NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.T.Pinkston Found 30 matches. 1986KA16 Phys.Lett. 172B, 292 (1986) M.W.Katoot, V.E.Oberacker, W.T.Pinkston Microscopic Theory of Heavy-Ion Potentials NUCLEAR STRUCTURE 16O, 28Si, 40Ca, 64Ni, 74Ge, 116Ba, 236U; calculated binding energy. Many-body theory, effective Skyrme nucleon interaction. NUCLEAR REACTIONS 28Si(28Si, 28Si), 40Ca(40Ca, 40Ca), 90Zr(90Zr, 90Zr), E not given; calculated heavy-ion potential parameters vs separation distance. Many-body theory, effective Skyrme nucleon-nucleon interaction.
doi: 10.1016/0370-2693(86)90254-6
1985RU06 Phys.Lett. 158B, 201 (1985) D.P.Russell, W.T.Pinkston, V.E.Oberacker Pockets in Heavy-Ion Potentials and Nucleon Transfer NUCLEAR REACTIONS 238U(238U, 238U), (238U, X), E=673 MeV; calculated elastic, single nucleon transfer σ(θ). Schematic model, potential pockets.
doi: 10.1016/0370-2693(85)90954-2
1985SE01 J.Phys.(London) G11, L21 (1985) M.Seiwert, W.Greiner, W.T.Pinkston Do Heavy-ion Potentials have Pockets ( Question ) NUCLEAR REACTIONS 208Pb(208Pb, X), (238U, X), 238U(238U, X), E not given; calculated interaction potentials.
doi: 10.1088/0305-4616/11/1/008
1984PI02 Phys.Rev. C29, 1123 (1984) Clustering of Nucleons in the Nuclear Surface NUCLEAR STRUCTURE 210Pb, 210Po; analyzed α-cluster, α-decay pair correlation dependence. Schematic, shell model comparisons.
doi: 10.1103/PhysRevC.29.1123
1984PI14 Phys.Rev. C30, 1431 (1984) Transfer Reaction Sum Rules and the Interacting Boson-Fermion Model NUCLEAR STRUCTURE 194,196,198Pt; calculated pickup, stripping sum rule spectroscopic factors. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.30.1431
1984SA04 Phys.Lett. 134B, 7 (1984) Comment on J-Dependence in (α, d) Transfer Reactions NUCLEAR REACTIONS 208Pb(α, d), E not given; calculated σ(θ); deduced simultaneous, sequential transfer interference J-dependence. Second-order DWBA amplitudes.
doi: 10.1016/0370-2693(84)90972-9
1983SA33 Nucl.Phys. A411, 144 (1983) Properties of the Transition Amplitude for Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 208Pb(α, d), E not given; calculated σ(θ). 210Bi levels deduced population J-dependence. Two-nucleon transfer, additional angular momemntum transfer sources.
doi: 10.1016/0375-9474(83)90512-2
1980FE01 Phys.Rev.Lett. 44, 1037 (1980) D.H.Feng, M.A.Nagarajan, M.R.Strayer, M.Vallieres, W.T.Pinkston Exact Finite-Range Distorted-Wave Born-Approximation Analyses of the Reactions 18O(p, t)16O, 48Ca(t, p)50Ca, and 90Zr(t, p)93Zr Using Realistic Triton and Nuclear Wave Functions NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 48Ca(t, p), E=12.08 MeV; 90Zr(t, p), E=11.89 MeV; calculated σ(θ). Finite-range DWBA, realistic t-, structure overlap-functions.
doi: 10.1103/PhysRevLett.44.1037
1980KR19 Phys.Rev. C22, 2465 (1980) H.Kruse, W.T.Pinkston, W.Greiner, V.Oberacker Dynamics of Coulomb Fission NUCLEAR REACTIONS, Fission 238U(132Xe, pF), (165Ho, pF), (206Pb, pF), (238U, pF), 238U(132Xe, nF), (165Ho, nF), (206Pb, nF), (238U, nF), E<Coulomb barrier; calculated σ(Ep, θ), Γn/Γγ, damping effects, double-humped barrier penetration. Prompt, asymptotic semiquantal Coulomb fission theory.
doi: 10.1103/PhysRevC.22.2465
1979OB01 Phys.Rev. C20, 1453 (1979) V.Oberacker, W.Greiner, H.Kruse, W.T.Pinkston Characteristics of Coulomb Fission NUCLEAR REACTIONS 136Xe, 165Ho, 208Pb, 238U(238U, F), E < Coulomb barrier; calculated fission σ(θ, E), fragment σ(θ). Semiquantal, coupled-channel theory.
doi: 10.1103/PhysRevC.20.1453
1979PI10 Nucl.Phys. A330, 91 (1979) Center-of-Mass Corrections to Overlap Factors for Transfer Reactions (III) NUCLEAR REACTIONS 16O, 40Ca(t, p), E=10, 20 MeV; 90Zr, 208Pb(t, p), E=20 MeV; calculated σ(θ). DWBA, center-of-mass correction to overlap factors.
doi: 10.1016/0375-9474(79)90539-6
1979VA07 Phys.Lett. 83B, 267 (1979) M.Vallieres, D.H.Feng, W.T.Pinkston Angular Momentum and Binding Energy Effects in Two-Nucleon Transfer NUCLEAR STRUCTURE 42Ca, 42Sc, 42Ti; calculated two-nucleon transfer overlaps. 18O, 18F, 18Ne; calculated zero-range form factors for ground states. Extended basis shell model, well-depth model.
