NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = W.Wilke Found 25 matches. 1991WE03 Nucl.Phys. A522, 443 (1991) Th.Weber, U.Kneissl, W.Pecho, A.Degener, K.Huber, K.Schaschek, W.Wilke Fragment Angular Distributions in Electron- and Positron-Induced Fission of 232Th. A Specific Test of Virtual Photon Spectra NUCLEAR REACTIONS 232Th(e, F), E=8-16 MeV; measured fission fragment σ(θ); deduced angular correlation coefficients, fission channels. Virtual photon spectra tests.
doi: 10.1016/0375-9474(91)90075-H
1990WE07 Nucl.Phys. A510, 1 (1990) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, Th.Kihm, K.T.Knopfle, H.J.Emrich (e, e'f) Coincidence Experiments on 235U and 238U NUCLEAR REACTIONS 235,238U(e, e'F), E=78-183 MeV; measured σ(θ(e'), E, θ(fragment)), in-, out-of-plane fission fragment σ(θ), fragment time-of-flight differences. 235,238U deduced multipole strength distributions for giant E0, E1, E2, E3 resonances, fission characteristics.
doi: 10.1016/0375-9474(90)90286-U
1990WI15 Phys.Rev. C42, 2148 (1990) W.Wilke, U.Kneissl, Th.Weber, H.Stroher, L.S.Cardman, P.T.Debevec, S.D.Hoblit, R.T.Jones, A.M.Nathan Photofission of 238U with Monochromatic Gamma Rays in the Energy Range 11-16 MeV NUCLEAR REACTIONS 238U(γ, F), E=11-16 MeV; measured fission fragment σ(θ), fragment mass distributions; deduced anisotropy, fragment mass asymmetry relationship.
doi: 10.1103/PhysRevC.42.2148
1989WE01 Phys.Rev.Lett. 62, 129 (1989) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Evidence for Different Mass Splits in Fission Decays of Giant Multipole Resonances from 235,238U(e, e'f) Reactions NUCLEAR REACTIONS 235,238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)-coin. 235,238U deduced giant multipole resonance fission decay features, Γ(S)/Γ(A).
doi: 10.1103/PhysRevLett.62.129
1989WE12 Nucl.Phys. A502, 279c (1989) Th.Weber, W.Wilke, H.J.Emrich, R.D.Heil, Th.Kihm, U.Kneissl, K.T.Knopfle, U.Seemann, F.Steiper, H.Stroher Evidence for Different Fission Fragment Mass Asymmetries for Specific Nuclear Excitations Studied in (e, e'F) and (γ, F) Reactions NUCLEAR REACTIONS 236U(e, e'F), E not given; measured fission fragment σ(θ). 235,238U(e, e'F), E=185 MeV; measured fission fragment spectra; deduced symmetric, asymmetric fission yield ratios, excitation multipolarity role.
doi: 10.1016/0375-9474(89)90668-4
1988WE18 Phys.Lett. 215B, 469 (1988) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Near Barrier Fission Channels (J(π), K) in 238U for Spins J(π) = 0+, 1-, and 2+ from (e, e'f) Angular Correlation Measurements NUCLEAR REACTIONS 238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)(θ), in-plane, out-of-plane; deduced partial fission channel σ. 238U levels deduced fission barriers.
doi: 10.1016/0370-2693(88)91343-3
1988WI15 Phys.Lett. 207B, 385 (1988) W.Wilke, R.D.Heil, U.Kneissl, U.Seemann, F.Steiper, H.Stroher, T.Weber Angular Distributions of Photofission Fragments of Particular Mass NUCLEAR REACTIONS 236U(γ, F), E=16 MeV bremsstrahlung; measured fission fragment σ(θ), mass distribution. 236U deduced fission mechanism.
doi: 10.1016/0370-2693(88)90669-7
1988WI20 Nucl.Instrum.Methods Phys.Res. A272, 785 (1988) W.Wilke, H.Bruckel, R.D.Heil, U.Kneissl, H.Stroher, Th.Weber A 4π Double Obelisk of Position Sensitive PPACs for New Vistas in Photofission Experiments NUCLEAR REACTIONS 238U(γ, F), E=5.6-16 MeV bremsstrahlung; measured fission fragment spectra, σ(θ), mass distribution. Position sensitive detectors, 4π array.
