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NSR database version of April 11, 2024.

Search: Author = J.L.Foster

Found 18 matches.

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1984CE01      Phys.Rev. C29, 49 (1984)

M.L.Cescato, M.C.Hermida, M.Ruiz, J.L.Foster, Jr., F.Krmpotic

144Sm(p, p') Scattering Isobaric Analog Resonances and the Structure of 145Sm

NUCLEAR STRUCTURE 145Sm; calculated low-lying parent state spectroscopic factors. Input from 144Sm(p, p') data analysis.

NUCLEAR REACTIONS 144Sm(p, p), (p, p'), E=8.5-14 MeV; measured σ(θ), σ(θ) vs E; deduced optical model parameters. 145Eu deduced IAR, J, π, Γp, Γp', Γ, spectroscopic factors.

doi: 10.1103/PhysRevC.29.49
Citations: PlumX Metrics


1984FO10      Phys.Rev. C30, 79 (1984)

J.L.Foster, Jr., S.E.Darden, M.C.Rozak, J.A.Ross, J.P.Martin, L.Lessard, S.Gales, G.Noury, J.M.Pearson, P.Depommier, M.C.Hermida, M.Ruiz

130Te(p(pol), p1) and 130Te(p, p1(pol)) Reactions on Analog Resonances

NUCLEAR REACTIONS 130Te(polarized p, p), (polarized p, p'), E(cm)=10.1-10.7 MeV; measured σ(θ) vs E, analyzing power vs θ, E, polarization vs θ; deduced optical model parameters. 131I deduced IAR, J, π, configuaration. Coupled-channels analysis.

doi: 10.1103/PhysRevC.30.79
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0096.


1984HE01      Phys.Rev. C29, 64 (1984)

M.C.Hermida, M.Ruiz, M.L.Cescato, J.L.Foster, Jr., F.Krmpotic

130Te(p, p') Reaction on Analog Resonances

NUCLEAR STRUCTURE 131Te; calculated low-lying parent state spectroscopic amplitudes.

NUCLEAR REACTIONS 130Te(p, p), (p, p'), E=7.5-14 MeV; measured σ(θ), σ(θ) vs E; deduced optical model parameters. 131I deduced IAR, Γp, Γp', Γ, spectroscopic amplitudes.

doi: 10.1103/PhysRevC.29.64
Citations: PlumX Metrics


1981FE05      Nucl.Phys. A369, 425 (1981)

M.Fernandez, G.Murillo, J.Ramirez, O.Avila, S.E.Darden, M.C.Rozak, J.L.Foster, B.P.Hichwa, P.L.Jolivette

20Ne(p(pol), p0)20Ne and States of 21Na

NUCLEAR REACTIONS 20Ne(polarized p, p), (polarized p, p'), E=3.7-7.9 MeV; measured σ(E, θ), P(E, θ). 21Na deduced resonances, J, π, Γ, Γp. Enriched target.

doi: 10.1016/0375-9474(81)90029-4
Citations: PlumX Metrics


1979DA11      Phys.Rev. C19, 2396 (1979)

S.E.Darden, J.L.Foster

Spin of the 14.174 MeV T = 3/2 Level in 17F

NUCLEAR REACTIONS 16O(polarized p, p), E=14.4-14.50 MeV; measured σ(θ), P(θ). 17F resonance deduced J, π, Γ, Γp.

doi: 10.1103/PhysRevC.19.2396
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1978FO07      Phys.Rev. C17, 1602 (1978)

J.L.Foster, Jr., F.Krmpotic, T.V.Ragland

Analysis of 136Xe(p, p1) on Analog Resonances and the Structure of 137Xe

NUCLEAR REACTIONS 136Xe(p, p'), E=10.26-11.82 MeV; analyzed σ(E, θ). 137Cs IAR deduced Γ, parentage coefficients. 137Xe calculated neutron parentage, levels.

doi: 10.1103/PhysRevC.17.1602
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1974BI01      Phys.Rev. C9, 741 (1974)

L.Bimbot, L.Lessard, S.Santhanam, R.Martin, O.Dietzsch, D.Spalding, K.Schechet, J.L.Foster, Jr.

142Nd(p, p') Reaction on Analog Resonances

NUCLEAR REACTIONS 142Nd(p, p'), E=9.5-11 MeV on analog resonances; measured σ(θ). 142Nd deduced levels, J, π, S. Enriched targets, Breit-Wigner analysis, resolution 5-15 keV, θ=20-170°.

doi: 10.1103/PhysRevC.9.741
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1973FO13      Phys.Rev.Lett. 31, 731 (1973)

J.L.Foster, Jr., O.Dietzsch, L.Bimbot

Comparison of Reactions 142Nd(p, p') and 143Nd(d, t) Leading to Neutron Particle-Hole States in 142Nd

NUCLEAR REACTIONS 142Nd(p, p'), 143Nd(d, t), E=9.505 MeV; measured σ(Ep', θ), σ(Et, θ). 142Nd deduced levels, J, π, S.

doi: 10.1103/PhysRevLett.31.731
Citations: PlumX Metrics


1973GA01      Nucl.Phys. A202, 535 (1973)

S.Gales, L.Lessard, J.L.Foster, Jr.

