NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = H.V.Geramb Found 33 matches. 1983PA08 Nucl.Phys. A403, 134 (1983) Elastic and Inelastic Scattering of 25.6 MeV Protons from Even Samarium Isotopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, p), (p, p'), E=25.6 MeV; measured σ(θ); deduced optical model potentials, deformation paramters. Enriched targets. Coupled-channels analysis, phenomenological, microscopic optical model potential comparison.
doi: 10.1016/0375-9474(83)90193-8
1979DE07 Phys.Rev. C19, 646 (1979) R.De Leo, G.D'Erasmo, A.Pantaleo, G.Pasquariello, G.Viesti, M.Pignanelli, H.V.Geramb 14-40 MeV Proton Scattering from Low-Lying States of 28Si NUCLEAR REACTIONS 28Si(p, p'γ), E=14-40 MeV; measured σ(Ep, θp', θγ=90°). 28Si levels deduced β(L), E1, E2, E3 giant resonance strength, optical-model parameters. Natural targets.
doi: 10.1103/PhysRevC.19.646
1979DE11 Can.J.Phys. 57, 540 (1979) R.de Swiniarski, Dinh-Lien Pham, G.Bagieu, H.V.Geramb Elastic and Inelastic Scattering of 40 MeV Polarized Protons from 90Zr and 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=40 MeV; measured σ(θ), A(θ). Microscopic, macroscopic, DWBA analysis, coupled-channels calculations with vibrational model.
1979DE20 Phys.Rev. C20, 13 (1979) R.De Leo, G.D'Erasmo, E.M.Fiore, A.Pantaleo, M.Pignanelli, H.V.Geramb Two-Step Effects in 15-35 MeV Proton Scattering from 24Mg Low-Lying States NUCLEAR REACTIONS 24Mg(p, p'), E=15-35 MeV; measured σ(θ); deduced optical model parameters. 24Mg levels deduced deformation parameters, reaction mechanism. Enriched target. Optical model, coupled-channels, compound nuclear model analysis.
doi: 10.1103/PhysRevC.20.13
1979GA13 Nucl.Phys. A327, 349 (1979) Y.R.Gaillard, P.Martin, G.Perrin, P.Desaintignon, M.Buenerd, J.M.Loiseaux, J.L.Escudie, A.Tarrats, H.V.Geramb Excitation Function of Giant Resonances as Doorway States in the 12C(P, P)12C Reaction between 19 and 23 MeV NUCLEAR REACTIONS 12C(p, p), E=19.15-23.34 MeV; measured σ(E, θ)A(E, θ). 13N deduced giant resonance strength distribution. Optical model, coupled channel, anti-symmetrized distorted-wave approximation.
doi: 10.1016/0375-9474(79)90264-1
1978BR30 Phys.Lett. 79B, 177 (1978) F.A.Brieva, H.V.Geramb, J.R.Rook A Realistic Complex Interaction for Elastic and Inelastic Nucleon Scattering NUCLEAR REACTIONS 27Al(p, n), E=40 MeV; calculated σ(θ) for 27Si ground state; 40Ca(p, p'), E=30, 35.8, 40 MeV; calculated σ(θ) for 3.74-MeV (3-) state in 40Ca. Complex nuclear t-matrix interaction.
doi: 10.1016/0370-2693(78)90216-2
1978BU27 Nuovo Cim. 48A, 100 (1978) A.Budzanowski, K.Grotowski, S.Micek, Z.Rogalska, A.Strzalkowski, E.Witkos, T.Delbar, G.Gregoire, J.Lega, G.Paic, P.Wastyn, H.V.Geramb Giant-Resonance Effects in the 12C(α, p)15N (3/2-, 6.328 MeV) Transition NUCLEAR REACTIONS 12C(α, p), E=24-33 MeV; measured σ(Ep, θp). 14N level deduced GQR effects, reaction mechanism.
doi: 10.1007/BF02786590
1978HE03 Z.Phys. A284, 413 (1978) E.F.Hefter, H.V.Geramb, F.Osterfeld, T.Udagawa Two-Step Processes in Inelastic Proton Scattering NUCLEAR REACTIONS 16O, 40Ca(p, p'), 16O(p, d), E=25-46 MeV; calculated σ(θ). Reaction mechanism study.
doi: 10.1007/BF01422110
1977PE09 Phys.Lett. 68B, 55 (1977) G.Perrin, D.Lebrun, J.Chauvin, P.Martin, P.De Saintignon, D.Eppel, H.V.Geramb, H.L.Yadav, V.A.Madsen The Octupole Giant Resonance Strength in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=42.5, 44.0, 49.3 MeV; measured σ(Ep', θ), A(θ). 16O deduced octupole strength.
