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NSR database version of May 22, 2024.

Search: Author = W.C.Parke

Found 15 matches.

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2000MA16      Phys.Rev. C61, 045502 (2000)

L.C.Maximon, W.C.Parke

Radiative Corrections to Elastic Electron-Proton Scattering for Polarized Electrons

NUCLEAR REACTIONS 1H(polarized e, e), E=high; calculated radiative corrections.

doi: 10.1103/PhysRevC.61.045502
Citations: PlumX Metrics

1997KO63      Few-Body Systems 23, 53 (1997)

Y.Koike, W.C.Parke, L.C.Maximon, D.R.Lehman

Accurate Three-Nucleon Bound-State Calculation with an Extended Separable Expansion of the Two-Body T-Matrix

NUCLEAR STRUCTURE 3H; calculated binding energy. Extended seperable expansion, two-potential formalism.

doi: 10.1007/s006010050064
Citations: PlumX Metrics

1991PA25      Few-Body Systems 11, 89 (1991)

W.C.Parke, Y.Koike, D.R.Lehman, L.C.Maximon

Quality of the Three-Nucleon Bound-State Wave Function from a Two-Nucleon Separable Expansion Method

NUCLEAR STRUCTURE 3H; calculated binding energy, convergence; deduced wave function quality. Separable expansion method.

doi: 10.1007/BF01318554
Citations: PlumX Metrics

1989ES05      Phys.Rev. C39, 1685 (1989)

A.Eskandarian, D.R.Lehman, W.C.Parke

Inelastic (1+ → 0+) Electromagnetic Form Factor of 6Li from Three-Body Models

NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated charge form factor. 6Li level deduced deexcitation Γγ. Three-body models.

doi: 10.1103/PhysRevC.39.1685
Citations: PlumX Metrics

1989LA13      Phys.Rev.Lett. 62, 2925 (1989)

J.B.J.M.Lanen, A.M.van den Berg, H.P.Blok, J.F.J.van den Brand, C.T.Christou, R.Ent, A.G.M.van Hees, E.Jans, G.J.Kramer, L.Lapikas, D.R.Lehman, W.C.Parke, E.N.M.Quint, G.van der Steenhoven, P.K.A.de Witt Huberts

Electrodisintegration of 6Li Studied with the Reaction 6Li(e, e'p)

NUCLEAR REACTIONS 6Li(e, e'p), E not given; measured missing energy spectra, momentum distributions; deduced spectroscopic strength. Three-body model.

doi: 10.1103/PhysRevLett.62.2925
Citations: PlumX Metrics

1988CH05      Phys.Rev. C37, 445 (1988)

C.T.Christou, D.R.Lehman, W.C.Parke

Structure of the 6Li → p + (nα) Vertex: Three-body formalism

NUCLEAR STRUCTURE 6Li; calculated three-body vertex structure.

doi: 10.1103/PhysRevC.37.445
Citations: PlumX Metrics

1988CH06      Phys.Rev. C37, 458 (1988)

C.T.Christou, D.R.Lehman, W.C.Parke

Structure of the 6Li → p + (nα) Vertex: 6Li(p, 2p)nα reaction

NUCLEAR REACTIONS, MECPD 6Li(p, 2p), E=100-460 MeV; calculated σ(θ1, θ2, E1, E2). Three-body models.

doi: 10.1103/PhysRevC.37.458
Citations: PlumX Metrics

1988ES01      Phys.Rev. C38, 2341 (1988); Erratum Phys.Rev. C39, 1188 (1989)

A.Eskandarian, D.R.Lehman, W.C.Parke

Elastic Electromagnetic Form Factors of 6Li from Three-Body Models

NUCLEAR STRUCTURE 6Li; calculated monopole, quadrupole, magnetic form factors. Three-body model, Pauli repulsion for the valence nucleons.

doi: 10.1103/PhysRevC.38.2341
Citations: PlumX Metrics

1986LE21      Few-Body Systems 1, 193 (1986)

D.R.Lehman, W.C.Parke

L-S Coupling and the Magnetic Moment of 6Li from Three-Body Models

NUCLEAR MOMENTS 6Li; calculated μ, L-S orbital probabilities. Three-body models.

doi: 10.1007/BF01076711
Citations: PlumX Metrics

1985CH01      Phys.Rev. C31, 250 (1985)

C.T.Christou, C.J.Seftor, W.J.Briscoe, W.C.Parke, D.R.Lehman

Consequences of Pauli Effects in 6Li and the Reaction 6Li(e, e'd)4He

NUCLEAR REACTIONS 6Li(e, e'd), E=400 MeV; calculated σ(θd, θ(e), E(e)); deduced α-d cluster momentum, Pauli effect role. One-photon exchange, deuteron pole dominance.

doi: 10.1103/PhysRevC.31.250
Citations: PlumX Metrics

1985LE08      Phys.Rev. C31, 1920 (1985); Erratum Phys.Rev. C37, 2266 (1988)

D.R.Lehman, W.C.Parke

6Li → α + d Distorted-Wave Born Approximation Parameter D2

NUCLEAR REACTIONS 4He(d, d), E not given; calculated S-, D-wave function, D2 parameter; deduced relevance to 6Li three-body model interpretation, tensor force α-nucleon interaction roles.

doi: 10.1103/PhysRevC.31.1920
Citations: PlumX Metrics

1984PA08      Phys.Rev. C29, 2319 (1984); Erratum Phys.Rev. C34, 1496 (1986)

W.C.Parke, D.R.Lehman

Further Consequences of the Excluded Bound State S1/2 α - N Interaction in 6He and 6Li

NUCLEAR STRUCTURE 6Li, 6He; calculated spectator wave function parameters, wave function normalization, single nucleon radial densities, rms orbital radii. 6Li calculated cluster α+d l=0, 1, 2 partial wave momentum distributions. Atractive α-nucleus interaction, three-body models.

RADIOACTIVITY 6He(β-); calculated β-decay rate, ft. Three-body models.

doi: 10.1103/PhysRevC.29.2319
Citations: PlumX Metrics

1983LE01      Phys.Rev.Lett. 50, 98 (1983)

D.R.Lehman, W.C.Parke

A = 6 Shell Structure from Three-Body Dynamics

NUCLEAR STRUCTURE 6Li, 6He; calculated single particle radial densities, orbital probabilities. Shell model, three-body dynamics.

doi: 10.1103/PhysRevLett.50.98
Citations: PlumX Metrics

1983LE14      Phys.Rev. C28, 364 (1983)

D.R.Lehman, W.C.Parke

Shell Structure of the A = 6 Ground States from Three-Body Dynamics

NUCLEAR STRUCTURE 6He, 6Li; calculated orbital probabilities, single particle radial densities. Three-body model.

doi: 10.1103/PhysRevC.28.364
Citations: PlumX Metrics

1978PA02      Phys.Lett. 74B, 158 (1978)

W.C.Parke, A.Ghovanlou, C.T.Noguchi, M.Rajan, D.R.Lehman

6He β-Decay from a Three-Body Model of the A=6 System

RADIOACTIVITY 6He; calculated β-decay rate, ft.

doi: 10.1016/0370-2693(78)90542-7
Citations: PlumX Metrics

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