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Search: Author = W.R.Coker

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1990CO19      Phys.Rev. C42, 659 (1990)

W.R.Coker, L.Ray

Comparison of Dirac and Schrodinger Descriptions of Spin Observables for Proton-Nucleus Elastic Scattering at 650 and 800 MeV

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca, ²⁰⁸Pb(polarized p, p), E=650, 800 MeV; calculated spin rotation parameter, analyzing power vs θ; deduced electromagentic spin-orbit effects role. Relativistic Schrodinger, Dirac equations.

doi: 10.1103/PhysRevC.42.659
Citations: PlumX Metrics

1990CO27      Phys.Rev. C42, 2242 (1990)

W.R.Coker, L.Ray

Nuclear Tensor Term in the Relativistic Impulse Approximation for Proton-Nucleus Elastic Scattering

NUCLEAR REACTIONS ⁴⁰Ca, ²⁰⁸Pb(polarized p, p), E=650, 800 MeV; calculated analyzing power, spin rotation parameter vs θ.

doi: 10.1103/PhysRevC.42.2242
Citations: PlumX Metrics

1985CO07      Phys.Rev. C31, 1412 (1985)

W.R.Coker, J.D.Lumpe, L.Ray

K⁺ Mesons as a Probe of the Nuclear Interior

NUCLEAR REACTIONS ²⁰⁸Pb, ⁴⁰Ca(K⁺, K⁺), (K⁺, K⁺'), E=442, 991 MeV; ⁴⁰Ca, ²⁰⁸Pb(p, p)(p, p'), E=297, 800 MeV; calculated σ(θ); deduced neutron ground state, transition density distributions.

doi: 10.1103/PhysRevC.31.1412
Citations: PlumX Metrics

1984BA11      Phys.Rev. C29, 1407 (1984)

M.L.Barlett, W.R.Coker, G.W.Hoffmann, L.Ray

Effective Isoscalar Nucleon-Nucleon Interactions at 500 MeV

NUCLEAR REACTIONS ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb(polarized p, p), E=500 MeV; analyzed σ(θ), analyzing power, spin rotation parameter vs θ. ⁹⁰Zr, ²⁰⁸Pb deduced neutron-proton rms radius difference. ^40,48Ca deduced neutron-proton, isotopic neutron rms radii differences. Folding model, Schrodinger equivalent Dirac optical potential, effective interactions.

doi: 10.1103/PhysRevC.29.1407
Citations: PlumX Metrics

1984BE05      Phys.Rev. C29, 709 (1984)

R.E.Benenson, M.T.McEllistrem, J.L.Weil, W.R.Coker, T.Tamura

Interference between Reaction Mechanisms in ³²S(³He, n)³⁴Ar

NUCLEAR REACTIONS ³²S(³He, n), E=4.6-6.5 MeV; measured σ(θ) vs E; deduced optical model parameters. ³⁵Ar deduced resonances, J, π, Γ, partial widths. Direct, compound reaction interference effects, DWBA. Tof.

doi: 10.1103/PhysRevC.29.709
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1616.

1984CO01      Phys.Lett. 135B, 363 (1984)

W.R.Coker, G.W.Hoffmann, L.Ray

Relative Sensitivities of Medium Energy K⁺ + Nucleus and p + Nucleus Elastic Angular Distributions to Neutron Density Distributions

NUCLEAR REACTIONS ^40,48Ca(p, p), E=800 MeV; ^40,48Ca(K⁺, K⁺), E=444, 991 MeV; calculated σ(θ); deduced target point neutron density dependences. Relativisitic kinematics, first-order Kerman-McManus-Thaler optical model.

doi: 10.1016/0370-2693(84)90294-6
Citations: PlumX Metrics

1981HO20      Phys.Rev. C24, 541 (1981)

G.W.Hoffmann, L.Ray, M.Barlett, W.R.Coker, J.McGill, G.S.Adams, G.J.Igo, F.Irom, A.T.M.Wang, C.A.Whitten, Jr., R.L.Boudrie, J.F.Amann, C.Glashausser, N.M.Hintz, G.S.Kyle, G.S.Blanpied

A(y)(θ) for p(pol) + ²⁰⁸Pb Elastic Scattering at 0.8 GeV and a Test of Multiple Scattering Theory

NUCLEAR REACTIONS ²⁰⁸Pb(polarized p, p), E=0.8 GeV; measured analyzing power vs θ. Microscopic optical model, second-order Kerman-McManus-Thaler multiple scattering approach, electromagnetic spin-orbit term.

doi: 10.1103/PhysRevC.24.541
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0074.