doi: 10.1016/0370-2693(77)90033-8
1976AM02 Lett.Nuovo Cim. 16, 165 (1976) Strength Estimate of Inelastic Hadron Scattering to Giant Resonances in 16O NUCLEAR STRUCTURE 16O; calculated isoscalar resonance characteristics.
doi: 10.1007/BF02746958
1976DA17 Z.Phys. A278, 281 (1976) P.David, J.Debrus, H.Essen, F.Lubke, H.Mommsen, R.Schoenmackers, W.Soyez, H.V.v.Geramb, E.F.Hefter Elastic and Inelastic 4He-Scattering on 208Pb, 232Th and 234,236,238U NUCLEAR REACTIONS 208Pb, 232Th, 234,236,238U(α, α), (α, α'), measured E=50 MeV; measured σ(θ). 232Th, 234,236,238U deduced β.
doi: 10.1007/BF01409180
1976LE16 Nucl.Phys. A265, 291 (1976) D.Lebrun, G.Perrin, P.Martin, P.de Saintignon, J.Arvieux, M.Buenerd, H.V.Geramb, K.A.Amos Evidence of an Isoscalar E3 Giant Resonance in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=31.7, 33.8, 35.8, 36.8, 39.9 MeV; measured σ(Ep', θ), A(θ). 16O deduced isoscalar resonance, E3 strengths. Distorted wave analyses include giant resonance effects.
doi: 10.1016/0375-9474(76)90355-9
1976YA08 Phys.Rev. C14, 1369 (1976) Microscopic Study of Doorway States in the Giant Resonance Region of 16O NUCLEAR REACTIONS 16O(p, p'), E=24-40 MeV; calculated σ. Microscopic study, RPA wave functions.
doi: 10.1103/PhysRevC.14.1369
1975GE05 Nucl.Phys. A246, 173 (1975) Microscopic Analyses of Proton Inelastic Scattering by 16O and 40Ca Using a Complex t-Matrix NUCLEAR REACTIONS 16O, 40Ca(p, p'), E=25-61 MeV; calculated σ(Ep', θ).
doi: 10.1016/0375-9474(75)90570-9
1975GE15 Phys.Rev. C12, 1697 (1975) H.V.Geramb, K.Amos, R.Sprickmann, K.T.Knopfle, M.Rogge, D.Ingham, C.Mayer-Boricke Investigation of Giant Resonances as Doorway States in Inelastic Nucleon Scattering from 12C NUCLEAR REACTIONS 12C(p, p'), E=22.5-45 MeV; measured σ(E, Ep', θ). 12C deduced giant dipole, quadrupole strength distribution. DWBA analysis, resonance effects included.
doi: 10.1103/PhysRevC.12.1697
1975GE17 Lett.Nuovo Cim. 14, 526 (1975) Indication of E4 Giant-Resonance Strength NUCLEAR REACTIONS 89Y(p, p'), E=155 MeV; analyzed data, calculated σ(θ); deduced angular momentum transfer.
1975GE18 Z.Phys. A275, 373 (1975) H.V.Geramb, T.Terasawa, K.Amos An Estimate of Giant Resonance Effects in (α, p) Transitions NUCLEAR REACTIONS 16O(α, p), E=20 MeV; calculated contributions to 19F 110-keV state due to virtual formation of GQR as doorway state in semi-direct process.
1975NE08 Aust.J.Phys. 28, 659 (1975) P.Nesci, R.Smith, K.Amos, H.V.Geramb Shell Structure of the Even Tellurium Isotopes and Inelastic Proton Scattering NUCLEAR REACTIONS 122,126,128,130Te(p, p'), E=51.9 MeV; calculated σ(θ). Shell structure of Te isotopes.
doi: 10.1071/PH750659
1975SP07 Z.Phys. A274, 339 (1975) R.Sprickmann, K.T.Knopfle, D.Ingham, M.Rogge, C.Mayer-Boricke, H.V.Geramb Optical Model Analysis of Proton-Carbon Elastic Scattering in the Range 20 to 50 MeV NUCLEAR REACTIONS 12C(p, p), E=20-50 MeV; analyzed σ(E, θ).
doi: 10.1007/BF01434044
1974AM04 Z.Phys. 270, 149 (1974) Giant Multipole Resonance Effects in 27Al(p, n)27Si NUCLEAR REACTIONS 27Al(p, n), E=10-40 MeV; calculated σ(E, En, θ). 28Si giant resonances deduced coupling constants.