doi: 10.1016/0370-2693(79)91104-3
1978PI10 Phys.Rev. C18, 1011 (1978) W.T.Pinkston, M.Vallieres, D.H.Feng Two-Nucleon Transfer: Random-Phase Approximation Theory, Pairing Vibrations, and the Extended Basis Shell Model NUCLEAR REACTIONS 16O(p, t), E=40 MeV; 16O(t, p), E=10 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.18.1011
1977PI10 Nucl.Phys. A291, 342 (1977) Center-of-Mass Corrections to Overlap Factors for Two-Nucleon Transfer NUCLEAR REACTIONS 16O(t, p), E=10 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90324-4
1975IA01 Nucl.Phys. A237, 189 (1975) Aspects of Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 40Ca(t, p), E=10.1 MeV; calculated σ(Ep, θ); deduced form factors.
doi: 10.1016/0375-9474(75)90418-2
1975RA40 Phys.Rev. C 12, 1360 (1975) A.V.Ramayya, R.M.Ronningen, J.H.Hamilton, W.T.Pinkston, G.Garcia-Bermudez, R.L.Robinson, H.J.Kim, H.K.Carter, W.E.Collins Mean life and collective effects of the 937 keV, 0+ state in 72Se: Evidence for nuclear coexistence RADIOACTIVITY 72Br(EC), (β+) [from 58Ni(16O, np), E=46 MeV]; measured Eγ, Iγ, γγ-coin, isomer T1/2 by γ(t) at the ORNL tandem Van de Graaff accelerator. 72Se; deduced levels, J, π, B(E2), E0/E2, monopole transition strength ρ(E0), shape coexistence.
doi: 10.1103/PhysRevC.12.1360
1974HA04 Phys.Rev.Lett. 32, 239 (1974) J.H.Hamilton, A.V.Ramayya, W.T.Pinkston, R.M.Ronningen, G.Garcia-Bermudez, H.K.Carter, R.L.Robinson, H.J.Kim, R.O.Sayer Evidence for Coexistence of Spherical and Deformed Shapes in 72Se RADIOACTIVITY 72Br; measured γγ(t). 72Se level deduced T1/2. NUCLEAR REACTIONS 58Ni(16O, 2pγ), E not given; measured Eγ, Iγ, γ(θ), γγ-coin. 72Se deduced levels, J, π.
doi: 10.1103/PhysRevLett.32.239
1973SO11 Part.Nucl. 6, 1 (1973) Y.K.So, W.T.Pinkston, K.T.R.Davies Nucleon Transfer Form Factors Calculated with Realistic Interactions NUCLEAR REACTIONS 40,42Ca(p, d); calculated form factor.
1972BH02 Particles Nucl. 3, 47 (1972) M.G.Bhattacharya, W.T.Pinkston Effect of the D-State on the Effective Interaction for (3He, t) Reactions
1971MC15 Particles Nucl. 1, 412 (1971) G.M.McAllen, W.T.Pinkston, G.R.Satchler Form Factors and Analysis of (p, d) Pick-up for Some Light Nuclei NUCLEAR REACTIONS 12C, 14N, 16O(p, d), E=30 MeV; calculated σ(θ), pickup form factors. Microscopic formalism.
1971TR04 Phys.Rev. C3, 2421 (1971) W.W.True, C.W.Ma, W.T.Pinkston Negative-Parity States in Pb208 NUCLEAR STRUCTURE 208Pb; calculated levels, T(El), S, isobaric analog.
doi: 10.1103/PhysRevC.3.2421
1969SA17 Phys.Rev. 182, 1141 (1969) G.R.Satchler, D.D.Armstrong, A.G.Blair, E.R.Flynn, R.J.Philpott, W.T.Pinkston Excitation of the 3/2+, 2.02-MeV State in 41Ca by the (t, d) Reaction NUCLEAR REACTIONS 40Ca(t, d), E=20 MeV; measured σ(θ); deduced optical model parameters. 41Ca levels deduced S.
doi: 10.1103/PhysRev.182.1141
1966HU09 Nucl.Phys. 82, 129 (1966) T.A.Hughes, R.Snow, W.T.Pinkston Central and Tensor Potentials in Nuclear Shell Model Calculations NUCLEAR STRUCTURE 42Ca, 42Sc, 18O, 18F, 206Tl, 206Pb, 208Tl, 208Bi, 210Pb, 210Bi, 210Po, 86Sr, 90Y, 90Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90527-X
1963PI01 Can.J.Phys. 41, 478 (1963) Two-Hole Two-Particle Levels in Pb208 NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p63-050
1962PI03 Nuclear Phys. 37, 312 (1962) Shell Theory and Pb208 (II) NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90267-5
1961PI04 Nuclear Phys. 27, 270 (1961) Collective Effects in Inelastic Scattering from Nuclei NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90349-2
1960CA13 Phys.Rev. 120, 504 (1960) J.C.Carter, W.T.Pinkston, W.W.True Shell Model and Pb208 NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.504
1960WA12 Phys.Rev. 118, 733 (1960) Shell Model Assignments for the Energy Levels of C14 and N14 NUCLEAR STRUCTURE 14N, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.118.733
1959PI45 Phys.Rev. 115, 963 (1959) Shell-Model Theory of Inelastic Scattering on Be9
doi: 10.1103/PhysRev.115.963
1959WA02 Bull.Am.Phys.Soc. 4, No.4, 219, AB9 (1959) E.K.Warburton, W.T.Pinkston, H.J.Rose, E.N.Hatch Direct Radiative Capture of Protons by C13
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