaction at Intermediate Energies NUCLEAR REACTIONS 3He(e, e'π+), E=555-855 MeV; measured transverse, longitudinal σ(θ(π)); deduced transverse, longitudinal structure functions. Standard Born amplitudes for elementary pion production, three-body Fadeev wave functions.
doi: 10.1016/S0375-9474(97)00463-6
1996BL02 Z.Phys. A353, 415 (1996) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, D.Drechsel, R.Edelhoff, J.Friedrich, R.Geiges, O.Hanstein, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.Rokavec, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, H.Schmieden, S.Sirca, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf Precise Pion Electroproduction in the p(e, e'π+)n Reaction at W = 1125 MeV NUCLEAR REACTIONS 1H(e, e'π+), E(cm)=1125 MeV; measured missing energy spectra, coincidence, longitudinal σ, asymmetry; deduced longitudinal, transverse structure functions, interference term.
doi: 10.1007/BF01285153
1996BL20 Phys.Rev.Lett. 77, 2396 (1996) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.M.Laget, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, C.Rangacharyulu, A.Rokavec, A.Richter, A.W.Richter, G.Rosner, P.Sauer, St.Schardt, G.Schrieder, T.Suda, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Forward-Angle 3He(e, e'π±) Coincident Electroproduction and the Search for Δ's in the Ground State of 3He NUCLEAR REACTIONS 3He(e, e'π+), E=555-855 MeV; measured σ(θ(π)) vs missing mass; deduced preformed Δ++ related features.
doi: 10.1103/PhysRevLett.77.2396
1995BL02 Phys.Lett. 344B, 85 (1995) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.Lac, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, Th.Veit, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf High-Momentum Components in the 1p Orbitals of 16O NUCLEAR REACTIONS 16O(e, e'p), E=855 MeV; measured σ(E(e'), θ(e'), Ep, θp). 16O deduced proton momentum distribution. Natural target.
doi: 10.1016/0370-2693(94)01540-S
1995BL10 Z.Phys. A351, 353 (1995) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.Lac, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, Th.Veit, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf No Evidence for Medium Effects in the 12C(e, e'p)11B(g.s.) Reaction NUCLEAR REACTIONS 12C(e, e'p), E not given; measured distorted momentum distribution vs missing momentum; deduced spectroscopic factor for transition to 11B(g.s). Parallel, anti-parallel kinenmatics.
doi: 10.1007/BF01291135
1995DE23 Phys.Rev. C52, 61 (1995) D.J.DeAngelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Multipole Strength in 12C from the (e, e'α) Reaction for Momentum Transfers up to 0.61 fm -1 NUCLEAR REACTIONS 12C(e, e'p), (e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e'), θ(α)), σ(θ(e'), θ(p)) vs energy transfer. 12C deduced B(E2), EWSR strength.
doi: 10.1103/PhysRevC.52.61
1994VE08 Z.Phys. A349, 161 (1994) T.Veit, K.I.Blomqvist, W.U.Boeglin, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, A.Wagner, Th.Walcher, S.Wolf Model-Independent Separation of Structure Functions Over an Extended Kinematical Region NUCLEAR REACTIONS 12C(e, e'p), E ≈ quasifree region; calculated structure functions, separation. Model independent approach.
doi: 10.1007/BF01291175
1993DE10 Phys.Rev.Lett. 70, 2872 (1993) D.De Angelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Isoscalar E2 Strength in 12C from the (e, e'α) Reaction NUCLEAR REACTIONS 12C(e, e'α), E=124.1-183.4 MeV; measured σ(θ(e), θ(α)) vs energy transfer. 12C deduced GQR associated EWSR, B(E2).
doi: 10.1103/PhysRevLett.70.2872
1992FR05 Phys.Rev.Lett. 68, 1667 (1992) J.P.Fritsch, H.J.Emrich, A.Grasmuck, R.Neuhausen, S.Schardt, N.Zimmermann, J.R.Calarco, M.Potokar Isoscalar E2 Strength in 16O from the (e, e'α) Reaction NUCLEAR REACTIONS 16O(e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e), θα). 16O deduced isoscalar electric quadrupole strength distribution.
