NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Wienhard Found 26 matches. 1984BE26 Phys.Lett. 140B, 191 (1984) U.E.P.Berg, K.Ackermann, K.Bangert, C.Blasing, W.Naatz, R.Stock, K.Wienhard, M.K.Brussel, T.E.Chapuran, B.H.Wildenthal Bound State M1 Transitions in sd-Shell Nuclei NUCLEAR REACTIONS 20,22Ne, 24Mg, 28,30Si, 32,34S(γ, γ'), E=65 MeV bremsstrahlung; 26Mg(γ, γ'), E not given; measured Eγ, Iγ. 22Ne, 26Mg, 28,30Si, 32,34S(polarized γ, γ), E=22 MeV bremsstrahlung; measured γ asymmetry, polarization effect. 20,22Ne, 24,26Mg, 28,30Si, 32,34S levels deduced B(M1), (Γ0/Γ), Γ0. Nuclear resonance fluorescence technique, linearly polarized γ-beam. Shell model comparison.
doi: 10.1016/0370-2693(84)90918-3
1984CA34 Phys.Lett. 146B, 179 (1984) J.R.Calarco, J.Arruda-Neto, K.A.Griffioen, S.S.Hanna, D.H.H.Hoffmann, B.Neyer, R.E.Rand, K.Wienhard, M.R.Yearian Observation of Monopole Strength in the 12C(e, e'p0)11B Reaction NUCLEAR REACTIONS 12C(e, e'p), E=86, 118, 126 MeV; measured σ(E(e'), θ(e'), θp), forward, backward asymmetry. 12C deduced possible monopole resonance, EWSR.
doi: 10.1016/0370-2693(84)91012-8
1983BE19 Phys.Rev. C27, 2981 (1983) U.E.P.Berg, K.Ackermann, K.Bangert, R.Stock, K.Wienhard 11262 keV 1+ State in 20Ne NUCLEAR REACTIONS 20Ne(γ, γ'), E < 18 MeV bremsstrahlung; measured Eγ, Iγ. 20Ne deduced level, relative γ-branching. Natural Ne target.
doi: 10.1103/PhysRevC.27.2981
1982BA03 Nucl.Phys. A376, 15 (1982) K.Bangert, U.E.P.Berg, G.Junghans, R.Stock, K.Wienhard Charged Photoparticles from the 18O Giant Resonances NUCLEAR REACTIONS 18O(γ, p), (γ, d), (γ, t), (γ, α), E=24, 32 MeV bremsstrahlung; measured σ(Ep), σ(Ed), σ(Et), σ(Eα); deduced σ(Eγ, θ) following t, α emission. 18O deduced giant resonance decay characteristics.
doi: 10.1016/0375-9474(82)90530-9
1982RA21 Z.Phys. A308, 63 (1982) R.Ratzek, W.Wilke, J.Drexler, R.Fischer, R.Heil, K.Huber, U.Kneissl, H.Ries, H.Stroher, R.Stock, K.Wienhard Photofission with Linearly Polarized Photons NUCLEAR REACTIONS 232Th(polarized γ, F), (γ, F), E=10, 12 MeV bremsstrahlung; measured fission σ(fragment θ), asymmetry. 232Th deduced E1 excitation role in fission. Linearly polarized beam, parallel plate avalanche detectors.
doi: 10.1007/BF01415850
1982WI06 Phys.Rev.Lett. 49, 18 (1982) K.Wienhard, K.Ackermann, K.Bangert, U.E.P.Berg, C.Blasing, W.Naatz, A.Ruckelshausen, D.Ruck, R.K.M.Schneider, R.Stock Parity of Bound Dipole States in 208Pb NUCLEAR REACTIONS 208Pb(polarized γ, γ), E=10 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry. 208Pb deduced level, J, π, B(M1), Γ02/Γ. Linearly polarized beam.
doi: 10.1103/PhysRevLett.49.18
1981AC02 Nucl.Phys. A372, 1 (1981) K.Ackermann, K.Bangert, U.E.P.Berg, G.Junghans, R.K.M.Schneider, R.Stock, K.Wienhard Ground State Dipole Transitions in 58Ni NUCLEAR REACTIONS 58Ni, 208Pb(γ, γ), E < 10 MeV; measured σ(θ). 58Ni deduced levels, J, π, Γγ, E1, M1 transition strength. 208Pb levels deduced Γγ. Enriched targets, nuclear resonance fluorescence technique.
