NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = H.V.Von Geramb Found 34 matches. 2020VO14 Eur.Phys.J. A 56, 282 (2020) Intricate partial waves in nuclear scattering
doi: 10.1140/epja/s10050-020-00284-9
2011MA44 Int.J.Mod.Phys. E20, 1817 (2011) S.E.Massen, V.P.Psonis, H.V.Von Geramb Augmentation of nucleon-nucleus scattering by information entropy
doi: 10.1142/S0218301311019647
2005AR20 Phys.Rev. C 72, 025203 (2005) Microscopic analysis of K+-nucleus elastic scattering based on K+-nucleon phase shifts NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, K+), E at 400-1000 MeV/c; analyzed kaon-nucleon phase shifts; calculated σ(θ). Microscopic optical model approach, comparison with data.
doi: 10.1103/PhysRevC.72.025203
2002AN03 Phys.Rev. C65, 024306 (2002) A.N.Antonov, M.K.Gaidarov, M.V.Ivanov, D.N.Kadrev, G.Z.Krumova, P.E.Hodgson, H.V.von Geramb Nucleon Momentum Distribution in Deuteron and Other Nuclei within the Light-Front Dynamics Method NUCLEAR STRUCTURE 2H, 4He, 12C, 56Fe; calculated nucleon momentum distributions. Light-front dynamics model.
doi: 10.1103/PhysRevC.65.024306
2002AR14 Phys.Rev. C66, 024602 (2002) Extension of the full-folding optical model for nucleon-nucleus scattering with applications up to 1.5 GeV NUCLEAR REACTIONS 16O, 40Ca, 90Zr, 208Pb(n, n), (p, p), E=100-1500 MeV; calculated total σ. 40Ca, 208Pb(p, p), E=300-1040 MeV; calculated σ(θ), analyzing power vs momentum transfer. Relativistic full-folding optical model approach, comparisons with data.
doi: 10.1103/PhysRevC.66.024602
2001FU17 Phys.Rev. C64, 054003 (2001) A.Funk, H.V.von Geramb, K.A.Amos Nucleon-Nucleon Optical Model for Energies up to 3 GeV NUCLEAR REACTIONS 1H(n, X), E=0-3 GeV; calculated phase shifts, related features. Several nucleon-nucleon potentials compared.
doi: 10.1103/PhysRevC.64.054003
1998JA01 Phys.Rev. C57, 496 (1998) Nucleon-Nucleon Scattering Observables from Solitary Boson Exchange Potential NUCLEAR REACTIONS 1H(polarized p, p), (polarized n, n), E < 300 MeV; analyzed total σ, σ(θ), polarization observables; deduced scaling law. One solitary boson exchange potential.
doi: 10.1103/PhysRevC.57.496
1998VO11 Phys.Rev. C58, 1948 (1998) H.V.von Geramb, K.A.Amos, H.Labes, M.Sander Analysis of NN Amplitudes Up to 2.5 GeV: An optical model and geometric interpretation NUCLEAR REACTIONS 1n, 1H(p, X), E < 2.5 GeV; analyzed partial wave amplitudes; deduced optical model potential strengths.
doi: 10.1103/PhysRevC.58.1948
1997JA01 Phys.Rev. C55, 57 (1997) Nonlinear Approach to NN Interactions using Self-Interacting Meson Fields NUCLEAR STRUCTURE 2H; calculated binding energy, μ, quadrupole moment, D-/S-state ratio, rms radius, D-state probability. Self-interacting meson fields, nonlinear approach to NN-interactions. NUCLEAR REACTIONS 1H(n, n), E ≤ 300 MeV; calculated phase shifts vs E. Self-interacting meson fields, nonlinear approach to NN-interactions.
doi: 10.1103/PhysRevC.55.57
1997SA41 Phys.Rev. C56, 1218 (1997) ππ, Kπ, and πN Potential Scattering and a Prediction of a Narrow σ Meson Resonance
doi: 10.1103/PhysRevC.56.1218
1996AR13 Phys.Rev. C54, 2570 (1996) H.F.Arellano, F.A.Brieva, M.Sander, H.V.von Geramb Sensitivity of Nucleon-Nucleus Scattering to the Off-Shell Behavior of On-Shell Equivalent NN Potentials NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=40-500 MeV; 208Pb(polarized p, p), (p, p), E=400 MeV; analyzed σ(θ), analyzing power vs θ; deduced sensitivity to off-shell behavior of on-shell equivalent. NN-potentials.
doi: 10.1103/PhysRevC.54.2570
1996SA12 Phys.Rev. C53, R2610 (1996) M.Sander, C.Kuhrts, H.V.von Geramb Theoretical Predictions for Pionium Searches
doi: 10.1103/PhysRevC.53.R2610
1995GI01 Phys.Rev. C51, R465 (1995) B.F.Gibson, H.Kohlhoff, H.V.von Geramb Inversion Potential Analysis of the Nuclear Dynamics in the Triton NUCLEAR STRUCTURE 3H; calculated binding energy. 2H; calculated binding energy, D-state probability, quadrupole moment, rms radius, asymptotic parameters. Inversion potentials.