1979IG01      Phys.Lett. 81B, 151 (1979)

G.Igo, G.S.Adams, T.S.Bauer, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, C.Glashausser, N.M.Hintz, M.A.Oothoudt, H.Nann, K.K.Seth, B.E.Wood, D.K.McDaniels, M.Gazzaly

Elastic Differential Cross Sections and Analyzing Powers for Polarized p + ^40,42,44,48Ca at 0.8 GeV

NUCLEAR REACTIONS ^40,42,44,48Ca(polarized p, p), E=0.8 GeV; measured σ(θ), A(θ); deduced rms radii of neutrons. Kerman-McManus-Thaler optical potential analysis.

doi: 10.1016/0370-2693(79)90510-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1488.

1979LI03      Phys.Rev.Lett. 42, 363 (1979)

R.P.Liljestrand, G.S.Blanpied, W.R.Coker, C.Harvey, G.W.Hoffmann, L.Ray, C.Glashausser, G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., M.A.Oothoudt, B.E.Wood, H.Nann

Effects of Spin-Orbit Deformation in Inelastic Scattering at 0.8 GeV

NUCLEAR REACTIONS ¹²C, ^116,124Sn(polarized p, p'), E=800 MeV; measured σ(θ), A(θ). DWBA analysis with collective form factors, spin-orbit β.

doi: 10.1103/PhysRevLett.42.363
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0390.

1979RA22      Phys.Rev. C20, 1236 (1979)

L.Ray, G.S.Blanpied, W.R.Coker

Coupled-Channels Analysis of Proton Inelastic Scattering to the γ-Vibrational Band in ²⁴Mg

NUCLEAR REACTIONS ²⁶Mg(p, p'), E=20.3, 40, 800 MeV; calculated σ(θ). Coupled channels with additional nuclear vibrational multipole.

doi: 10.1103/PhysRevC.20.1236
Citations: PlumX Metrics

1979ZW01      Nucl.Phys. A315, 124 (1979)

B.Zwieglinski, W.Benenson, R.G.H.Robertson, W.R.Coker

Study of the ¹⁰Be(d, p)¹¹Be Reaction at 25 MeV

NUCLEAR REACTIONS ¹⁰Be(d, p), E=25 MeV; measured σ(θ). ¹¹Be levels deduced S, DWBA analysis. Comparison with shell model. Reactor-produced ¹⁰Be target.

doi: 10.1016/0375-9474(79)90637-7
Citations: PlumX Metrics

1978BL02      Phys.Rev. C18, 1436 (1978)

G.S.Blanpied, W.R.Coker, R.P.Liljestrand, G.W.Hoffmann, L.Ray, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, T.Kozlowski, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, G.Igo, R.J.Ridge, C.A.Whitten, Jr., P.M.Lang, H.Nann, K.K.Seth

Proton Elastic and Inelastic Scattering at 0.8 GeV from ^12,13C and ²⁰⁸Pb

NUCLEAR REACTIONS ^12,13C, ²⁰⁸Pb(p, p'), E=0.8 GeV; measured σ(θ). ^12,13C, ²⁰⁸Pb deduced deformation length. Optical potential, DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.18.1436
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0071.

1978HO05      Phys.Rev.Lett. 40, 1256 (1978)

G.W.Hoffman, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., D.Madland, J.C.Pratt, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese

Analyzing Power in Proton-Nucleus Elastic Scattering at 0.8 GeV

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb(polarized p, p), E=0.8 GeV; measured A(θ), σ(θ).

doi: 10.1103/PhysRevLett.40.1256
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0079.

1978HO12      Phys.Lett. 76B, 383 (1978)

G.W.Hoffmann, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese

Analysis of Elastic Scattering of 0.8 GeV Polarized Protons from ¹¹⁶Sn and ¹²⁴Sn

NUCLEAR REACTIONS ^116,124Sn(polarized p, p), E=800 MeV; analyzed A(θ), σ(θ). Spin-dependent Kerman-McManus-Thaler formalism.

doi: 10.1016/0370-2693(78)90888-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0127.

1978HO18      Phys.Lett. 79B, 376 (1978)

G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, N.M.Hintz, G.Kyle, M.A.Oothoudt, B.E.Wood, D.K.McDaniels, C.Glashausser, M.Gazzaly

Elastic Differential Cross Sections and Analyzing Powers for p + ⁵⁴Fe, ^58,64Ni at 800 MeV

NUCLEAR REACTIONS ⁵⁴Fe, ^58,64Ni(polarized p, p), E=800 MeV; measured σ(θ); deduced neutron density distribution. Approximately model-independent analysis.

doi: 10.1016/0370-2693(78)90386-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0258.

