NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.W.Put Found 31 matches. 1984VA31 Nucl.Phys. A429, 1 (1984); Erratum Nucl.Phys. A441, 757 (1985) A.M.Van Den Berg, A.Saha, G.D.Jones, L.W.Put, R.H.Siemssen Study of Even-A Zirconium and Strontium Isotopes with the (d, 6Li) Reaction NUCLEAR REACTIONS 90,92Zr, 92,94,96,98,100Mo(d, 6Li), E=45 MeV; measured σ(E(6Li), θ). 86,88Sr, 88,90,92,94,96Zr levels deduced S(α), J, π. DWBA analysis, shell model wave functions. Enriched targets, magnetic spectograph.
doi: 10.1016/0375-9474(84)90147-7
1982DE29 Nucl.Phys. A386, 200 (1982) R.J.De Meijer, L.W.Put, J.Akkermans, J.C.Vermeulen, C.R.Bingham Microscopic and Macroscopic DWBA Analysis of the Reactions 28Si(α, d)30P, 32S(d, α)30P and 32S(α, d)34Cl Studied at E(α) = 50 MeV and E(d) = 40 MeV NUCLEAR REACTIONS 32S, 28Si(α, d), E=50 MeV; 32S(d, α), E=40 MeV; measured σ(θ). 30P, 34Cl deduced levels, L, S, J, π. Natural targets. Microscopic, macroscopic DWBA calculations.
doi: 10.1016/0375-9474(82)90111-7
1982PU01 Phys.Lett. 119B, 253 (1982) Hadronic Excitation of the Octupole Bands in Deformed Nuclei: Necessity of the isoscalar dipole degree of freedom ( Question ) NUCLEAR REACTIONS 150Nd, 152Sm(p, p), (p, p'), E=50 MeV; measured σ(θ); deduced isoscalar dipole degree of freedom insignificance. 152Sm deduced octupole band excitation characteristics, deformation parameter. QMG/2 magnetic spectrograph. Coupled-channels analysis.
doi: 10.1016/0370-2693(82)90664-5
1982RI08 Phys.Lett. 118B, 287 (1982) H.J.Riezebos, R.De Leo, P.B.Goldhoorn, M.N.Harakeh, L.W.Put, H.Sakai, R.H.Siemssen Multipole Strength Distribution in 156Gd from the (p, t) Reaction at E(p) = 40 MeV NUCLEAR REACTIONS 158Gd(p, t), E=40 MeV; measured σ(Et), σ(θ); deduced optical model parameters. 156Gd levels deduced integrated spectroscopic factors, multipole strength distribution. DWBA analysis, dineutron cluster form factor.
doi: 10.1016/0370-2693(82)90186-1
1981DE37 Phys.Lett. 107B, 14 (1981) R.J.de Meijer, L.W.Put, J.C.Vermeulen Two-Nucleon Cluster Spectroscopic Factors: A search for the bound-state parameters NUCLEAR REACTIONS 28Si, 32S(α, d), E=50 MeV; 32S(d, α), E=40 MeV; analyzed σ(θ). 30P, 34Cl levels deduced two-nucleon transfer S. DWBA, macroscopic form factor.
doi: 10.1016/0370-2693(81)91136-9
1981GO13 Phys.Lett. 103B, 291 (1981) P.B.Goldhoorn, M.N.Harakeh, Y.Iwasaki, L.W.Put, F.Zwarts, P.van Isacker Hexadecapole Transition Moments in Strongly Deformed Nuclei and the Validity of the sd-Boson Approximation in the IBA NUCLEAR REACTIONS 156Gd(p, p'), E=40 MeV; measured σ(θ, Ep). 156Gd deduced levels, hexadecapole transition strength. QMG/2 magnetic spectrograph. DWBA, coupled-channels analyses, interacting boson approximation model.
doi: 10.1016/0370-2693(81)90226-4
1981VE05 Nucl.Phys. A362, 189 (1981) J.C.Vermeulen, A.G.Drentje, H.T.Fortune, L.W.Put, R.R.De Ruyter Van Steveninck, R.H.Siemssen, J.F.A.Van Hienen, H.Hasper High-Resolution Study of Four-Nucleon Pickup Via the (d, 6Li) Reaction at Ed = 55 MeV on sd Shell Nuclei (I) . Even-A Nuclei NUCLEAR REACTIONS 24,26Mg, 28Si(d, 6Li), E=55 MeV; measured σ(E(6Li), θ). 20,22Ne, 24Mg deduced levels, Sα, L, J, π. Magnetic spectrograph, enriched targets.
