NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = H.Dinter Found 11 matches. 2000DI26 Nucl.Instrum.Methods Phys.Res. A455, 460 (2000) H.Dinter, A.Leuschner, K.Tesch, D.Dworak, J.Loskiewicz Calculation of Hadron Yields Around Thick Targets and Doses Behind Concrete Shielding of High-Energy Electron Accelerators NUCLEAR REACTIONS 27Al, Cu, Nb, Pb(e, X), E=1-250 GeV; calculated neutron, proton, pion thick-target yields, spectra. Shielding requirements for electron accelerators discussed.
doi: 10.1016/S0168-9002(00)00511-8
1977BL02 Phys.Rev. C15, 988 (1977) I.Blomqvist, P.Janecek, G.G.Jonsson, H.Dinter, K.Tesch, N.Freed, P.Ostrander Electroproduction and Photoproduction of Charged Pions on 27Al and 51V At Intermediate Energies NUCLEAR REACTIONS 27Al, 51V(γ, π+), (e, e'π+), 51V(γ, π-), (e, e'π-), E=130-580 MeV; measured σ. Activation method. Ge(Li) detector.
doi: 10.1103/PhysRevC.15.988
1976BL09 Z.Phys. A278, 83 (1976) I.Blomqvist, P.Janecek, G.G.Jonsson, R.Petersson, H.Dinter, K.Tesch Electro- and Photoinduced Spallation Reactions on 27Al and 51V at Intermediate Energies NUCLEAR REACTIONS 27Al(e, e'n2p), (γ, n2p), 51V(e, e'2n2p), (γ, 2n2p), 51V(e, e'3n), (γ, 3n), (e, e'3n2p), (γ, 3n2p), (e, e'5n2p), (γ, 5n2p), (e, e'6n6p), (γ, 6n6p), (e, e'2n4p), (γ, 2n4p), (e, e'11n6p), (γ, 11n6p), (e, e'π-2n), (γ, π-2n), E < 1000 MeV; measured spallation yields.
doi: 10.1007/BF01547345
1974HE17 Nucl.Phys. A228, 478 (1974) F.H.Heimlich, E.Rossle, M.Kobberling, J.Moritz, K.H.Schmidt, D.Wegener, D.Zeller, J.K.Bienlein, J.Bleckwenn, H.Dinter Quasi-Elastic Electron Scattering (e, e'p) and (e, e'd) from 6Li in a Coincidence Experiment NUCLEAR REACTIONS 6Li(e, e'p), (e, e'd), E=2.5, 2.7 GeV; measured σ(E, Ep, θ(p)), σ(E, Ed, θ(d)); deduced momentum distributions. Enriched target.
doi: 10.1016/0375-9474(74)90616-2
1974HE20 Nucl.Phys. A231, 509 (1974) F.H.Heimlich, M.Kobberling, J.Moritz, K.H.Schmidt, D.Wegener, D.Zeller, J.K.Bienlein, J.Bleckwenn, H.Dinter High-Energy Electron Scattering from 6Li and 12C NUCLEAR REACTIONS 6Li, 12C(e, e'), E=2.5, 2.7 GeV; measured σ(Ee', θ); deduced effective A for quasielastic scattering, excitation of Δ(1236). Enriched target.
doi: 10.1016/0375-9474(74)90514-4
1974KO21 Nucl.Phys. A231, 504 (1974) M.Kobberling, J.Moritz, K.H.Schmidt, D.Wegener, D.Zeller, J.K.Bienlein, J.Bleckwenn, H.Dinter, F.H.Heimlich Momentum Distribution of Bound State Protons Derived from Quasi-Free Electron Scattering on 12C NUCLEAR REACTIONS 12C(e, e'p), E=2.5, 2.7 GeV; measured σ(Ee', θ(p)); deduced momentum distribution of protons.
doi: 10.1016/0375-9474(74)90513-2
1968DI03 Nucl.Phys. A111, 360(1968) Gammaspektren und Wirkungsquerschnitte beim Einfang von 14 MeV Neutronen in 27Al und 127I NUCLEAR REACTIONS 27Al, 127I(n, γ), E=14 MeV; measured σ(Eγ); deduced reaction mechanism. Natural targets.
doi: 10.1016/0375-9474(68)90130-9
1968HO04 Phys.Letters 26B, 378 (1968) A.Hofmann, W.Emmerich, H.Dinter, G.Philipp Abhangigkeit des Wirkungsquerschnitts fur 27Al(d, α)25Mg von Den Rotationszustanden des 25Mg NUCLEAR STRUCTURE 25Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90618-7
1968HO14 Nucl.Phys. A113, 86(1968) A.Hofmann, W.Emmerich, H.Dinter, G.Philipp Die Reaktion 27Al(d, α)25Mg NUCLEAR REACTIONS 27Al(d, α), E=4.74, 9.2, 10.1 MeV; measured σ(E;Eα, θ). 25Mg deduced levels, σ direct, reaction mechanism.
doi: 10.1016/0375-9474(68)90885-3
1966CL02 Nucl.Phys. 81, 155(1966) Die Halbwertszeit von 8Li RADIOACTIVITY 8Li[from 7Li(d, p)]; measured T1/2; deduced log ft.
doi: 10.1016/0029-5582(66)90648-1
1964BI11 Nucl. Phys. 55, 113 (1964) Gamma-Spektroskopie beim Zerfall Mn56 → Fe56 RADIOACTIVITY 56Mn[from 56Fe(n, p)]; measured T1/2, Eγ, Iγ, γγ. 56Mn deduced Iβ. Natural target.
doi: 10.1016/0029-5582(64)90131-2
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