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NSR database version of April 11, 2024.

Search: Author = W.R.Coker

Found 72 matches.

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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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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.


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