doi: 10.1103/PhysRevLett.68.1667
1991PO06 Nucl.Phys. A527, 372c (1991) M.Potokar, J.R.Calarco, J.E.Wise, N.Zimmermann, H.Weyand, H.J.Emrich, J.P.Fritsch, A.Grasmuck, R.Neuhausen, S.Schardt Separation of the Longitudinal and Transverse Amplitudes for the Giant Dipole Resonances of 12C and 16O from Measurement of the (e, e'p0) Angular Correlations NUCLEAR REACTIONS 12C, 16O(e, e'p), E not given; measured σ(θ(e'), θ(p)) vs energy transfer. 12C, 16O deduced GDR amplitudes features.
doi: 10.1016/0375-9474(91)90126-Q
1990HE15 Ann.Phys.(Paris) 15, 39 (1990) W.Heil, J.Ahrens, H.G.Andresen, A.Bornheimer, D.Conrath, K.-J.Dietz, W.Gasteyer, H.-J.Gessinger, W.Hartmann, J.Jeth-Wa, H.-J.Kluge, H.Kessler, T.Kettner, L.Koch, F.Neugebauer, R.Neuhausen, E.W.Otten, E.Reichert, F.P.Schafer, B.Wagner Measurement of the Parity Violation in the Quasi-Elastic Scattering of Polarized Electrons from 9Be NUCLEAR REACTIONS 9Be(polarized e, e'X), E=300 MeV; measured parity violating asymmetry; deduced Weinberg angle. Model independent electron-nucleon coupling constants.
1989TI02 Nucl.Phys. A501, 751 (1989) L.Tiator, C.Bennhold, R.Neuhausen Inelastic Electron Scattering and Pion Photoproduction on 12C NUCLEAR REACTIONS 12C(e, e'), E=350 MeV; measured σ(E, θ); deduced form factors, nuclear structure coefficients, 12C(γ, π+) reaction σ(θ). Non-local DWIA.
doi: 10.1016/0375-9474(89)90159-0
1988NE06 Can.J.Phys. 66, 513 (1988) Measurement of the Parity Violation in the Quasi-Elastic Scattering of Polarized Electrons from 9Be NUCLEAR REACTIONS 9Be(polarized e, e'X), E=300 MeV; measured parity nonconserving asymmetry. Longitudinal beam polarization.
doi: 10.1139/p88-084
1987AH06 Helv.Phys.Acta 60, 738 (1987) J.Ahrens, H.G.Andresen, H.J.Gessinger, W.Hartmann, W.Heil, H.J.Kluge, R.Neuhausen, E.W.Otten, E.Reichert, F.P.Schafer, B.Wagner Measurement of the Parity Violation in the Quasi-Free Scattering of Polarized Electrons from 9Be NUCLEAR REACTIONS 9Be(polarized e, e'), E=300 MeV; measured parity violating helicity asymmetry; deduced weak, neutral current, nucleon model independent weak coupling constants.
1986KI09 Phys.Rev.Lett. 56, 2789 (1986) Th.Kihm, K.T.Knopfle, H.Riedesel, P.Voruganti, H.J.Emrich, G.Fricke, R.Neuhausen, R.K.M.Schneider E1 and E2-E0 Form Factors and Strength Distributions from 28Si(e, e'p) and 28Si(e, e'α) Coincidence Scattering NUCLEAR REACTIONS 28Si(e, e'p), (e, e'α), E=183.5 MeV; measured e'p-, e'α-coin, σ(E(e')). 28Si deduced form factors, giant resonances, multipole transition strength distribution.
doi: 10.1103/PhysRevLett.56.2789
1984BE13 Phys.Rev. C29, 1168 (1984) J.C.Bergstrom, R.Neuhausen, G.Lahm Electroexcitation of Levels in 14N between 12 and 21 MeV NUCLEAR REACTIONS 14N(e, e'), E=112-300 MeV; measured σ(E(e'), θ) vs E. 14N levels deduced form factors, transition strengths, configuration. Comparison with pion scattering.
doi: 10.1103/PhysRevC.29.1168
1984HU07 Phys.Lett. 139B, 249 (1984) R.L.Huffman, R.S.Hicks, J.Dubach, B.Parker, M.A.Plum, G.Lahm, R.Neuhausen, J.C.Bergstrom Comparison of Isoscalar and Isovector (e, e') M1 Form Factors at High Momentum Transfer NUCLEAR REACTIONS 14N(e, e), (e, e'), E not given; measured M1 form factors. 14N deduced isoscalar, isovector transition differences. Shell model comparison.