1978RA08      Phys.Rev.Lett. 40, 1547 (1978)

L.Ray, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, G.W.Hoffmann

Coupled-Channels Analysis of Inelastic Proton Scattering from ¹²C at 0.8 GeV

NUCLEAR REACTIONS ¹²C(p, p'), E=0.8 GeV; calculated σ(Ep', θ). DWBA, coupled-channels calculations.

doi: 10.1103/PhysRevLett.40.1547
Citations: PlumX Metrics

1978RA17      Phys.Rev. C18, 1756 (1978)

L.Ray, G.W.Hoffmann, G.S.Blanpied, W.R.Coker, R.P.Liljestrand

Analysis of 0.8-GeV Polarized-Proton Elastic Scattering from ²⁰⁸Pb, ⁹⁰Zr, ⁵⁸Ni, and ¹²C

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb(polarized p, p), E=800 MeV; analyzed σ(θ), A(θ). ¹²C, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb deduced neutron densities, rms radii. Kerman, McManus, Thaler spin-dependent optical potential analysis.

doi: 10.1103/PhysRevC.18.1756
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0071.

1978RA20      Phys.Lett. 79B, 182 (1978)

L.Ray, W.R.Coker

'Spin-Orbit Deformation' in Elastic Scattering of Protons at Medium Energies

NUCLEAR REACTIONS ¹²C(p, p'), E=0.8 GeV; ⁵⁸Ni(p, p'), E=1.04 GeV; ²⁰⁸Pb(p, p'), E=0.8 GeV; calculated σ(θ). ¹²C 4.439-MeV level, ⁵⁸Ni 1.45-MeV, 2.46-MeV levels, ²⁰⁸Pb 2.6-MeV, 3.2-MeV levels deduced spin-orbit deformation length.

doi: 10.1016/0370-2693(78)90217-4
Citations: PlumX Metrics

1978RA22      Phys.Rev. C18, 2641 (1978)

L.Ray, W.R.Coker, G.W.Hoffmann

Uncertainties in Neutron Densities Determined from Analysis of 0.8 GeV Polarized Proton Scattering from Nuclei

NUCLEAR REACTIONS ⁵⁸Ni, ⁹⁰Zr, ^116,124Sn, ²⁰⁸Pb(p, p), E=0.8 GeV; calculated σ(θ), A(θ). Kerman, McManus, Thaler optical potential; deduced model-independent densities, neutron radii.

doi: 10.1103/PhysRevC.18.2641
Citations: PlumX Metrics

1977BL09      Phys.Rev.Lett. 39, 1447 (1977); Erratum Phys.Rev.Lett. 40, 420 (1978)

G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, G.W.Hoffman, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr., Y.Kozlowski, D.K.McDaniels, P.Varghese, P.M.Lang, H.Nann, K.K.Seth, C.Glashausser

Elastic Scattering of 0.8-GeV Protons from ¹²C, ⁵⁸Ni, and ²⁰⁸Pb

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ²⁰⁸Pb(p, p), E=0.8 GeV; measured σ(θ).

doi: 10.1103/PhysRevLett.39.1447
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0260.

1977RA07      Phys.Rev. C16, 340 (1977)

L.Ray, W.R.Coker

'Nuclear Matter' Approach to the Energy Dependence of the Real Part of The Proton-Nucleus Optical Potential at Intermediate Incident Energies

NUCLEAR REACTIONS ⁴⁰Ca, ²⁰⁸Pb(p, p), E=100-1050 MeV; calculated potential, σ.

doi: 10.1103/PhysRevC.16.340
Citations: PlumX Metrics

1976CO18      Phys.Lett. 62B, 374 (1976)

W.R.Coker, T.Tamura

Phenomenological Analysis of ⁴He + ⁴He Scattering at 0.65 and 0.85 GeV

NUCLEAR REACTIONS ⁴He(α, α), E=650, 850 MeV; calculated σ.

doi: 10.1016/0370-2693(76)90660-2
Citations: PlumX Metrics

1976CO30      Phys.Lett. 64B, 403 (1976)

W.R.Coker, L.Ray, G.W.Hoffmann

DWBA Approach to Inelastic Scattering at Medium Energies

NUCLEAR REACTIONS ⁵⁸Ni, ²⁰⁸Pb(p, p), (p, p'), E=1.04 GeV; ⁴⁰Ca(α, α), (α, α'), E=1.37 GeV; calculated σ(θ). Partial wave approach.

doi: 10.1016/0370-2693(76)90106-4
Citations: PlumX Metrics

1976FO03      Nucl.Phys. A262, 365 (1976)

J.C.Fong, M.M.Gazzaly, G.Igo, A.D.Liberman, R.J.Ridge, S.L.Verbeck, C.A.Whitten, Jr., V.Perez-Mendez, W.R.Coker

The Elastic Scattering of α-Particles from Helium at 0.85 and 0.65 GeV

NUCLEAR REACTIONS ⁴He(α, α), E=650, 850 MeV; measured σ(θ). Results compared with predictions of α-α potential obtained by a folding procedure which used a p-α potential, α charge distribution.

doi: 10.1016/0375-9474(76)90503-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2776.