doi: 10.1016/0168-9002(88)90760-7
1987LE19 Nucl.Phys. A472, 533 (1987) A.Lepretre, R.Bergere, P.Bourgeois, P.Carlos, J.Fagot, J.L.Fallou, P.Garganne, A.Veyssiere, H.Ries, R.Goble, U.Kneissl, G.Mank, H.Stroher, W.Wilke, D.Ryckbosch, J.Jury Absolute Photofission Cross Sections for 232Th and 235,238U Measured with Monochromatic Tagged Photons (20 MeV < E(γ) < 110 MeV) NUCLEAR REACTIONS 232Th, 235,238U(γ, F), E=20-110 MeV; measured fission σ(E). 232Th, 235,238U deduced fission evaporation competition, fission probabilities. Hybrid model. Parallel plate avalanche detector, monochromatic tagged photons.
doi: 10.1016/0375-9474(87)90044-3
1987WE09 Phys.Rev.Lett. 59, 2028 (1987) Th.Weber, R.D.Heil, U.Kneissl, W.Pecho, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Multipole Strength Distributions and Form Factors for E1, E2/E0, and E3 from 238U(e, e'f) Coincidence Experiments NUCLEAR REACTIONS 238U(e, e'F), E=78, 183, 124 MeV; measured fission (fragment)(fragment)-coin. 238U deduced multipole strength distributions, form factors.
doi: 10.1103/PhysRevLett.59.2028
1985DR01 Nucl.Phys. A437, 253 (1985) J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, B.Fischer, H.Hollick The ' Isomeric Shelf ' in the Deep Subbarrier Photofission of 238U NUCLEAR REACTIONS 238U(γ, F), E=3.9-4.3 MeV bremsstrahlung; measured T1/2, isomeric to prompt yield ratio. Depleted targets.
doi: 10.1016/0375-9474(85)90087-9
1985HE21 Nucl.Instrum.Methods 239, 545 (1985) R.D.Heil, J.Drexler, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, T.Weber, W.Wilke A Compact Time-of-Flight Spectrometer for Electrofission Studies RADIOACTIVITY 252Cf(SF); measured fission fragment velocities, masses, energies before neutron emission.
doi: 10.1016/0168-9002(85)90034-8
1984DR04 Nucl.Instrum.Methods 220, 409 (1984) J.Drexler, R.D.Fischer, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke Arrangements of Parallel Plate Avalanche Detectors for Electrofission and Photofission experiments NUCLEAR REACTIONS 232Th(e+, F), (e-, F), E=9 MeV; measured fission fragment σ(θ). Parallel plate avalanche detectors. RADIOACTIVITY 252Cf(SF); measured fission fragment tof spectra. Parallel plate avalanche detectors.
doi: 10.1016/0167-5087(84)90303-X
1984RI08 Phys.Rev. C29, 2346 (1984) H.Ries, G.Mank, J.Drexler, R.Heil, K.Huber, U.Kneissl, R.Ratzek, H.Stroher, T.Weber, W.Wilke Absolute Photofission Cross Sections for 235,238U in the Energy Range 11.5-30 MeV NUCLEAR REACTIONS 238,235U(γ, F), E=11.5-30 MeV; measured absolute fission σ(E). Quasimonoenergetic photons from positron annihilation, multiple parallel plate detectors.
doi: 10.1103/PhysRevC.29.2346
1984RI09 Phys.Lett. 139B, 254 (1984) H.Ries, U.Kneissl, G.Mank, H.Stroher, W.Wilke, R.Bergere, P.Bourgeois, P.Carlos, J.L.Fallou, P.Garganne, A.Veyssiere, L.S.Cardman Absolute Photofission Cross Sections of 235,238U Measured with Tagged Photons between 40 and 105 MeV NUCLEAR REACTIONS 235,238U(γ, F), E=40-105 MeV; measured absolute fission σ(E). 235,238U deduced total fission probability vs E. Tagged photon beam. Evaporation cascade model.