doi: 10.1016/0370-2693(84)91073-6
1983DE53 Nucl.Phys. A411, 337 (1983) U.Deutschmann, G.Lahm, R.Neuhausen, J.C.Bergstrom Electron Scattering Studies of Magnetic Isovector Transitions in 12C at High Momentum Transfer NUCLEAR REACTIONS 12C(e, e'), E=80-330 MeV; measured σ(E, E(e'), θ). 12C deduced levels, Γ, form factors, transition current density, Γ(γ0).
doi: 10.1016/0375-9474(83)90534-1
1983ST09 Nucl.Phys. A404, 413 (1983) W.Steffen, H.-D.Graf, A.Richter, A.Harting, W.Weise, U.Deutschmann, G.Lahm, R.Neuhausen Form Factor of the M1 Transition to the 10.23 MeV State in 48Ca and the Role of the Δ(1232) NUCLEAR REACTIONS 48Ca(e, e'), E=30-145 MeV; measured σ(E, θ). 48Ca level deduced B(M1), form factor. Shell model, isobar-hole calculations.
doi: 10.1016/0375-9474(83)90267-1
1982BE11 Phys.Rev. C25, 1156 (1982) J.C.Bergstrom, S.B.Kowalski, R.Neuhausen Elastic Magnetic Form Factor of 6Li NUCLEAR REACTIONS 6Li(e, e'), E=80-300 MeV; measured σ(E, E(e'), θ). 6Li deduced M1 form factor, ground state current density. Cluster model, exchange currents.
doi: 10.1103/PhysRevC.25.1156
1979BE38 Nucl.Phys. A327, 439 (1979) J.C.Bergstrom, U.Deutschmann, R.Neuhausen Electron Scattering from the 3.65 MeV (O+, T = 1) State in 6Li at High Momentum Transfer NUCLEAR REACTIONS 6Li(e, e'), E=140-330 MeV; measured σ(E;Ee', θ). 6Li levels deduced form factors, transition current density, Γγ.
doi: 10.1016/0375-9474(79)90268-9
1977NE05 Nucl.Phys. A282, 125 (1977) Transition Charge Densities of Low-Lying Collective States in Even Zn Isotopes NUCLEAR REACTIONS 64,66,68Zn(e, e'), E=100-275 MeV; measured σ(E, θ). 64,66,68Zn levels deduced transition charge density, B(EL), transition charge radii. Enriched targets.
doi: 10.1016/0375-9474(77)90175-0
1976NE06 Nucl.Phys. A263, 249 (1976) R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner Electron Scattering Studies of Low-Lying Collective States of Even Zn Isotopes NUCLEAR REACTIONS 64,66,68,70Zn(e, e'), E=40-112 MeV; measured σ(E, Ee', θ). 64,66,68,70Zn deduced B(E2), B(E3). Application of anharmonic vibrator model. Enriched targets.
doi: 10.1016/0375-9474(76)90171-8
1972NE01 Phys.Rev. C5, 124 (1972) R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner Elastic Electron Scattering from Zn Isotopes NUCLEAR REACTIONS 64,66,68,70Zn(e, e), E=61-120 MeV; measured σ(E;θ). 64,66,68,70Zn deduced rms radii, charge distribution parameters.
doi: 10.1103/PhysRevC.5.124
1971NE03 Nucl.Phys. A164, 497 (1971) Investigation of the Low-Lying States in 6Li by Inelastic Electron Scattering NUCLEAR REACTIONS 6Li(e, e'), E=80-190 MeV; measured σ(E, θ); deduced form factors. 6Li deduced nucleon distributions. Enriched targets.
doi: 10.1016/0375-9474(71)90775-5
1970HU09 Z.Naturforsch. 25a, 973 (1970) R.M.Hutcheon, R.Neuhausen, F.Eigenbrod An Investigation of the 5.36 MeV Level in 6Li by Electron Scattering NUCLEAR REACTIONS 6Li(e, e'), E=159 MeV; measured σ(Ee'); deduced inelastic form factor. 6Li deduced level, level-width.
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