1976RA06      Phys.Rev. C13, 1367 (1976)

L.Ray, W.R.Coker

Multistep Inelastic Processes in the Reaction ²⁸Si(³He, d)²⁹P Leading to Bound and Unbound States

NUCLEAR REACTIONS ²⁸Si(³He, d), E=20, 35.3, 40 MeV; calculated σ(Ed, θ); deduced multistep inelastic contributions. ²⁹P levels deduced S. DWBA, CCBA.

doi: 10.1103/PhysRevC.13.1367
Citations: PlumX Metrics

1975CO16      Z.Phys. A273, 251 (1975)

W.R.Coker

Comments on 'The (³He, d) Reaction on ²⁸Si'

NUCLEAR REACTIONS ²⁸Si(³He, d), E=18-40 MeV; analyzed data; deduced inconsistencies in previous analyses. ²⁹P levels deduced S.

doi: 10.1007/BF01410005
Citations: PlumX Metrics

1975LI09      Phys.Rev. C11, 1570 (1975)

R.Liljestrand, J.McIntyre, G.Blanpied, J.Lynch, L.Ray, W.R.Coker, G.W.Hoffmann

Fractionated Single-Particle States of ³³S at E(x) = 8.6-9.5 MeV

NUCLEAR REACTIONS ³²S(d, p), Ed=12 MeV; measured σ(θ). ³³S deduced levels, L, J, π, S. DWBA analysis, resolution 12 keV; comparison to neutron total σ, ³²S.

doi: 10.1103/PhysRevC.11.1570
Citations: PlumX Metrics

1975RA13      Phys.Lett. 56B, 318 (1975)

L.Ray, W.R.Coker, T.Udagawa

Exact Finite-Range DWBA Treatment of Heavy-Ion-Induced Reactions to Unbound Residual States

NUCLEAR REACTIONS ⁴⁰Ca(³He, d), E=40 MeV; calculated σ(Ed, θ). ⁴⁰Ca(¹⁴N, ¹³C), E=154.5 MeV; calculated σ(E(¹³C), θ). ¹²C(¹⁰B, ⁹Be), E=100 MeV; calculated σ(E(⁹Be), θ).

doi: 10.1016/0370-2693(75)90308-1
Citations: PlumX Metrics

1975RA33      Phys.Lett. 59B, 427 (1975)

L.Ray, G.Westfall, S.A.A.Zaidi, W.R.Coker

Elastic Scattering of the Carbon Isotopes from Light Nuclei (Z=7 to 16) In Optical Model, Strong-Absorption, and Folding Approaches

NUCLEAR REACTIONS ¹⁶O, ²⁸Si, ³²S(¹²C, ¹²C), (¹³C, ¹³C), E=36-40 MeV; ¹²C(¹⁴N, ¹⁴N), E=155 MeV; analyzed data.

doi: 10.1016/0370-2693(75)90337-8
Citations: PlumX Metrics

1974CO03      Phys.Rev. C9, 784 (1974)

W.R.Coker

Gamow-State Analysis of ⁵⁴Fe(d, n) to Proton Resonances in ⁵⁵Co

NUCLEAR REACTIONS ⁵⁴Fe(d, n), E=10.0 MeV; measured nothing, calculated σ(θ); ⁵⁵Co deduced proton-unbound levels, J, π.

doi: 10.1103/PhysRevC.9.784
Citations: PlumX Metrics

1974CO26      Phys.Rev. C10, 1130 (1974)

W.R.Coker, T.Udagawa, J.R.Comfort

Successive Pickup Contributions to the ⁹⁸Mo(d, α)⁹⁶Nb Reaction

NUCLEAR REACTIONS ^92,98Mo(d, α), E=17 MeV; calculated σ(Eα, θ), DWBA, coupled-reaction channels.

doi: 10.1103/PhysRevC.10.1130
Citations: PlumX Metrics

1974CO32      Phys.Rev. C10, 1792 (1974)

W.R.Coker, T.Udagawa, G.W.Hoffmann

Coupled-Channel Born Approximation and l = 2j Dependence in ²⁸Si(d, p)²⁹Si from 10 to 18 MeV

NUCLEAR REACTIONS ²⁸Si(d, p), E=10.0, 13.0, 18.0 MeV; calculated σ(θ) with coupled channel Born approximation. L=2j dependence of σ(θ) accounted for.

