NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Laegsgaard Found 7 matches. 1987FO05 Nucl.Phys. A464, 497 (1987) J.S.Forster, I.V.Mitchell, J.U.Anderson, A.S.Jensen, E.Laegsgaard, W.M.Gibson, K.Reichelt Angular Momentum Dependence of 200Pb Fission Studied by Comparison of 19F on 181Ta with 16O on 184W NUCLEAR REACTIONS 181Ta(19F, F), E=84.3-120 MeV; 184W(16O, F), E=83.4-107.9 MeV; measured σ(fragment θ) following fission. 200Pb deduced fission angular momentum dependence, long lived component. Blocking technique, natural Ta single crystal target, enriched 184WO3 target. Model comparisons.
doi: 10.1016/0375-9474(87)90312-5
1983JO04 Nucl.Phys. A396, 479c (1983) B.Jonson, J.U.Andersen, G.J.Beyer, G.Charpak, A.De Rujula, B.Elbek, H.A.Gustafsson, P.G.Hansen, P.Knudsen, E.Laegsgaard, J.Pedersen, H.L.Ravn Determination of the Electron-Neutrino Mass from Experiments on Electron-Capture Beta Decay RADIOACTIVITY 193Pt(EC); measured E(L X-ray), I(L X-ray), internal bremsstrahlung Eγ, Iγ, γ(X-ray)-coin; deduced Q(EC), electron neutrino mass upper limit. 163Ho(EC) [from Ta(p, X), E=600 MeV]; measured Auger electrons, E(X-ray), I(X-ray); deduced T1/2, electron neutrino mass upper limit. Reaction data input.
doi: 10.1016/0375-9474(83)90040-4
1982AN03 Nucl.Instrum.Methods 192, 79 (1982) J.U.Andersen, E.Laegsgaard, M.Lund Impact-Parameter Dependence of K-Shell Ionization ATOMIC PHYSICS Cu, Ag, Au(p, X), E=0.5-2.5 MeV; measured K-shell ionization probability; deduced impact parameter dependence. Semi-classical calculations, first Born approximation.
doi: 10.1016/0029-554X(82)90742-X
1982AN19 Phys.Lett. 113B, 72 (1982) J.U.Andersen, G.J.Beyer, G.Charpak, A.De Rujula, B.Elbek, H.A.Gustafsson, P.G.Hansen, B.Jonson, P.Knudsen, E.Laegsgaard, J.Pedersen, H.L.Ravn A Limit on the Mass of the Electron Neutrino: The case of 163Ho NUCLEAR REACTIONS 163Dy(d, t), 162Dy(3He, d), E not given; measured Q-value difference. 163Dy, 163Ho deduced mass difference. RADIOACTIVITY 163Ho(EC) [from Ta(p, X), E=600 MeV, mass separation]; measured partial decay T1/2; deduced T1/2, electron neutrino mass upper limit. Mass excess input from reaction data.
doi: 10.1016/0370-2693(82)90112-5
1980LA04 Nucl.Instrum.Methods 169, 293 (1980) E.Laegsgaard, J.U.Andersen, F.Hogedal Accurate Determination of Cross Sections for K-Shell Ionization by Proton Impact NUCLEAR REACTIONS Ti, Fe, Cu, Se, Zr, Ag(p, p), (p, p'), E=1-2 MeV; measured σ(Ep), X-ray production σ; deduced K-shell ionization σ.
1979AN12 Nucl.Phys. A324, 39 (1979) J.U.Andersen, N.G.Chechenin, A.S.Jensen, K.Jorgensen, E.Laegsgaard Decay Times for Second-Chance Fission of 239U Studied by Crystal Blocking NUCLEAR REACTIONS 238U(n, F), E=4.9, 5.5, 7.2, 7.5 MeV; measured blocking patterns. 239U, 238U deduced compound nuclear T1/2. Compared to theoretical calculation. Natural UO2 single-crystal target.
doi: 10.1016/0375-9474(79)90076-9
1976AN07 Phys.Rev.Lett. 36, 1539 (1976) J.U.Andersen, E.Laegsgaard, K.O.Nielsen, W.M.Gibson, J.S.Forster, I.V.Mitchell, D.Ward Time Evolution of Heavy-Ion-Induced Fission Studied by Crystal Blocking NUCLEAR REACTIONS W(16O, F), E=40, 90, 97 MeV; measured crystal-blocking angular distribution shapes.
doi: 10.1103/PhysRevLett.36.1539
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