doi: 10.1007/BF01677446
1974AM05 Phys.Lett. 52B, 138 (1974) K.A.Amos, H.V.Geramb, R.Sprickmann, J.Arvieux, M.Buenerd, G.Perrin Resonance Effects in the 12C(p, p')12C*, 1+ Transition NUCLEAR REACTIONS 12C(polarized p, p'), E=22.3, 26.7, 30.5 MeV; measured σ(E, Ep', θ), A(E, θ). 12C deduced resonance coupling strengths.
doi: 10.1016/0370-2693(74)90071-9
1974GE04 Z.Phys. 267, 367 (1974) Inelastic Proton Scattering to the Lowest 1+ State in 58Ni NUCLEAR REACTIONS 58Ni(p, p'); measured nothing, calculated σ.
1974GE15 Nuovo Cim. 23A, 447 (1974) H.V.Geramb, G.L.Strobel, R.Sprickmann Giant-Dipole-Resonance Effects in the 90Zr(p, p') 0+1 to 0+2 Transition NUCLEAR REACTIONS 90Zr(p, p'), E=12.7, 18.8, 40 MeV; calculated σ(E, Ep', θ).
1974ME29 Nucl.Phys. A232, 472 (1974) G.Mertens, M.Thumm, H.V.Geramb Spin-Flip Probability in the Inelastic Scattering of 16.9 MeV Neutrons From 12C NUCLEAR REACTIONS 12C(n, n'γ), E=16.9 MeV; measured n'γ(θ); deduced neutron spin-flip probabilities. Polyvinyltoluene target. MADWBA analysis with resonance terms.
doi: 10.1016/0375-9474(74)90633-2
1973GE01 Nucl.Phys. A199, 545 (1973) H.V.Geramb, R.Sprickmann, G.L.Strobel Excitation of Giant Multipole Resonances L = 1-4 in the 16O(p, p') Spin-Flip Transition NUCLEAR REACTIONS 16O(p, p'), E=23-46 MeV; analyzed σ(E;θ) 17F deduced resonances, level-width.
doi: 10.1016/0375-9474(73)90597-6
1973GE07 Z.Phys. 261, 177 (1973) Excitation of Giant Multipole Resonances L = 1, 2 and 3 in the 16O(p, 2p) Reaction NUCLEAR REACTIONS 16O(p, 2p), E=45 MeV; measured nothing, calculated giant multipole resonances, σ(θ).
1973ST16 Nucl.Phys. A210, 67 (1973) The Continuous 3He Spectrum from Deuterons Incident on 12C NUCLEAR REACTIONS 12C(d, 3He), E=52 MeV; calculated σ(E(3He)).
doi: 10.1016/0375-9474(73)90504-6
1972GE01 Nucl.Phys. A183, 582 (1972) Features of Core Polarization Knock-Out Exchange Contributions to Inelastic Nucleon Scattering NUCLEAR REACTIONS 89Y(p, p'), E=24 MeV; calculated core polarization σ(θ). Collective virtual core excitation model.
doi: 10.1016/0375-9474(72)90356-9
1972GE07 Phys.Lett. 39B, 611 (1972) Two Step Process in the 16O(p, 2p)15N Reaction NUCLEAR REACTIONS 16O(p, 2p), E=45 MeV; calculated σ(Ep, θ(p)). 2-step mechanism, core polarization term.
doi: 10.1016/0370-2693(72)90010-X
1972GE16 Lett.Nuovo Cim. 5, 333 (1972) H.V.Geramb, G.L.Strobel, R.Sprickmann Evidence for Core Polarization Exchange Contribution in Inelastic Scattering
1971GE03 Nucl.Phys. A163, 337 (1971) Antisymmetrized Distorted Wave Theory of Inelastic Nucleon Scattering NUCLEAR REACTIONS 89Y(p, p'), E=18.8, 24.5, 61.2 MeV; measured nothing; analyzed σ(θ). Antisymmetrized DW theory.
doi: 10.1016/0375-9474(71)90495-7
1971GE12 Phys.Lett. 37B, 351 (1971) A Microscopic Analysis of 13C(p, n)13N(gs), Including the Core Polarization Exchange Process NUCLEAR REACTIONS 13C(p, n), E=12.2, 13.3 MeV; calculated σ(θ). Antisymmetrized DWBA, core polarization exchange.
doi: 10.1016/0370-2693(71)90199-7
1970GE11 Phys.Lett. 32B, 665 (1970) Proton Scattering to the 3/2- State of 207Pb NUCLEAR REACTIONS 207Pb(p, p'), E=20.2 MeV; measured nothing; analyzed σ(θ).
doi: 10.1016/0370-2693(70)90438-7
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