doi: 10.1103/PhysRevC.10.1792
Citations: PlumX Metrics

1974HO16      Phys.Lett. 50B, 249 (1974)

G.W.Hoffmann, T.Udagawa, W.R.Coker, J.McIntyre, M.Mahlab

The Coupled-Channel Born Approximation and J-Dependence in ³⁰Si(d, p)³¹Si

NUCLEAR REACTIONS ³⁰Si(d, p), E=10 MeV; measured σ(Ep, θ). ³¹Si levels deduced reaction mechanism.

doi: 10.1016/0370-2693(74)90551-6
Citations: PlumX Metrics

1974HO22      Z.Phys. 269, 307 (1974)

G.W.Hoffmann, W.R.Coker

Microscopic Versus Macroscopic Descriptions of the (p, n) Charge-Exchange Reaction

NUCLEAR REACTIONS ^90,91Zr(p, n), E=22-40 MeV; calculated σ(E, θ).

doi: 10.1007/BF01668601
Citations: PlumX Metrics

1974HO28      Phys.Rev. C10, 1671 (1974)

G.W.Hoffmann, J.McIntyre, W.R.Coker

Fractionated Single-Particle States of ³¹Si at E(x) = 5.3-9.4 MeV

NUCLEAR REACTIONS ³⁰Si(d, p), Ed=10 MeV; measured σ(Ep, θ). ³¹Si deduced levels, L, J, π, S. Enriched target.

doi: 10.1103/PhysRevC.10.1671
Citations: PlumX Metrics

1974HO33      Nucl.Instrum.Methods 120, 489 (1974)

G.W.Hoffmann, J.McIntyre, M.Mahlab, W.R.Coker

Biased Magnetic Quadrupole Spectrometer for High-Resolution Charged-Particle Mass Identification

NUCLEAR REACTIONS ³⁰Si(d, p), E=10 MeV; measured Ep.

doi: 10.1016/0029-554X(74)90014-7
Citations: PlumX Metrics

1973CO09      Phys.Rev. C7, 1154 (1973)

W.R.Coker, T.Udagawa, H.H.Wolter

Coupled-Reaction-Channels Study of (h, t) Reactions

NUCLEAR REACTIONS ⁴⁰Ar(³He, t), ⁴⁸Ca(³He, t) calculated contribution of (³He, α)-(α, t) two-step process to σ(θ).

doi: 10.1103/PhysRevC.7.1154
Citations: PlumX Metrics

1973CO14      Phys.Rev. C7, 2426 (1973)

W.R.Coker

Distorted-Wave Born-Approximation Analysis of ^36,38Ar(d, p) to Neutron Resonances in ^37,39Ar

NUCLEAR REACTIONS ^36,38Ar(d, p), E=9, 10 MeV; measured nothing. ^37,39Ar resonances deduced level-width, S, L, DWBA.

doi: 10.1103/PhysRevC.7.2426
Citations: PlumX Metrics

1973CO19      Phys.Lett. 45B, 321 (1973)

W.R.Coker, J.Lin, J.L.Duggan, P.D.Miller

Multistep Contributions to ¹¹B(h, α)¹⁰B from 8.0 to 12.0 MeV

NUCLEAR REACTIONS ¹¹B(³He, α), E=8.0, 10.0, 12.0 MeV; measured σ(θ). ¹⁰B level deduced S.

doi: 10.1016/0370-2693(73)90044-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0447.

1973CO22      Phys.Lett. 46B, 27 (1973)

W.R.Coker, T.Udagawa, H.H.Wolter

Multistep Contributions in ⁸⁸Sr(h, t)⁸⁸Y

NUCLEAR REACTIONS ⁸⁸Sr(³He, t), E=23 MeV; calculated σ(θ). ⁸⁸Y levels calculated relative strengths.

doi: 10.1016/0370-2693(73)90466-8
Citations: PlumX Metrics

1973CO24      Z.Phys. 263, 179 (1973)

W.R.Coker, G.W.Hoffmann

Analysis of Stripping to Analog Resonances Using Complex Energy Eigenstates

NUCLEAR REACTIONS ⁹²Mo(³He, d), E=30.2 MeV; calculated σ(Ed, θ). ⁹³Tc levels deduced L, S, level-width.

doi: 10.1007/BF01392560
Citations: PlumX Metrics

1973HO45      Phys.Lett. 47B, 285 (1973)

G.W.Hoffmann, W.R.Coker

Complex Microscopic Effective Interaction for (p, n) Reactions

NUCLEAR REACTIONS ²⁰⁸Pb, ²⁰⁹Bi(p, n), E=25-50 MeV; calculated σ(En, θ).