doi: 10.1016/0370-2693(84)91074-8
1984ST07 Nucl.Phys. A419, 295 (1984) H.Stroher, J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, H.J.Maier Fission Barriers of Preactinide Nuclei from Electrofission Experiments NUCLEAR REACTIONS 182,184,186W, Pt, 209Bi(e, F), E=25-55 MeV; measured electron induced fission σ(E); deduced fission barriers B. Natural, enriched targets. Statistical model analysis.
doi: 10.1016/0375-9474(84)90394-4
1984WE05 Z.Phys. A315, 125 (1984) T.Weber, J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, W.Wilke A New Method to Test Virtual Photon Spectra NUCLEAR REACTIONS 232Th(e-, F), E=9 MeV; 232Th(e+, F), E=16 MeV; measured fission fragment σ(θ), anisotropy.
doi: 10.1007/BF01436220
1983DR14 Nucl.Phys. A411, 17 (1983) J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke The Decay of Uranium Shape Isomers Investigated by Photonuclear Reactions NUCLEAR REACTIONS 238U(γ, γ'), E=12 MeV bremsstrahlung; measured isomer T1/2, isomeric to prompt yield ratio; deduced isomeric fission cross section. 238U deduced isomer decay branching ratio. Natural target.
doi: 10.1016/0375-9474(83)90505-5
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
1982ST05 Nucl.Phys. A378, 237 (1982) H.Stroher, R.D.Fischer, J.Drexler, K.Huber, U.Kneissl, R.Ratzek, H.Ries, W.Wilke, H.J.Maier Absolute Cross Sections for Electron- and Positron-Induced Fission of 238U and Tests of DWBA Virtual-Photon Spectra NUCLEAR REACTIONS 238U(e, F), (e+, F), E=10-35 MeV; measured absolute σ. Natural targets.
doi: 10.1016/0375-9474(82)90590-5
1981GU04 Nucl.Phys. A359, 397 (1981) W.Gunther, K.Huber, U.Kneissl, H.Krieger, H.Ries, H.Stroher, W.Wilke Yield Ratio for the Two 241Pu Fission Isomers in the 242Pu(γ, n) Reaction NUCLEAR REACTIONS 242Pu(γ, n), E=40-48 MeV bremsstrahlung; measured T1/2, isomeric to prompt yield ratio. 241Pu levels deduced isomeric ratio, J. Enriched target.
doi: 10.1016/0375-9474(81)90245-1
1981ST12 Phys.Rev.Lett. 47, 318 (1981) H.Stroher, R.D.Fischer, J.Drexler, K.Huber, U.Kneissl, R.Ratzek, H.Ries, W.Wilke, H.J.Maier Investigation of the Fission Decay of the Isoscalar Giant Quadrupole Resonance in 238U by Electron- and Positron-Induced Fission NUCLEAR REACTIONS, Fission 238U(e, F), (e+, F), E=10-35 MeV; measured σ(E), σ(ratio). 238U deduced no GQR fission decay. DWBA, virtual photon treatment.
doi: 10.1103/PhysRevLett.47.318
1980GU20 Nucl.Phys. A350, 1 (1980) W.Gunther, K.Huber, U.Kneissl, H.Krieger, H.Ries, H.Stroher, W.Wilke, H.J.Maier Systematics of Photonuclear Yields and Cross Sections for Plutonium and Uranium Fission Isomers NUCLEAR REACTIONS, Fission 240Pu, 235U(γ, xn), 239Pu(γ, 2n), 242Pu(γ, n), E=45 MeV bremsstrahlung; measured T1/2, isomeric to prompt yield ratios. 236U, 237,239,241Pu levels deduced σ(fission). Natural, enriched targets.
doi: 10.1016/0375-9474(80)90385-1
1978WI07 Phys.Rev. C18, 1452 (1978) W.W.Wilke, M.W.Johnson, W.U.Schroder, J.R.Huizenga, D.G.Perry Neutron Emission from Actinide Muonic Atoms NUCLEAR REACTIONS 232Th, 235,238U, 237Np, 239,242Pu(μ-, F), E=0 MeV; measured n(t); deduced total muon capture rates, isotope effect, Γn/Γf.
doi: 10.1103/PhysRevC.18.1452
1961WI13 Z.Physik 165, 562 (1961) NUCLEAR STRUCTURE 85Rb, 87Rb, 133Cs; measured not abstracted; deduced nuclear properties.
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