doi: 10.1103/PhysRevC.51.R465
1994JE01 Phys.Rev. C49, 1832 (1994) Nucleon-Nucleon Potentials and Their Test with Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), (polarized p, γ), E=157, 294 MeV; analyzed σ(θ1, θ2, θγ), polarization data. Nucleon-nucleon bremsstrahlung, complete potential model.
doi: 10.1103/PhysRevC.49.1832
1994KA12 Phys.Rev. C49, 2342 (1994) A.Katsogiannis, K.Amos, M.Jetter, H.V.von Geramb Coulomb Correction Calculations of pp Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), (polarized p, γ), E=5-280 MeV; analyzed bremsstrahlung σ(θ1, θ2, θγ), analyzing power data; deduced Coulomb interaction effects. Coulomb T-matrices, off-shell properties included.
doi: 10.1103/PhysRevC.49.2342
1993JE01 Nucl.Phys. A553, 655c (1993) M.Jetter, H.Freitag, H.V.von Geramb Studies of Nucleon-Nucleon Potentials with pp- and np-Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), E=280 MeV; analyzed bremsstrahlung σ(θ) data; deduced two-nucleon t-matricies properties. Potential model formalism.
doi: 10.1016/0375-9474(93)90674-M
1993JE04 Phys.Scr. 48, 229 (1993) M.Jetter, H.Freitag, H.V.von Geramb Half Off-Shell T-Matrix Studies with pp-Bremsstrahlung NUCLEAR REACTIONS 1H(p, X), E=280 MeV; calculated coplanar σ, analyzing power for pp bremsstrahlung. Half off-shell T-matrix.
doi: 10.1088/0031-8949/48/2/021
1993KO30 Phys.Scr. 48, 238 (1993) H.Kohlhoff, M.Kuker, H.Freitag, H.V.von Geramb Nucleon-Nucleon Potentials from Inversion NUCLEAR STRUCTURE 2H; calculated D-state probability, μ, rms radius, quadrupole moment, wave function. NN potentials from quantum inversion theory, partial wave phase shifts analysis.
doi: 10.1088/0031-8949/48/2/022
1989MA24 Nucl.Phys. A493, 412 (1989) A Microscopic Analysis of Antiproton-Nucleus Inelastic Scattering at 600 MeV/c NUCLEAR REACTIONS 12C(p-bar, p-bar'), E=179.6 MeV; 18O(p-bar, p-bar'), E=180 MeV; calculated σ(θ). Microscopic model.
doi: 10.1016/0375-9474(89)90095-X
1988IN01 Phys.Scr. 37, 530 (1988) Inelastic Antiproton Scattering to 02+ State in Carbon NUCLEAR REACTIONS 12C(p-bar, p-bar), (p-bar, p-bar'), E=180 MeV; calculated σ(θ). Coupled-channels formalism.
doi: 10.1088/0031-8949/37/4/003
1988LE10 Phys.Lett. 205B, 219 (1988) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen, H.V.von Geramb Intermediate Energy Proton Scattering from 40Ca, 90Zr and 208Pb NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(polarized p, p), E=200, 362, 400 MeV; measured σ(θ), analyzing power vs θ, spin rotation parameter vs θ.
doi: 10.1016/0370-2693(88)91653-X
1987AD04 Nucl.Phys. A470, 461 (1987) Microscopic Analysis of Antiproton-Nucleus Elastic Scattering NUCLEAR REACTIONS 12C(p-bar, p-bar), E at 300, 600 MeV/c; 40Ca, 208Pb(p-bar, p-bar), E at 600 MeV/c; analyzed σ(θ); deduced model parameters, medium effects. Microscopic optical model.
doi: 10.1016/0375-9474(87)90581-1
1987CO13 Z.Phys. A326, 345 (1987) M.Coz, J.Kuberczyk, H.V.von Geramb Nucleon Nucleon Interaction Potential from Experimental Phase Shifts NUCLEAR REACTIONS 1n(p, p), E ≤ 2000 MeV; analyzed phase shifts; deduced nucleon-nucleon interaction potential.
1987KU20 Z.Phys. A328, 265 (1987) J.Kuberczyk, M.Coz, H.V.von Geramb, J.D.Lumpe Neutron Proton Interaction Potentials from Experimental Phase Shifts NUCLEAR REACTIONS 1H(n, n), 1H(p, p), E not given; analyzed phase shifts; deduced interaction potentials. Marchenko inverse scattering technique.