doi: 10.1016/0370-2693(73)90602-3
Citations: PlumX Metrics

1973KE01      Phys.Rev. C7, 388 (1973)

J.J.Kent, W.R.Coker, C.F.Moore

Inelastic Proton Scattering from ⁹⁶Mo Through Isobaric Analog Resonances

NUCLEAR REACTIONS ⁹⁶Mo(p, p'), (p, p), E=5.2-8.0 MeV; measured σ(θ). ⁹⁶Mo level deduced J, π. ⁹⁷Tc deduced IAR, level-width, J, π, S.

doi: 10.1103/PhysRevC.7.388
Citations: PlumX Metrics

1973ZA01      Z.Phys. 260, 329 (1973)

S.A.A.Zaidi, G.W.Hoffmann, W.R.Coker

The ⁸⁸Sr(d, np)⁸⁸Sr Reaction

NUCLEAR REACTIONS ⁸⁸Sr(d, np), E=7.5-10 MeV; measured σ(E;Ep, θ).

doi: 10.1007/BF01396024
Citations: PlumX Metrics

1972CO14      Nucl.Phys. A188, 65 (1972)

W.R.Coker, S.A.A.Zaidi

(³He, d) Population of Analog Resonances in ⁹³Tc

NUCLEAR REACTIONS ⁹²Mo(³He, d), E=35 MeV; analyzed σ(θ). ⁹³Tc deduced IAR, S, L(p).

doi: 10.1016/0375-9474(72)90180-7
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1972CO19      Phys.Lett. 40B, 81 (1972)

W.R.Coker, G.W.Hoffmann

Microscopic Form Factors for Charge Exchange Reactions to Unbound Residual States

doi: 10.1016/0370-2693(72)90288-2
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1972CO21      Phys.Lett. 40B, 164 (1972)

W.R.Coker, H.Bledsoe, T.Tamura

Total and Partial Widths of Isobaric Analog Resonances

NUCLEAR REACTIONS ⁸⁶Kr, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ⁹²Zr, ⁹⁶Mo(p, p), analyzed σ(E). ⁸⁷Rb, ⁸⁹Y, ⁹¹Nb, ⁹³Tc, ⁹³Nb, ⁹⁷Tc deduced IAR level-width, S, resonance mixing phases.

doi: 10.1016/0370-2693(72)90398-X
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1972CO29      Phys.Lett. 41B, 237 (1972)

W.R.Coker, T.Udagawa, H.H.Wolter

Contribution of Single-Nucleon Transfer Reactions to ⁴⁰Ar(tau, t)⁴⁰K

NUCLEAR REACTIONS ⁴⁰Ar(³He, t), E=35, 18 MeV; analyzed σ(θ); deduced reaction mechanism. ⁴⁰K deduced analog, antianalog states amplitudes.

doi: 10.1016/0370-2693(72)90567-9
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1972HO27      Phys.Rev.Lett. 29, 227 (1972); Erratum Phys.Rev.Lett. 30, 249 (1973)

G.W.Hoffmann, W.R.Coker

Coupled-Channel Calculations of the Energy Dependence of the (p, n) Charge-Exchange Reaction

NUCLEAR REACTIONS ⁹¹Zr, ¹¹⁹Sn, ²⁰⁸Pb, ²⁰⁹Bi(p, np), E=20-48 MeV; analyzed σ(E). DWBA, coupled-channel formalisms.

doi: 10.1103/PhysRevLett.29.227
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1972HO29      Phys.Lett. 40B, 453 (1972)

G.W.Hoffmann, W.H.Dunlop, G.J.Igo, J.G.Kulleck, C.A.Whitten, Jr., W.R.Coker

Energy Dependence of the (p, np) Reaction

NUCLEAR REACTIONS ⁹¹Zr, ¹¹⁹Sn, ²⁰⁸Pb, ²⁰⁹Bi(p, np), E < 45 MeV; measured σ(E). DWBA analysis.

doi: 10.1016/0370-2693(72)90549-7
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1972HO36      Phys.Lett. 41B, 47 (1972)

G.W.Hoffmann, W.R.Coker, S.A.A.Zaidi, D.O.Elliott, Jr.

