NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.Uberall Found 39 matches. 1988ST07 Phys.Lett. 205B, 183 (1988) A.J.Stoyanov, A.Nagl, H.Uberall Excitation of the 15.11 MeV Level in 12C by Pion Scattering NUCLEAR REACTIONS 12C(e, e'), E not given; calculated form factors; deduced transition densities. 12C(π+, π+'), E=180-260 MeV; analyzed σ(θ). Transition densities from (e, e') analysis.
doi: 10.1016/0370-2693(88)91645-0
1986FA12 Phys.Rev. C34, 2134 (1986) A.R.Farhan, B.J.Stoyanov, A.Nagl, H.Uberall, M.de Llano Resonating Rays in Ion-Ion Scattering from an Optical Potential NUCLEAR REACTIONS 40Ca(α, α), E ≤ 44 MeV; calculated scattering amplitudes, σ(E, θ); deduced optical potential resonances. Wentzel-Kramers-Brillouin approximation.
doi: 10.1103/PhysRevC.34.2134
1984MO13 Can.J.Phys. 62, 771 (1984) J.A.Montgomery, H.Uberall, Kwang-Bock Yoo All-Multipolarity Electric Sum Rule NUCLEAR STRUCTURE 12C, 16O; calculated electric multipole transition sum rule fraction, Helm model parameters, nuclear moments. Electric sum rule for nonmonopole transitions.
doi: 10.1139/p84-106
1983GI02 Phys.Rev. C27, 1169 (1983) V.Girija, V.Devanathan, A.Nagl, H.Uberall Coherent Pion Photoproduction NUCLEAR REACTIONS 4He(γ, π0), E=200-350 MeV; 12C(γ, π0), E=170-380 MeV; calculated σ(E), σ(θ). 16O(γ, π0), E=250, 290, 370 MeV; 40Ca(γ, π0), E=250 MeV; calculated σ(θ). DWIA, coherent production mechanism.
doi: 10.1103/PhysRevC.27.1169
1981MO21 Can.J.Phys. 59, 1194 (1981) J.A.Montgomery, J.P.Ertel, H.Uberall High-multipolarity Magnetic Sum Rule NUCLEAR STRUCTURE 12C, 16O, 24Mg, 58Ni; calculated magnetic multipole transitions, sum rule exhaustion fraction for L=2, 3, 4, 6, 8, charge moment distributions. Helm model, spin-flip effects.
doi: 10.1139/p81-157
1981UB01 Nucl.Phys. A362, 241 (1981) H.Uberall, A.R.Farhan, O.Dragun, E.Maqueda Nuclear Surface Waves in Alpha-Particle and Ion-Ion Collisions NUCLEAR REACTIONS 40Ca(α, α), E=10-50 MeV; calculated σ(θ, E), transmission coefficient vs L, E. Nuclear surface wave approach.
doi: 10.1016/0375-9474(81)90679-5
1980DR08 Phys.Lett. B94, 24 (1980) Nuclear Rayleigh and Whispering Gallery Waves Excited in Heavy Ion Collisions NUCLEAR REACTIONS 12C(16O, 16O), (12C, 12C), E(cm)=15-35 MeV; 28Si(16O, 16O), E=20-50 MeV; analyzed σ(E); calculated dispersion curves. 28Si, 24Mg, 44Ti resonances deduced surface wave character. Rayleigh, Whispering Gallery waves, curved boundaries.
doi: 10.1016/0370-2693(80)90816-3
1980FA13 Nuovo Cim. A57, 205 (1980) A.R.Farhan, H.Uberall, O.Dragun, E.Maqueda A Nuclear-Surface-Wave Interpretation of Quasi-Molecular Orbiting in Heavy-Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=12-25 MeV; calculated dispersion curves; deduced surface wave nature of quasimolecular orbiting. Regge pole features, Rayleigh, whispering gallery type waves.
doi: 10.1007/BF02776453
1980GR05 Can.J.Phys. 58, 48 (1980) R.D.Graves, B.A.Lamers, A.Nagl, H.Uberall, V.Devanathan, P.R.Subramanian Helm Model Interpretation of 16O Form Factors: Application to Pion Photoproduction and Muon Capture NUCLEAR REACTIONS 16O(γ, π+), E=130-300 MeV; calculated σ(θ, E). 16O(μ-, ν), E at rest; calculated muon capture rates. Helm model, electron scattering data parameters.
doi: 10.1139/p80-009
1980NA11 Phys.Lett. B96, 254 (1980) Theory of Pion Photoproduction in 12C NUCLEAR REACTIONS 12C(γ, π-), E=threshold-360 MeV; calculated σ(E(π-)); 12C(γ, π+), E=threshold-7 MeV above threshold, 195, 200 MeV; calculated σ(θ). Helm model, pion optical-model wave functions.