doi: 10.1016/0375-9474(81)90082-8
1981BE32 Phys.Lett. 103B, 301 (1981) U.E.P.Berg, D.Ruck, K.Ackermann, K.Bangert, C.Blasing, K.Kobras, W.Naatz, R.K.M.Schneider, R.Stock, K.Wienhard Parities of Dipole Ground-State Transitions in 52Cr NUCLEAR REACTIONS 52Cr(polarized γ, γ), E=7-9 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry. 52Cr deduced strong E1 transitions, B(M1) limit. Nuclear resonance fluorescence technique.
doi: 10.1016/0370-2693(81)90228-8
1981WI09 Phys.Rev. C24, 1363 (1981) K.Wienhard, R.K.M.Schneider, K.Ackermann, K.Bangert, U.E.P.Berg, R.Stock 16O(γ, p)15N Reaction with Linearly Polarized Photons NUCLEAR REACTIONS 16O(polarized γ, p), E=15-25 MeV bremsstrahlung; measured σ(Ep), analyzing power vs θ. 16O levels deduced π, proton decay amplitudes.
doi: 10.1103/PhysRevC.24.1363
1981WI12 Z.Phys. A302, 185 (1981) K.Wienhard, C.Blasing, K.Ackermann, K.Bangert, U.E.P.Berg, K.Kobras, W.Naatz, D.Ruck, R.K.M.Schneider, R.Stock Parities of Strong Dipole Ground State Transitions in 88Sr NUCLEAR REACTIONS 88Sr(polarized γ, γ), E=16 MeV bremsstrahlung; measured asymmetry. 88Sr levels deduced π. Nuclear resonance fluorescence technique, enriched targets.
doi: 10.1007/BF01413049
1979BE10 Nucl.Phys. A318, 453 (1979) Nuclear Resonance Fluorescence in 22Ne NUCLEAR REACTIONS 22Ne(γ, γ), E < 18 MeV; measured Eγ, σ(γ, γ). 22Ne deduced T1/2, Γγ0, B(M1) values. Enriched target.
doi: 10.1016/0375-9474(79)90659-6
1979JU02 Z.Phys. A291, 353 (1979) G.Junghans, K.Bangert, U.E.P.Berg, R.Stock, K.Wienhard The Photodisintegration of 6Li and 7Li NUCLEAR REACTIONS 6Li(γ, p), (γ, d), (γ, t), (γ, α), E(max)=30, 35 MeV; 7Li(γ, p), (γ, d), (γ, t), (γ, α), E(max)=28, 40, 50 MeV from bremsstrahlung; measured σ(θ). 7Li(γ, pd), (γ, αd), (γ, dt), (γ, d3He), (γ, pt), (γ, αp), E(max)=40 MeV; measured pd-, αd-, dt-, d3He-, pt-, αp-coin; deduced reaction mechanism.
doi: 10.1007/BF01408386
1978BE46 Nucl.Phys. A306, 178 (1978) U.E.P.Berg, K.Bangert, G.Junghans, R.Stock, K.Wienhard Lifetimes of Highly Excited States in 34S from Nuclear Resonance Fluorescence NUCLEAR REACTIONS 34S(γ, γ), E < 18 MeV; measured Eγ, σ(γ, γ). 34S deduced mean lives, Γγ0, B(M1) values. Enriched target.
doi: 10.1016/0375-9474(78)90321-4
1977CA21 Phys.Rev.Lett. 39, 925 (1977) J.R.Calarco, S.W.Wissink, M.Sasao, K.Wienhard, S.S.Hanna Structure in the Giant Dipole Resonance of 16O: Evidence for a Secondary Doorway State from Polarized-Proton Capture NUCLEAR REACTIONS 15N(polarized p, γ); measured σ. 16O deduced doorway state, parameters in GDR region.
doi: 10.1103/PhysRevLett.39.925
1977WI03 Nucl.Phys. A280, 109 (1977) K.Wienhard, K.Bangert, U.E.P.Berg, G.Junghans, R.Stock, H.Wolf Angular Distributions of Protons from the 26Mg(γ, p) Reaction between E(x) = 16 and 23 MeV NUCLEAR REACTIONS 26Mg(γ, p), E=16-23 MeV; measured σ(γ, p, θ). Enriched target.
doi: 10.1016/0375-9474(77)90297-4
1976BA14 Nucl.Phys. A261, 149 (1976) K.Bangert, U.E.P.Berg, G.Junghans, R.Stock, K.Wienhard, H.Wolf A Comparative Study of the Electric Giant Dipole Resonance of 24-26Mg NUCLEAR REACTIONS 24,25Mg(γ, p), (γ, α), 25Mg(γ, d), 24,25,26Mg(γ, γ'), E < 30 MeV; measured particle spectra, σ(E, Ep), σ(E, Eα), σ(E, Ed). 24,25,26Mg GDR deduced particle-hole, isospin configurations. Enriched targets.