The 144Nd(d, p) and 144Nd(d, t) Reactions and Isobaric Analog Resonances In 144Nd(p, p0) and 144Nd(p, p')

NUCLEAR REACTIONS 144Nd(d, p), (d, t), Ed=12.6 MeV; measured Q, σ(E, θ). 145Nd, 143Nd deduced levels, (J), π, L. 144Nd(p, p0), 144Nd(p, p'), Ep=9.3-12 MeV; measured σ(E). 145Pm deduced isobaric analog resonances level-width, J, π.

doi: 10.1016/0375-9474(73)90641-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2510.


1973MA31      Nucl.Phys. A210, 221 (1973)

R.Martin, L.Bimbot, S.Gales, L.Lessard, D.Spalding, W.G.Weitkamp, O.Dietzsch, J.L.Foster, Jr.

The 144Sm(p, p') Reaction on Analog Resonances

NUCLEAR REACTIONS 144Sm(p, p'), E=9.3-11 MeV; measured σ(E, θ). 144Sm deduced levels, J, π, S.

doi: 10.1016/0375-9474(73)90299-6
Citations: PlumX Metrics


1973RA01      Nucl.Phys. A201, 21 (1973)

S.Raman, J.L.Foster, Jr., O.Dietzsch, D.Spalding, L.Bimbot, B.H.Wildenthal

Energy Levels in 142Nd

RADIOACTIVITY 142Pm; measured T1/2, Eγ, Iγ. 142Nd deduced levels, J, π, γ-branching.

NUCLEAR REACTIONS 142Nd(p, p') at analog resonances, E=9.505, 10.245, 10.805, 11.070 MeV; measured σ(Ep, θ). 142Nd deduced levels, J, π, particle-hole states.

doi: 10.1016/0375-9474(73)90685-4
Citations: PlumX Metrics


1972LE17      Phys.Rev. C6, 517 (1972)

L.Lessard, S.Gales, J.L.Foster, Jr.

142Ce(d, p) and 142Ce(d, t) Reactions and Isobaric Analog Resonances in 142Ce(p, p0) and 142Ce(p, p1)

NUCLEAR REACTIONS 142Ce(d, p), (d, t), E=12.6 MeV; measured Q, σ(θ). 142Ce(p, p), (p, p'), E=9.5-12 MeV; measured σ(E). 143Ce deduced levels, J, π, L(n), S. 143Pr deduced isobaric analog resonance, level-width, J, π. 143Ce, 143Pr deduced Coulomb displacement energy.

doi: 10.1103/PhysRevC.6.517
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2611.


1971FO10      Nucl.Phys. A169, 187 (1971)

J.L.Foster, Jr., O.Dietzsch, D.Spalding

The 142Nd(d, t)141Nd Reaction

NUCLEAR REACTIONS 142Nd(d, t), Ed=17 MeV; measured σ(Et, θ). 141Nd deduced levels, (J), π, L, S. Enriched target.

doi: 10.1016/0375-9474(71)90571-9
Citations: PlumX Metrics


1970MO11      Phys.Rev. C1, 1100 (1970)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Isobaric Analog Resonances in Proton Inelastic Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p'), E=9.77-12.89 MeV; measured σ(E;Ep', θ). 137Cs deduced isobaric analog resonances, level-width, S. 136Xe deduced levels, J, π, configurations.

doi: 10.1103/PhysRevC.1.1100
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1969MO02      Phys.Rev.Letters 22, 356(1969)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Neutron Particle-Hole States Observed by Inelastic Proton Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p'), E=9.8-13.0 MeV; measured σ(E; Ep', θ). 137Cs deduced resonances, S, isobaric analog. 136Xe deduced levels J, π.

doi: 10.1103/PhysRevLett.22.356
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1969MO14      Phys.Rev. 180, 1213 (1969)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

Isobaric Analog Resonances in Proton Elastic Scattering from 136Xe

NUCLEAR REACTIONS 136Xe(p, p), E=9.77-12.98 MeV; measured σ(E;Ep). 137Cs deduced resonances, level-width, L(p), S. Deduced 137Cs-137Xe Coulomb energy difference. Enriched target.

doi: 10.1103/PhysRev.180.1213
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1968FO08      Phys.Rev. 175, 1498 (1968)

J.L.Foster, Jr., P.J.Riley, C.F.Moore

Isobaric Analog Resonances in Proton Scattering from 124Te, 126Te, 128Te, and 130Te

NUCLEAR STRUCTURE 129I, 131I, 125I, 127I; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1498
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2691.


1968MO21      Phys.Rev. 175, 1516 (1968)

P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.

136Xe(d, p) and 136Xe(d, t) Reactions

NUCLEAR STRUCTURE 135Xe, 137Xe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1516
Citations: PlumX Metrics


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