doi: 10.1016/0375-9474(81)90677-1
1981VE13 Nucl.Phys. A369, 82 (1981) J.C.Vermeulen, A.G.Drentje, L.W.Put, R.R.De Ruyter Van Steveninck, J.F.A.Van Hienen, H.Hasper, H.T.Fortune High-Resolution Study of Four-Nucleon Pickup via the (d, 6Li) Reaction at E(d) = 55 MeV on sd-Shell Nuclei (II). Odd-A Nuclei NUCLEAR REACTIONS 25Mg, 27Al(d, 6Li), E=55 MeV; measured σ(E(6Li), θ). 21Ne, 23Na deduced levels, Sα, L, J, π. Magnetic spectrograph, enriched 25Mg target.
doi: 10.1016/0375-9474(81)90008-7
1980HA47 Phys.Lett. B97, 21 (1980) M.N.Harakeh, P.Goldhoorn, Y.Iwasaki, J.Lukasiak, L.W.Put, S.Y.van der Werf, F.Zwarts The Supersymmetry Scheme and E2 Transition Rates in the Pt Region NUCLEAR REACTIONS 191,193Ir, 194Pt(p, p), (p, p'), E=50 MeV; measured σ(Ep, θ). 191,193Ir, 194Pt levels deduced B(E2), supersymmetry model validation. QMG/2 Spectrograph. DWBA analysis.
doi: 10.1016/0370-2693(80)90537-7
1980SC23 Nucl.Phys. A348, 301 (1980) O.Scholten, M.N.Harakeh, J.Van Der Plicht, L.W.Put, R.H.Siemssen, S.Y.Van Der Werf, M.Sekiguchi Neutron Pickup Reactions on the Even Palladium Isotopes and the Deeply Bound Hole-State Excitation NUCLEAR REACTIONS 102,104,106,108,110Pd(d, t), E=50 MeV; measured σ(Et, θ). 101,103Pd levels deduced L, J, π, C2S. 102,104,106,108,110Pd; deduced deeply bound hole states, spectroscopic strength distributions. DWBA analysis. 102,104,106,108,110Pd(3He, α), E=70 MeV; measured σ(Eα); deduced deeply bound hole states.
doi: 10.1016/0375-9474(80)90339-5
1979HA03 Nucl.Phys. A313, 95 (1979) O.Hansen, M.N.Harakeh, J.V.Maher, L.W.Put, J.C.Vermeulen Proton Hole States in 63Co and 63Cu NUCLEAR REACTIONS 64Ni, 64Zn(d, 3He), E=55.0 MeV; measured σ(E(3He), θ). 63Co, 63Cu levels deduced L, S. Enriched targets, DWBA analysis.
doi: 10.1016/0375-9474(79)90569-4
1979SA12 Phys.Lett. 82B, 208 (1979) A.Saha, G.D.Jones, L.W.Put, R.H.Siemssen Unusually Strong Excitation of the 1.59 MeV 0+ State in the 100Mo(d, 6Li)96Zr Reaction NUCLEAR REACTIONS 94,96,98,100Mo(d, 6Li), E=45 MeV; measured σ(E(6Li)), σ(θ). 90,92,94,96Zr deduced change in proton configuration with neutron number. DWBA analysis. Enriched targets.
doi: 10.1016/0370-2693(79)90737-8
1979TA11 Phys.Lett. 84B, 371 (1979) Critical Energies in Elastic α-Nucleus Scattering NUCLEAR REACTIONS 90Zr(α, α), E=40, 99.5, 220 MeV; calculated σ(θ), classical deflection functions, energy surfaces for certain L-values; deduced critical energies. Semiclassical theory.
doi: 10.1016/0370-2693(79)91218-8
1979VE04 Nucl.Phys. A329, 93 (1979) J.C.Vermeulen, C.R.Bingham, D.Dijkhuizen, R.J.De Meijer, L.W.Put Investigation of the Decay Properties of High-Spin Two-Nucleon States Via the 28Si(α, dγ)30P Reaction at E = 50 MeV NUCLEAR REACTIONS 28Si(α, dγ), E=50 MeV; measured dγ(θ). 30P deduced levels, J, π. ΔE-E surface barrier telescope, Ge(Li) detectors, natural target. PWBA, DWBA analysis.
