NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = J.L.Foster Found 18 matches. 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
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
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
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
1979DA11 Phys.Rev. C19, 2396 (1979) 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
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
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
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
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
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
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
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
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
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
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
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
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
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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