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NSR database version of April 26, 2024.

Search: Author = J.L.Foster

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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
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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
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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
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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
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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
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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
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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 T_1/2, 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
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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
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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
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