doi: 10.1016/0375-9474(79)90283-5
1978FO32 Phys.Lett. 79B, 205 (1978) H.T.Fortune, J.C.Vermeulen, A.Saha, A.G.Drentje, L.W.Put, R.R.de Ruyter van Steveninck, J.F.A.van Hienen Configuration of 3.59 MeV 0+ State in 44Ca NUCLEAR REACTIONS 48Ti(d, 6Li), E=55 MeV; measured σ(E(6Li), θ). 44Ca deduced relative α-pickup S for 0+ states.
doi: 10.1016/0370-2693(78)90223-X
1978LO04 Z.Phys. A286, 99 (1978) H.Lohner, H.Eickhoff, D.Frekers, G.Gaul, K.Poppensieker, R.Santo, A.G.Drentje, L.W.Put Investigation of Large Angle Structure in α-Scattering from Calcium Isotopes between E = 36-61 MeV NUCLEAR REACTIONS 40Ca(α, α), E=36.2, 39.6, 42.6, 49.5, 61.0 MeV; 44Ca(α, α), E=36.2, 42.6, 49.5, 61.0 MeV; measured σ(θ). Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0639. 1977HA47 Nucl.Phys. A292, 253 (1977) O.Hansen, J.V.Maher, J.C.Vermeulen, L.W.Put, R.H.Siemssen, A.van der Woude Four-Nucleon Pickup from 64Zn and 64Ni NUCLEAR REACTIONS 64Zn, 64Ni(d, 6Li), E=55.0 MeV; measured σ(E(Li), θ). 60Ni, 60Fe deduced levels, α-spectroscopic strengths, L, J, π. Enriched targets.
doi: 10.1016/0375-9474(77)90372-4
1977PU06 Nucl.Phys. A291, 93 (1977) The Form Factor of the Real Part of the α-Nucleus Potential Studied over a Wide Energy Range NUCLEAR REACTIONS 90Zr(α, α), E=40, 59.1, 79.5, 118 MeV; 92Zr(α, α), E=40, 90, 120 MeV; measured σ(θ). 90Zr(α, α), E=28-54 MeV; measured σ(E, θ), θ=77.9°, 141.3°, 176.2°; deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(77)90201-9
1977VA15 Nucl.Phys. A289, 141 (1977) S.Y.van der Werf, M.N.Harakeh, L.W.Put, O.Scholten, R.H.Siemssen The 116Sn(d, t)115Sn Reaction and the Investigation of Deeply Bound Hole States in the Odd-A Tin Isotopes NUCLEAR REACTIONS 116Sn(d, t), E=50 MeV; measured σ(Et, θ). 115Sn levels deduced L, J, π, C2S. 112,114,116,118,120,122,124Sn(d, t), E=50 MeV; measured spectra. 111,113,115,117,119,121,123Sn deduced deeply bound hole states, binding energies, widths. DWBA analysis.
doi: 10.1016/0375-9474(77)90526-7
1976VA25 Nucl.Phys. A273, 15 (1976) S.Y.Van der Werf, B.Fryszczyn, L.W.Put, R.H.Siemssen Investigation of Proton Hole States in 109,111Ag Excited in the 110,112Cd(d, 3He) Reaction NUCLEAR REACTIONS 110,112Cd(d, 3He), E=50 MeV; measured σ(E(3He), θ). 109,111Ag deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(76)90297-9
1974HE11 Nucl.Phys. A226, 229 (1974) W.H.A.Hesselink, B.R.Kooistra, L.W.Put, R.H.Siemssen, S.Y.van der Werf Proton-Hole States in 115In Observed in the 116Sn(d, 3He) Reaction NUCLEAR REACTIONS 116Sn(d, 3He), E=50 MeV; measured σ(E(3He), θ). 115In deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(74)90404-7
1974PU01 Phys.Lett. 49B, 266 (1974) Evidence for an Energy Dependent Form Factor of the α-Particle Optical Potential NUCLEAR REACTIONS 90Zr(α, α), E=40, 59.1, 79.5, 99.5, 118 MeV; measured σ(θ), deduced optical model parameters.