A Consistent Coupled Channel Born Approximation Analysis of ⁸⁸Sr(d, np)⁸⁸Sr and ⁸⁸Sr(d, p)⁸⁹Sr

NUCLEAR REACTIONS ⁸⁸Sr(d, np), E < 10 MeV; measured σ(E). Consistent coupled-channel Born approximation.

doi: 10.1016/0370-2693(72)90364-4
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1972KE32      Z.Phys. 256, 199 (1972)

J.J.Kent, W.R.Coker, C.E.Watson

Absence of Proton Weak Coupling States in ⁹³Nb

NUCLEAR REACTIONS ⁹³Nb(p, p)(p, n), (p, p'), E=5.8-7.6 MeV; measured σ(E). ⁹⁴Mo deduced IAR, level-width. ⁹³Nb deduced levels.

doi: 10.1007/BF01392093
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1972MO36      Phys.Rev. C6, 1391 (1972)

C.F.Moore, G.W.Hoffmann, J.F.Fitch, W.R.Coker

In-Beam Internal-Conversion Electrons from ⁹²Mo + p

NUCLEAR REACTIONS ⁹²Mo(p, p'γ), (p, nγ) , E=8, 11 MeV; measured E(ce). ⁹²Mo, ⁹²Tc deduced levels.

doi: 10.1103/PhysRevC.6.1391
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1972PI04      Phys.Rev. C6, 170 (1972)

J.M.Picone, W.R.Coker, J.F.Fitch, C.F.Moore

Excited States in ⁹⁷Tc from the Reaction ⁹⁷Mo(p, nγ)⁹⁷Tc

NUCLEAR REACTIONS ⁹⁷Mo(p, nγ), E=3-6 MeV; measured Eγ, Iγ, γγ-coin. ⁹⁷Tc deduced levels, J, π, γ-branching.

doi: 10.1103/PhysRevC.6.170
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1971CO01      Priv.Comm. (January 1971)

W.R.Coker

1971CO14      Nucl.Phys. A168, 307 (1971)

W.R.Coker, P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, J.Lin

The ¹⁴C(t, α₀)¹³C Reaction at 6.0, 8.0 and 10.0 MeV

NUCLEAR REACTIONS ¹⁴C(³He, α), ¹⁴C(³He, ³He), E=6.0, 8.0, 10.0 MeV; ¹³C(α, α), E=15, 18, 20 MeV; measured σ(θ); deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(71)90795-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2331.

1971CO21      Phys.Rev. C4, 836 (1971)

W.R.Coker, C.L.Hollas, P.J.Riley, S.Sen

⁸⁶Kr(d, n)⁸⁷Rb(A) Threshold Cusp and the Systematic Appearance of Charge-Exchange Cusps

NUCLEAR REACTIONS ⁸⁶Kr(d, n), E=5-10.5 MeV; measured σ(E); deduced charge-exchange effects coupled-channel Born approximation.

doi: 10.1103/PhysRevC.4.836
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1971HO11      Z.Phys. 243, 446 (1971)

F.F.Hopkins, W.J.Courtney, W.R.Coker, C.F.Moore, P.Richard

²⁰⁸Pb(p, α)²⁰⁵Tl Reaction at 16.475 MeV

NUCLEAR REACTIONS ²⁰⁸Pb(p, α), E=16.475 MeV; measured σ(Eα, θ). ²⁰⁵Tl deduced levels, J, π.

doi: 10.1007/BF01396619
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1971SU06      Nucl.Phys. A176, 89 (1971)

S.H.Suck, W.R.Coker

Pick-up Form Factors for (p, α) Reactions

NUCLEAR REACTIONS ^90,92Zr(p, α), E=20, 28 MeV; analyzed σ(θ); deduced pickup form factors.

doi: 10.1016/0375-9474(71)90732-9
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1971ZA05      Phys.Rev. C4, 236 (1971)

S.A.A.Zaidi, W.R.Coker

Form Factors for Proton Transfer Reactions to Unbound Isobaric Analog States

NUCLEAR REACTIONS ⁹²Mo(d, n), E=12 MeV; calculated σ(θ), isobaric analog resonance form factors.

doi: 10.1103/PhysRevC.4.236
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1970CL04      Phys.Rev. C2, 1097 (1970)

R.G.Clarkson, W.R.Coker, C.F.Moore

Effects of Charge Exchange in ^90,91Zr(d, p)

NUCLEAR REACTIONS ^90,91Zr(d, d), E=5-11 MeV; ^90,91Zr(p, p), E=9.5-14 MeV; measured σ(E;θ); deduced optical model parameters. ^90,91Zr(d, p), E=5-11 MeV; measured σ(E;Ep, θ), analyzing power(E;θ); deduced charge exchange effects.

doi: 10.1103/PhysRevC.2.1097
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1970CL05      Phys.Rev. C2, 1108 (1970)

R.G.Clarkson, W.R.Coker

Charge Exchange in ⁹²Zr(d, p)⁹³Zr

NUCLEAR REACTIONS ⁹²Zr(d, p), E=4.2-11.2 MeV; measured σ(E;Ep, θ). ⁹²Zr(d, d), E=6.25, 7.5, 11 MeV; measured σ(θ); deduced optical model parameters. ⁹³Zr deduced levels, L(n), S.

