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NSR database version of May 22, 2024.

Search: Author = W.T.Pinkston

Found 30 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1984PI02      Phys.Rev. C29, 1123 (1984)

W.T.Pinkston

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
Citations: PlumX Metrics


1984PI14      Phys.Rev. C30, 1431 (1984)

W.T.Pinkston, Da Hsuan Feng

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
Citations: PlumX Metrics


1984SA04      Phys.Lett. 134B, 7 (1984)

G.R.Satchler, W.T.Pinkston

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
Citations: PlumX Metrics


1983SA33      Nucl.Phys. A411, 144 (1983)

G.R.Satchler, W.T.Pinkston

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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1979PI10      Nucl.Phys. A330, 91 (1979)

W.T.Pinkston, P.J.Iano

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1977PI10      Nucl.Phys. A291, 342 (1977)

W.T.Pinkston

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
Citations: PlumX Metrics


1975IA01      Nucl.Phys. A237, 189 (1975)

P.J.Iano, W.T.Pinkston

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1963PI01      Can.J.Phys. 41, 478 (1963)

W.T.Pinkston, W.W.True

Two-Hole Two-Particle Levels in Pb208

NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p63-050
Citations: PlumX Metrics


1962PI03      Nuclear Phys. 37, 312 (1962)

W.T.Pinkston

Shell Theory and Pb208 (II)

NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90267-5
Citations: PlumX Metrics


1961PI04      Nuclear Phys. 27, 270 (1961)

W.T.Pinkston, G.R.Satchler

Collective Effects in Inelastic Scattering from Nuclei

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(61)90349-2
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1960WA12      Phys.Rev. 118, 733 (1960)

E.K.Warburton, W.T.Pinkston

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
Citations: PlumX Metrics


1959PI45      Phys.Rev. 115, 963 (1959)

W.T.Pinkston

Shell-Model Theory of Inelastic Scattering on Be9

doi: 10.1103/PhysRev.115.963
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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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