doi: 10.1016/0370-2693(74)90430-4
1974VA15 Phys.Rev. C10, 952 (1974) A.van der Woude, W.J.Ockels, P.J.Pasma, L.W.Put Isospin Mixing in 12C Studied with the 14N(d, α)12C Reaction at E = 40 MeV NUCLEAR REACTIONS 14N(d, α), E=40 MeV; measured σ(Eα, θ). 12C deduced upper limit for isospin mixing.
doi: 10.1103/PhysRevC.10.952
1974VA17 Phys.Rev.Lett. 33, 712 (1974) S.Y.van der Werf, B.R.Kooistra, W.H.A.Hesselink, F.Iachello, L.W.Put, R.H.Siemssen Deeply Bound Hole States as a Giant-Resonance-Like Phenomenon NUCLEAR REACTIONS 112,116,118,120,122,124Sn(d, t), E=50 MeV; measured σ(Et, θ). 115Sn resonances deduced L. 111,115,117,119,121,123Sn deduced resonance structure.
doi: 10.1103/PhysRevLett.33.712
1972UR01 Nucl.Phys. A186, 344 (1972) P.P.Urone, L.W.Put, B.W.Ridley Global Optical-Model Analysis of 37.7 MeV 3He Elastic Scattering from Medium-A Nuclei (46 < A < 91) NUCLEAR REACTIONS 46,50Ti, 51V, 62Ni, 91Zr(3He, 3He), E=37.7 MeV; measured σ(θ). Enriched targets. Global optical-model analysis.
doi: 10.1016/0375-9474(72)90051-6
1971PU02 Phys.Lett. 35B, 311 (1971) L.W.Put, P.P.Urone, A.M.J.Paans Scattering of 30 MeV Protons from 28Si, 58Ni and 120Sn at Large Backward Angles NUCLEAR REACTIONS 28Si, 58Ni, 120Sn(p, p), E=30 MeV; measured σ(θ) to 178°; deduced optical model parameters.
doi: 10.1016/0370-2693(71)90266-8
1971UR01 Nucl.Phys. A163, 225 (1971) P.P.Urone, L.W.Put, H.H.Chang, B.W.Ridley Isospin Dependence of the Mass-3 Optical Potential from the Comparison Of Triton and 3He Elastic Scattering NUCLEAR REACTIONS 40Ca, 52Cr, 54Fe, 62Ni, 64Ni, 90Zr, 92Zr, 94Zr, 118Sn(3He, 3He), E=21 MeV; measured σ(θ); deduced optical model parameters. Enriched targets except Ca, Cr.
doi: 10.1016/0375-9474(71)90531-8
1971UR02 Nucl.Phys. A167, 383 (1971) P.P.Urone, L.W.Put, B.W.Ridley, G.D.Jones Optical-Model Analysis of 38 MeV 3He Elastic Scattering Extended into the Backward Hemisphere NUCLEAR REACTIONS 48Ti, 58Fe, 90Zr(3He, 3He), E=37.7 MeV; 58Ni(3He, 3He), E=36.8, 37.4, 37.5, 38.1 MeV; measured σ(θ). Enriched targets.
doi: 10.1016/0375-9474(71)90084-4
1969RO34 Nuovo Cimento Lett. 2, 209 (1969) J.D.A.Roeders, L.W.Put, A.G.Drentje, A.van der Woude Energy-Dependent Coherence Width of 28Si at Excitation Energies between 22 and 33 MeV NUCLEAR REACTIONS 24Mg(α, α), (α, α'), E=18-27 MeV; measured σ(E;θ). 28Si deduced coherence width.
doi: 10.1007/BF02755748
1968PU02 Nucl.Phys. A112, 561(1968) L.W.Put, J.D.A.Roeders, A.van der Woude Analysis of Fluctuations in the 27Al(p, α)24Mg Excitation Functions from 10.9 to 19.7 MeV NUCLEAR REACTIONS 27Al(p, α), E=10.9-19.7 MeV; measured σ(Ep; Eα, θ). 28Si levels deduced coherence width level-width. Fluctuation analysis.
doi: 10.1016/0375-9474(68)90078-X
1966PU03 Physica 32, 1397 (1966) L.W.Put, C.Bot, W.J.Coenders, J.W.Koen, J.Blok An Associated Particle Method for the D(d, n)3He Reaction NUCLEAR STRUCTURE 54Fe, 56Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(66)90131-5
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