doi: 10.1016/0370-2693(80)90760-1
1979MI06 Phys.Rev. C19, 1416 (1979) F.L.Milder, E.C.Booth, B.Chasan, A.M.Bernstein, J.Comuzzi, G.Franklin, A.Nagl, H.Uberall Positive-Pion Photoproduction on 12C Near Threshold NUCLEAR REACTIONS 12C(γ, π+), E=bremsstrahlung endpoint to 175 MeV; deduced σ(E); calculated σ(E), DWIA.
doi: 10.1103/PhysRevC.19.1416
1977AL18 Phys.Rev. C16, 503 (1977) D.J.Albert, A.Nagl, J.George, R.F.Wagner, H.Uberall Isospin Splitting of Giant Resonances in 13C and 17O NUCLEAR REACTIONS 13C, 17O(γ, X); calculated σ. 13C, 17O; calculated resonances, T. Two-particle, one-hole shell model.
doi: 10.1103/PhysRevC.16.503
1977AL32 Phys.Rev. C16, 2452 (1977) D.J.Albert, J.George, H.Uberall Shell-Model Study of the Giant Dipole States in 15N NUCLEAR REACTIONS 15N(γ, p), (γ, n), (γ, d); calculated total σ.
doi: 10.1103/PhysRevC.16.2452
1977LA04 Nucl.Phys. A280, 351 (1977) J.B.Langworthy, B.A.Lamers, H.Uberall Inelastic Neutrino Reactions on 16O NUCLEAR REACTIONS 16O(ν, e), E < 500 MeV; calculated differential, total neutrino induced σ(E).
doi: 10.1016/0375-9474(77)90610-8
1976NA16 Phys.Lett. 63B, 291 (1976) Calculation of π- Photoproduction in 12C Leading to the 12N Ground State NUCLEAR REACTIONS 12C(γ, π-), E=150-350 MeV; calculated yields.
doi: 10.1016/0370-2693(76)90266-5
1975DE18 Phys.Lett. 57B, 241 (1975) V.Devanathan, P.R.Subramanian, R.D.Graves, H.Uberall Partial Muon Capture Rates in 12C from the Generalized Helm Model NUCLEAR REACTIONS 12C(μ-, ν); calculated partial capture rates.
doi: 10.1016/0370-2693(75)90065-9
1975MU02 Phys.Rev. C11, 829 (1975) Eikonal Calculations for High-Energy Electron-Nucleus Scattering NUCLEAR REACTIONS 27Al, 115In, 208Pb(e, e'), E=500 MeV; 51V(e, e'), E=250 MeV; 209Bi(e, e'), E=300 MeV; calculated σ. 27Al, 208Pb, 51V, 209Bi deduced magnetic form factors.
doi: 10.1103/PhysRevC.11.829
1975NA16 Phys.Rev. C12, 1586 (1975) Distorted-Wave Approximation and Nuclear Correlations in Pion Reactions NUCLEAR REACTIONS 12C(γ, π-); calculated σ(θ). Distorted pion wave.
doi: 10.1103/PhysRevC.12.1586
1975UB01 Acta Phys.Austr. 41, 341 (1975) H.Uberall, A.Nagl, R.A.Lindgren, L.W.Fagg Giant Multipole Spin Flip Resonances and Spin Flip Sum Rules NUCLEAR REACTIONS 20Ne, 24Mg, 58Ni(e, e'), E=60 MeV; 12C, 24Mg, 58Ni(e, e'), E=100, 200, 300 MeV; calculated σ. 12C, 24Mg, 58Ni calculated E2 spin flip strengths.
1974CA21 Can.J.Phys. 52, 1405 (1974) F.Cannata, B.A.Lamers, C.W.Lucas, A.Nagl, H.Uberall, C.Werntz, F.J.Kelly Radiative Pion Capture in Flight and Charged Pion Photoproduction in Nuclei NUCLEAR REACTIONS 12C(γ, π+), E=160, 170, 180 MeV; 12C(π, γ), E=20, 30, 40 MeV; calculated σ(θ).
doi: 10.1139/p74-187
1974SE02 Nucl.Phys. A219, 461 (1974) J.B.Seaborn, V.Devanathan, H.Uberall Helm-Model and Shell-Model Studies of the Photoproduction of Charged Pions in 12C NUCLEAR REACTIONS 12C(γ, π+), (γ, π-); calculated σ.
doi: 10.1016/0375-9474(74)90112-2
1973MU08 Phys.Lett. 44B, 347 (1973) Eikonal Approximation for Magnetic Electron Scattering NUCLEAR REACTIONS 209Bi(e, e); calculated magnetic form factors.
doi: 10.1016/0370-2693(73)90403-6
1973NA14 Phys.Lett. 45B, 99 (1973) Pion Photoproduction and T > Versus T < Analog States in N > Z Nuclei NUCLEAR REACTIONS 13C(γ, π+), (γ, π-), E=200 MeV; measured nothing, calculated σ(θ).