doi: 10.1016/0375-9474(76)90047-6
1976BA41 Z.Phys. A278, 295 (1976) K.Bangert, U.E.P.Berg, K.Wienhard, H.Wolf The Decay of the 18O Giant Dipole Resonance to Excited Residual Nuclear States NUCLEAR REACTIONS 18O(γ, X), E=23.5, 28 MeV bremsstrahlung; measured prompt γ spectrum. 18O GDR deduced decay to levels in 17N, 17,16O, 14C.
doi: 10.1007/BF01409182
1975BE14 Phys.Rev. C11, 1851 (1975) U.E.P.Berg, K.Wienhard, H.Wolf Resonance Fluorescence of Giant Magnetic Dipole States in 24Mg NUCLEAR REACTIONS 24Mg(γ, γ), E < 23.5 MeV bremsstrahlung; measured Eγ, Iγ. 24Mg deduced levels, level-width, γ-branching.
doi: 10.1103/PhysRevC.11.1851
1974WI12 Z.Phys. 270, 93 (1974) K.Wienhard, K.Bangert, R.Stock, H.Wolf Photoproton Spectrum from Carbon with Good Energy Resolution NUCLEAR REACTIONS 12C(γ, p), E=31 MeV bremsstrahlung; measured σ(E, Ep). 12C giant resonances deduced fragmentation, level-width.
doi: 10.1007/BF01677439
1974WO03 Phys.Lett. 50B, 244 (1974) The Decay of the Giant Dipole Resonance in 26Mg to T = 3/2 States of 25Mg NUCLEAR REACTIONS 26Mg(γ, nγ'), E=0-30 MeV; measured Eγ', Iγ'. 26Mg GDR deduced T-splitting questionable.
doi: 10.1016/0370-2693(74)90549-8
1974WO08 Nucl.Phys. A234, 365 (1974) H.Wolf, R.Stock, U.E.P.Berg, K.Wienhard Charged Particles from the Giant Dipole Resonance of 26Mg NUCLEAR REACTIONS 26Mg(γ, p), (γ, α), E < 23.5 MeV; measured σ(E, Ep), σ(E, Eα); deduced total σ. 26Mg GDR deduced isospin effects.
doi: 10.1016/0375-9474(74)90569-7
1972WI26 Z.Phys. 256, 457 (1972) K.Wienhard, G.Clausnitzer, G.Hartmann Phase Shift Analysis of Elastic Proton Scattering by 12C NUCLEAR REACTIONS 12C(p, p), E=9.95-10.90 MeV; measured σ(E;θ), P(E;θ); deduced phase shifts. 13N deduced resonances, J, π, level-width.
doi: 10.1007/BF01386991
1969CL01 Phys.Rev.Letters 22, 793(1969) G.Clausnitzer, G.Graw, C.F.Moore, K.Wienhard An Anomaly in the Analyzing Power of 90Zr(d, p0)91Zr NUCLEAR REACTIONS 90Zr(vector-polarized d, p0), E=6-9 MeV; measured σ(E; θ=170°), vector analyzing power (E; θ).
doi: 10.1103/PhysRevLett.22.793
1969GR01 Phys.Letters 28B, 583 (1969) G.Graw, G.Clausnitzer, R.Fleischmann, K.Wienhard Spin Determination of Isobaric Analogue States in N = 85 and 87 Nuclei By Elastic Scattering of Polarized Protons NUCLEAR REACTIONS 142Ce, 144Nd, 146Nd(polarized p, p), E=9.745, 9.95, 10.16 MeV; measured analyzing power A(E;θ). 143Pr, 145,147Pm deduced resonances, J.
doi: 10.1016/0370-2693(69)90190-7
1969GR25 Phys.Letters 30B, 465 (1969) G.Graw, G.Clausnitzer, H.Clement, K.Wienhard, R.Fleischmann Inelastic Scattering of Polarized Protons Through Isobaric Analogue Resonances in 91Nb NUCLEAR REACTIONS 90Zr(polarized p, p'), E = 8.2-8.7 MeV; measured P(E;θ), σ(E;θ); deduced nonresonant scattering amplitude. 91Nb deduced isobaric analog resonance, level-width.
doi: 10.1016/0370-2693(69)90172-5
1969WI15 Z.Physik 228, 129 (1969) K.Wienhard, G.Clausnitzer, G.Graw, R.Fleischmann Untersuchung isobarer Analogresonanzen oberhalb der N = 50-Schale mit polarisierten Protonen NUCLEAR REACTIONS 88Sr, 90,92,94Zr(polarized p, p), E = 5-8.5 MeV; measured σ (E; θ). 89Y, 91,93,95Nb deduced resonances, J, π, level-width, isobaric analog.
doi: 10.1007/BF01397534
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