NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = V.H.Walther Found 21 matches. 1990GH01 Phys.Rev. C41, 653 (1990) L.Ghedira, D.Myers, B.H.Cottman, K.Sankhavaram, M.D.Seneviratne, P.Stoler, E.J.Winhold, M.Yamazaki, P.F.Yergin, J.H.J.Distelbrink, K.Rohrich, Ch.Schmitt, V.H.Walther, A.M.Bernstein, K.I.Blomqvist, J.A.Nelson 14N(γ, π+)14C(g.s.) at Photon Energies of 230, 260, and 320 MeV NUCLEAR REACTIONS 14N(γ, π+), E=230, 260 MeV; measured σ(θ); deduced Δ effects. Delta-hole model analysis.
doi: 10.1103/PhysRevC.41.653
1989SP05 Phys.Rev.Lett. 63, 1574 (1989) M.Spahn, Th.Kihm, K.T.Knopfle, J.Friedrich, N.Voegler, Ch.Schmitt, V.H.Walther, M.Unkelbach, H.M.Hofmann Study of Charge Symmetry in 4He by Simultaneous 4He(e, e'p)3H and 4He(e, e'n)3He Measurements NUCLEAR REACTIONS 4He(e, e'p), (e, e'n), E=183.4 MeV; measured σ(θ(e'), θ(p)), σ(θ(e'), θ(n)); deduced σ. 4He deduced no charge symmetry breaking in GDR region.
doi: 10.1103/PhysRevLett.63.1574
1988LI23 Nucl.Phys. A485, 580 (1988) A.Liesenfeld, B.Alberti, D.Eyl, G.Kobschall, A.W.Richter, K.Rohrich, Ch.Schmitt, L.Tiator, V.H.Walther Electroproduction of Negative Pions on 15N Leading to the Ground State of 15O NUCLEAR REACTIONS 15N(e, π-), E=170 MeV; measured σ(E(e), θ(π), E(π)). Virtual photon theory.
doi: 10.1016/0375-9474(88)90554-4
1987KO16 Nucl.Phys. A466, 612 (1987) G.Kobschall, B.Alberti, H.Jansen, K.Rohrich, Ch.Schmitt, V.H.Walther, K.Weinand, M.Kobayashi, H.Arenhovel Low Energy Charged Pion Production from the Deuteron NUCLEAR REACTIONS 2H(e, e'π+), E=170, 183 MeV; measured σ(E(nn), θ); deduced nn-system 1S0 state. Effective hamiltonian Born amplitudes. Liquid target, magnetic spectrometer.
doi: 10.1016/0375-9474(87)90459-3
1987RO23 Nucl.Phys. A475, 761 (1987) K.Rohrich, G.Kobschall, C.Reifferscheid, C.Schmitt, V.H.Walther, K.Weinand Measurement of Positive Pion Production from 14N at Low Momentum Transfer NUCLEAR REACTIONS 14N(e, π+), E=173.5 MeV; measured σ(E, θ(π), E(π)). 14C, 14N deduced wave function mixing parameters. Shell model.
doi: 10.1016/0375-9474(87)90236-3
1986TE01 Phys.Lett. 177B, 25 (1986) P.K.Teng, B.H.Cottman, L.Ghedira, K.Min, P.Stoler, E.J.Winhold, M.Yamazaki, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, J.H.J.Distelbrink, J.A.Nelson, K.Rohrich, Ch.Schmitt, L.Tiator, V.H.Walther, S.A.Dytman, L.E.Wright Angular Distribution Measurement of 14N(γ, π+)14C(gs) at E(γ) = 320 MeV NUCLEAR REACTIONS 14N(γ, π+), E=320 MeV; measured σ(θ). DWIA, momentum space.
doi: 10.1016/0370-2693(86)90007-9
1985CO15 Phys.Rev.Lett. 55, 684 (1985) B.H.Cottman, K.Min, P.Stoler, P.K.Teng, E.J.Winhold, M.Yamazaki, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, J.H.J.Distelbrink, J.A.Nelson, K.Rohrich, C.Schmitt, L.Tiator, V.H.Walther, G.Audit, S.A.Dytman, L.E.Wright Measurement of 14N(γ, π+)14C(g.s.) at 200 MeV: A test of the distorted-wave impulse approximation for charged-pion photoproduction below the Δ(1232) resonance NUCLEAR REACTIONS 14N(γ, π+), E=200 MeV bremsstrahlung; measured σ(θ, E(π)) vs pion momentum, σ(θ) vs momentum transfer; deduced structure effects. DWIA, one-body pion photoproduction operator.
doi: 10.1103/PhysRevLett.55.684
1985OT02 Nucl.Phys. A436, 688 (1985) C.R.Ottermann, G.Kobschall, K.Maurer, K.Rohrich, Ch.Schmitt, V.H.Walther Elastic Electron Scattering from 3He and 4He NUCLEAR REACTIONS 3,4He(e, e), E=105-320 MeV; measured σ(θ, E), charge, magnetic form factors. 3,4He deduced rms radii. Model independent analysis.
doi: 10.1016/0375-9474(85)90554-8
1985RO05 Phys.Lett. 153B, 203 (1985) K.Rohrich, L.Tiator, G.Kobschall, Ch.Reifferscheid, Ch.Schmitt, V.H.Walther, K.Weinand, L.E.Wright Pion Photoproduction on 14N at 173 MeV Photon Energy NUCLEAR REACTIONS 14N(γ, π+), E=173 MeV; measured σ(θ(π), E(π)); deduced σ(θ).