doi: 10.1016/0370-2693(73)90074-9
1973UB01 Phys.Lett. 44B, 324 (1973) H.Uberall, B.A.Lamers, C.W.Lucas, A.Nagl Charged Pion Photoproduction from 12C with Excitation of Analog States NUCLEAR REACTIONS 12C(γ, π+), (γ, π-); 12B, 12N deduced levels, calculated σ(θ).
doi: 10.1016/0370-2693(73)90396-1
1973WE18 Z.Phys. 265, 405 (1973) Solar-Neutrino Related M1 Transition in 6Li NUCLEAR REACTIONS 6Li(e, e), E=50.4 MeV; calculated σ(θ). 6Li calculated levels, J, π, level-width, B(M1).
doi: 10.1007/BF01391615
1972HI04 Nucl.Phys. A190, 341 (1972) Spectra of Neutrons Emitted after Muon Capture in 16O, 28Si, 32S and 40Ca NUCLEAR REACTIONS 16O, 32S, 28Si, 40Ca(μ-, xn), E approx 0; calculated σ(En). Particle-hole model.
doi: 10.1016/0375-9474(72)90146-7
1972KE06 Phys.Rev. C5, 1432 (1972) Low-Energy Neutrino Excitation of the Giant Resonance in 12C NUCLEAR REACTIONS 12C(ν, e), calculated σ(Eν). 12C analyzed giant resonance excitation.
doi: 10.1103/PhysRevC.5.1432
1972UB01 Phys.Rev. C6, 1911 (1972) H.Uberall, B.A.Lamers, J.B.Langworthy, F.J.Kelly Multipole Theory of Neutrino-Nuclear Reactions: Application to 12C NUCLEAR REACTIONS 12C(ν, e), (ν, μ-), E < 53 MeV, approx GeV; calculated σ(θ). Multipole theory.
doi: 10.1103/PhysRevC.6.1911
1972UG01 Nucl.Phys. A198, 494 (1972) Nuclear Size Effects in the Polarization of Elastically Scattered Positrons
doi: 10.1016/0375-9474(72)90704-X
1971FA15 Phys.Rev. C4, 2089 (1971) L.W.Fagg, W.L.Bendel, L.Cohen, E.C.Jones, Jr., H.F.Kaiser, H.Uberall Magnetic Transition Strength in 32S and 40Ca from 180° Electron Scattering NUCLEAR REACTIONS 32S, 40Ca(e, e'), E=39, 56 MeV; measured σ(Ee'). 32S, 40Ca deduced levels, level-width, transition radii.
doi: 10.1103/PhysRevC.4.2089
1970LA13 Phys.Rev. C2, 911 (1970) Electron Scattering from Light, Deformed, Oriented Nuclei NUCLEAR REACTIONS 10B(e, e), (e, e'), E=50, 200 MeV; calculated form factors. Oriented targets.
doi: 10.1103/PhysRevC.2.911
1970UG01 Nucl.Phys. A158, 418 (1970) P.Ugincius, H.Uberall, G.H.Rawitscher Nuclear Size Effects in the Polarization of Elastically Scattered Electrons NUCLEAR REACTIONS 51V, 208Pb(e, e), E=1-100 MeV; calculated polarization functions(θ). Nuclear size effects.
doi: 10.1016/0375-9474(70)90193-4
1969DR05 Phys.Rev. 181, 1383 (1969) Particle and Photon Decay of Nuclei Following Electroexcitation NUCLEAR REACTIONS 12C(e, e'p), E = 200 MeV; calculated σ(Ee', θ(p), phi(p)).
doi: 10.1103/PhysRev.181.1383
1969KE12 Nucl.Phys. A139, 329 (1969) F.J.Kelly, L.J.McDonald, H.Uberall Inelastic Photopion Production with Excitation of Giant Resonance Analogs: Application to 16O NUCLEAR REACTIONS 16O(γ, π+), E=200 MeV; calculated σ(E(π), θ(π)). 16N deduced giant resonance spin-flip states.
doi: 10.1016/0375-9474(69)91113-0
1969UB01 Acta Phys.Austr. 30, 89 (1969) Analogs of Giant Resonance States and their Experimental Discovery NUCLEAR STRUCTURE 12B, 12C, 16O, 16N, 40Ca reviewed giant resonance analog data.
1968KE10 Phys.Rev. 175, 1235 (1968) Electroexcitation of the Giant Resonance in 12C NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.175.1235
1967HI07 Phys.Letters 24B, 364 (1967) Inelastic Electron Scattering in 32S NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90290-0
1967RA02 Phys.Letters 24B, 15 (1967) R.Raphael, H.Uberall, C.Werntz Neutron Emission Following Muon Capture in 16O NUCLEAR STRUCTURE 16O, 16N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90324-3
1966UB01 Phys.Rev.Letters 17, 1292 (1966) Electroexcitation of Giant-Resonance, Surface-Phonon States in 12C NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.1292
Back to query form |