1986MI06 Phys.Lett. 169B, 166 (1986) C.A.Miller, A.Scott, R.Abegg, R.Helmer, K.P.Jackson, M.Whiten, S.Yen, L.Lee, T.E.Drake, D.Frekers, S.S.M.Wong, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Dymarz, H.V.von Geramb, C.J.Horowitz Large Angle Elastic Scattering of 200 MeV Protons from 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced exchange medium effects role. Microscopic Schrodinger, relativistic impulse approximation analyses.
doi: 10.1016/0370-2693(86)90643-X
1985VO06 Lett.Nuovo Cim. 42, 209 (1985) H.V.von Geramb, K.Nakano, L.Rikus Microscopic Analysis of Antiproton Scattering from Carbon NUCLEAR REACTIONS 12C(p-bar, p-bar), E at 300 MeV/c; analyzed data. Paris, Bryan-Phillips potentials, microscopic model.
doi: 10.1007/BF02739457
1984RI03 Nucl.Phys. A414, 413 (1984) L.Rikus, K.Nakano, H.V.Von Geramb Microscopic Analysis of Elastic and Inelastic Proton Scattering from 12C NUCLEAR REACTIONS 12C(p, p), (p, p'), (polarized p, p), (polarized p, p'), E=122-400 MeV; calculated σ(θ), polarization, analyzing power, spin flip probability vs θ. First-principle optical potentials, distorted wave inelastic transition amplitude.
doi: 10.1016/0375-9474(84)90611-0
1984RI14 Nucl.Phys. A426, 496 (1984) Microscopic Analyses of Proton Scattering from Lead NUCLEAR REACTIONS 207Pb(p, p), E=134.8, 198.6 MeV; 208Pb(p, p), E=134.8-400 MeV; calculated σ(θ), P(θ). Microscopic optical potentials, Paris nucleon-nucleon potential.
doi: 10.1016/0375-9474(84)90160-X
1983BA25 Phys.Rev. C27, 2466 (1983) W.Bauhoff, H.V.von Geramb, G.Palla Nonlocal and Local Equivalent Microscopic Optical Potentials NUCLEAR REACTIONS 12C(p, p), E=40, 180, 200 MeV; 40Ca(p, p), E=160, 180 MeV; calculated σ(θ); deduced potential parameters. Microscopic, nonlocal, nucleon-nucleus optical model.
doi: 10.1103/PhysRevC.27.2466
1983CE02 Nucl.Phys. A396, 281c (1983) E.Cereda, M.Pignanelli, S.Micheletti, H.V.Von Geramb, M.N.Harakeh, R.De Leo, G.D'Erasmo, A.Pantaleo A Study of Proton Scattering on A = 92-116 Nuclei with Extended Optical Models and the Interacting Boson Approximation NUCLEAR REACTIONS 92,94,96,98,100Mo, 106,108,110Pd, 102Ru, 106,110,112,116Cd(p, p'), E=22.3 MeV; measured σ(θ). 104Pd(p, p'), E=10-35 MeV; measured σ(θ) vs E. Extended optical model analysis, interacting boson approximation.
doi: 10.1016/0375-9474(83)90025-8
1982CE04 Phys.Rev. C26, 1941 (1982) E.Cereda, M.Pignanelli, S.Micheletti, H.V.von Geramb, M.N.Harakeh, R.De Leo, G.D'Erasmo, A.Pantaleo Proton Scattering on A = 92-116 Nuclei with Extended Optical Models and the Interacting Boson Approximation NUCLEAR REACTIONS 92,94,96,98,100Mo, 102Ru, 106,110,112,116Cd, 104,106,108,110Pd(p, p), (p, p'), E=22.3 MeV; 104Pd(p, p), (p, p'), E=10.25, 12.1, 15, 17.3, 22.3, 30.2, 35.4 MeV; measured σ(θ); deduced optical model parameters. 92,94,96,98,100Mo, 102Ru, 104,106,108,110Pd, 106,110,112,116Cd deduced β2, β3. Optical model, coupled-channels analyses, interacting boson model form factors.
doi: 10.1103/PhysRevC.26.1941
1982PA13 J.Phys.(London) G8, 1007 (1982) G.Palla, H.V.von Geramb, G.Lindstrom Two-Step Processes in (p, t) Reactions on Even Sm Isotopes NUCLEAR REACTIONS 144,148,150,154Sm(p, t), E=25.5 MeV; analyzed σ(θ); deduced higher order inelastic processes role. 142,146,148,152Sm levels deduced spectroscopic data, configuration. CCBA, single, multi-step mechanisms.
doi: 10.1088/0305-4616/8/7/017
1981PI11 Phys.Rev. C24, 369 (1981) M.Pignanelli, H.V.von Geramb, R.De Leo Feedback of Giant Resonances on Optical Model Potentials NUCLEAR REACTIONS 16,18O, 24Mg, 40Ar, 40Ca(p, p), E=21-48 MeV; calculated σ(θ); deduced strong coupling to giant multipole resonances. Optical model, coupled-channels calculations.
doi: 10.1103/PhysRevC.24.369
1980FO15 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 2388 (1980) H.V.Von Geramb, K.A.Gridnev, P.P.Zarubin Analysis of Proton Scattering by Even Palladium Isotopes near E(p) = 6 MeV NUCLEAR REACTIONS 102,104,106,108,110Pd(p, p), (p, p'), E=6 MeV; analyzed σ(θ); deduced optical model parameters. 102,104,106,108,110Pd level deduced β2. Optical, Hauser-Feshbach, DWBA, coupled-channel model analyses.
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