doi: 10.1103/PhysRevC.2.1108
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1970CO29      Phys.Rev. C2, 2023 (1970)

W.R.Coker, J.J.Kent

Charge-Exchange Threshold Effect in ⁹³Nb(d, p)⁹⁴Nb

NUCLEAR REACTIONS ⁹³Nb(d, p), E=5-10 MeV; measured σ(E); deduced charge-exchange threshold effect.

doi: 10.1103/PhysRevC.2.2023
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1970HA16      Phys.Rev. C1, 938 (1970)

K.Haravu, C.L.Hollas, P.J.Riley, W.R.Coker

⁸⁶Kr(d, p)⁸⁷Kr Reaction

NUCLEAR REACTIONS ⁸⁶Kr(d, p), E=11 MeV; measured σ(Ep, θ). ⁸⁷Kr deduced levels, J, π, S, L(n).

doi: 10.1103/PhysRevC.1.938
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1970MO15      Nucl.Instrum.Methods 79, 353 (1970)

C.F.Moore, J.G.Kulleck, W.R.Coker, R.G.Clarkson, J.J.Kent, W.J.Courtney

Detection of Internal Conversion Electrons in Charged Particle Spectra

NUCLEAR REACTIONS ⁹⁰Zr(p, p'), E=7.34 MeV; Zr(p, X), E=9.4 MeV; ⁸⁹Y(p, n), (p, p'), E not given; ⁷²Ge(p, n), E=5.2-5.9 MeV; measured E(ce), σ(E). Detector - Si(Li).

doi: 10.1016/0029-554X(70)90164-3
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1970ZA08      Phys.Rev. C2, 1384 (1970)

S.A.A.Zaidi, W.R.Coker, D.G.Martin

⁸⁸Sr(d, p)⁸⁹Sr Reaction in the Region of the ⁸⁸Sr(d, n)⁸⁹Y(A) Threshold

NUCLEAR REACTIONS ⁸⁸Sr(d, p), E=5.-10.5 MeV; measured σ(E;θ); deduced charge exchange threshold.

doi: 10.1103/PhysRevC.2.1384
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1969CU08      Phys.Rev. 185, 1416 (1969)

J.R.Curry, W.R.Coker, P.J.Riley

Direct Two-Nucleon Pickup in (d, α) Reactions

NUCLEAR REACTIONS ¹³C, ¹⁴N, ³¹P(d, α), E = 10-12 MeV; ³¹P(d, α), E = 33.7 MeV; measured σ(Eα, θ). ¹¹B, ¹²C, ²⁹Si levels deduced L, J. Zero-range DWBA.

doi: 10.1103/PhysRev.185.1416
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1969MI15      Nucl.Phys. A136, 229 (1969)

P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, W.R.Coker, J.Lin

¹¹B(³He, d)¹²C Spectroscopic Factors

NUCLEAR REACTIONS ¹¹B(³He, d), (³He, ³He); E = 10, 12, 18 MeV; measured σ(Ed, θ). ¹²C levels deduced S. Enriched target.

doi: 10.1016/0375-9474(69)90050-5
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1967CO03      Nucl.Phys. A91, 97 (1967)

W.R.Coker, M.M.Duncan, J.L.Duggan, P.D.Miller

An Investigation of the ⁹Be(³He, p)¹¹B Reaction at Low Energies

NUCLEAR REACTIONS ⁹Be(³He, p), E = 1-3 MeV; measured σ(Ep, θ). ¹¹B deduced levels J, π, L.

doi: 10.1016/0375-9474(67)90453-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0413.

1967CO21      Phys.Letters 25B, 271 (1967)

W.R.Coker, C.F.Moore

Charge Exchange Effects in ⁸⁰Se(d, p)⁸¹Se

NUCLEAR STRUCTURE ⁸¹Se; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90010-X
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1967MO19      Phys.Letters 25B, 468 (1967)

C.F.Moore, W.R.Coker, V.Valkovic, C.Joseph, J.Sandler

Coincidence Spectra of the ⁹²Mo(d, np)⁹²Mo Reaction

NUCLEAR STRUCTURE ⁹³Tc; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90110-4
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1963CO24      Bull.Am.Phys.Soc. Southeastern Section, p. 18, S8, (November 1963); Bull.Am.Phys.Soc. 9, No.3, 351, S8 (1964)

W.R.Coker, M.M.Duncan, J.L.Duggan, V.H.Webb, P.D.Miller

The Be⁹(He³, p)B¹¹ Reaction

NUCLEAR STRUCTURE ⁹Be; measured not abstracted; deduced nuclear properties.