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NSR database version of April 27, 2024.

Search: Author = L.W.Put

Found 31 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1829.


1982PU01      Phys.Lett. 119B, 253 (1982)

L.W.Put, M.N.Harakeh

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1829.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1821.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1814.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1826.


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
Citations: PlumX Metrics


1979TA11      Phys.Lett. 84B, 371 (1979)

N.Takigawa, L.W.Put

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1830.


1977PU06      Nucl.Phys. A291, 93 (1977)

L.W.Put, A.M.J.Paans

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0249.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974PU01      Phys.Lett. 49B, 266 (1974)

L.W.Put, A.M.J.Paans

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0124.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0694.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20234.


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