doi: 10.1016/0370-2693(85)90531-3
1985SC17 Nucl.Instrum.Methods 237, 523 (1985) Ch.Schmitt, G.Kobschall, Ch.Reifferscheid, K.Rohrich, K.Weinand, V.H.Walther A Magnetic Spectrometer for Low Energy Pion Identification in Pion Production Experiments NUCLEAR REACTIONS 12C(γ, π+), E=183.8 MeV bremsstrahlung; measured σ(θ(π), E(π)); deduced σ(θ(π)). Low energy pions, magnetic spectrometer.
doi: 10.1016/0168-9002(85)91062-9
1984KO05 Nucl.Phys. A412, 294 (1984) G.Kobschall, E.Fein, C.Ottermann, K.Maurer, F.Rohrich, Ch.Schmitt, V.H.Walther Electrodisintegration of 3He NUCLEAR REACTIONS 3He(e, e'), E=100-300 MeV; measured σ(E(e'), θ(e')) vs E. Plane wave impulse approximation calculations.
doi: 10.1016/0375-9474(84)90684-5
1983KO25 Nucl.Phys. A405, 648 (1983) G.Kobschall, C.Ottermann, K.Maurer, K.Rohrich, Ch.Schmitt, V.H.Walther Excitation of the Quasi-Bound State in 4He by Electron Scattering at Medium Momentum Transfer NUCLEAR REACTIONS 4He(e, e'), E=400 MeV; measured σ(θ(e), E(e)). 4He deduced level excitation, longitudinal transition form factor.
doi: 10.1016/0375-9474(83)90523-7
1983SC03 Nucl.Phys. A392, 345 (1983) Ch.Schmitt, K.Rohrich, K.Maurer, C.Ottermann, V.H.Walther Experimental Test of the Virtual Photon Theory for Pion Electroproduction NUCLEAR REACTIONS 1H, 12C(e, π+), E ≥ threshold; measured σ(θ, E(π), E). Virtual photon theory test.
doi: 10.1016/0375-9474(83)90130-6
1983SC36 Nuovo Cim. 76A, 419 (1983) Ch.Schmitt, K.Rohrich, V.H.Walther The Pion Electroproduction and the Virtual-Photon Theory NUCLEAR REACTIONS 1H, 12C(e, π+), E ≈ threshold; measured σ(θ, E(π)), σ(θ). 12C(γ, π+), E not given; deduced σ(θ). Virtual photon theory.
doi: 10.1007/BF02833737
1982OT01 Nucl.Phys. A379, 396 (1982) C.R.Ottermann, Ch.Schmitt, G.G.Simon, F.Borkowski, V.H.Walther Elastic Electron Scattering from 40Ar NUCLEAR REACTIONS 40Ar(e, e), E=116, 249 MeV; measured σ(θ). 40Ar deduced rms charge radius. Fourier-Bessel analysis.
doi: 10.1016/0375-9474(82)90004-5
1981SI06 Nucl.Phys. A364, 285 (1981) G.G.Simon, Ch.Schmitt, V.H.Walther Elastic Electric and Magnetic e - d Scattering at Low Momentum Transfer NUCLEAR REACTIONS 2H(e, e), E=80.1-298.9 MeV; measured σ(θ, E). 2H deduced rms radius. High pressure gas, liquid target systems.
doi: 10.1016/0375-9474(81)90572-8
1980SI01 Nucl.Phys. A333, 381 (1980) G.G.Simon, C.Schmitt, F.Borkowski, V.H.Walther Absolute Electron-Proton Cross Sections at Low Momentum Transfer Measured with a High Pressure Gas Target System NUCLEAR REACTIONS 1H(e, e), E=150-321 MeV; measured σ(θ). 1H deduced electromagnetic form factors, rms charge radius.
doi: 10.1016/0375-9474(80)90104-9
1979SI14 Nucl.Phys. A324, 277 (1979) G.G.Simon, F.Borkowski, C.Schmitt, V.H.Walther, H.Arenhovel, W.Fabian Inelastic Electromagnetic Form Factors of the Deuteron and Exchange Current Effects NUCLEAR REACTIONS 2H(e, e), (e, e'), (e, n), E=80-350 MeV; measured σ(Ee), longitudinal, transverse form factors as function of E(np). Reid soft core potential, meson exchange currents, isobar configurations.
doi: 10.1016/0375-9474(79)90584-0
1976SI12 Phys.Rev.Lett. 37, 739 (1976) G.G.Simon, F.Borkowski, C.Schmitt, V.H.Walther, H.Arenhovel, W.Fabian Observation of Meson-Exchange Effects in Deuteron Electrodisintegration NUCLEAR REACTIONS 2H(e, X), (e, e), E=80-300 MeV; measured σ; deduced meson-exchange effects.
doi: 10.1103/PhysRevLett.37.739
1974BO16 Nucl.Phys. A222, 269 (1974) F.Borkowski, P.Peuser, G.G.Simon, V.H.Walther, R.D.Wendling Electromagnetic Form Factors of the Proton at Low Four-Momentum Transfer NUCLEAR REACTIONS 1H(e, e), E=150-275 MeV; measured σ(Ee, θ). 1H deduced electromagnetic form factors. Liquid target.
doi: 10.1016/0375-9474(74)90392-3
1974WE02 Nucl.Phys. A219, 450 (1974) Charge Distributions of the Isobar Pair 40Ar-40Ca from a Phenomenological and a Model-Independent Analysis of Elastic Electron Scattering NUCLEAR REACTIONS 40Ar(e, e), E=248 MeV; measured σ(Ee, θ). 40Ar deduced charge distribution parameters. Natural target.
doi: 10.1016/0375-9474(74)90111-0
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