NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = P.L.Kerr Found 19 matches. 1999LE32 Phys.Rev. C60, 024317 (1999) C.Lee, J.A.Liendo, P.D.Cathers, N.R.Fletcher, K.W.Kemper, P.L.Kerr Three-Particle Cluster Structure above Ex =11 MeV in 15N NUCLEAR REACTIONS 12C(7Li, α), E=52.5 MeV; measured σ(θ). 12C(polarized 6Li, 3He), E=50 MeV; measured σ(θ), iT11. 15N deduced J, π, spectroscopic factors.
doi: 10.1103/PhysRevC.60.024317
1997KE04 Phys.Rev. C55, 2441 (1997) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, B.G.Schmidt Analyzing Powers for Mirror States in 12C(6Li, 7Li/7Be) at E(6Li) = 50 MeV: Evaluation of channel coupling NUCLEAR REACTIONS 12C(polarized 6Li, 7Li), (polarized 6Li, 7Be), E=50 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced optical model, double folding, coupling strength parameters, spectroscopic amplitudes. Finite-range DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.55.2441
1997RU06 Phys.Rev. C56, 1895 (1997); Erratum Phys.Rev. C58, 1353 (1998) K.Rusek, P.V.Green, P.L.Kerr, K.W.Kemper Continuum-Discretized Coupled-Channels Analysis of 6Li(pol)4He Scattering at E(c.m.) = 11.1 MeV NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), (polarized 6Li, dα), E=27.8 MeV; measured σ(θ), scalar, vector analyzing powers vs θ; deduced reaction mechanism related features. Continuum-discretized coupled-channels method.
doi: 10.1103/PhysRevC.56.1895
1996GA29 Phys.Rev. C54, 3273 (1996) D.L.Gay, E.E.Bartosz, P.D.Cathers, D.D.Caussyn, T.L.Drummer, K.W.Kemper, P.L.Kerr, D.Robson Compound-Nucleus Contributions to 6Li + 12C Scattering NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30 MeV; measured σ(θ), recoil 12C spectra, vector analyzing powers; deduced compound nucleus formation related features. Coupled-channels approach.
doi: 10.1103/PhysRevC.54.3273
1996GR08 Phys.Rev. C53, 2862 (1996) P.V.Green, K.V.Kemper, P.L.Kerr, K.Mohajeri, E.G.Myers, D.Robson, K.Rusek, I.J.Thompson Analyzing Powers in 4He(6Li(pol), 6Li)4He NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E ≤ 27.8 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. Optical model with, without α exchange process.
doi: 10.1103/PhysRevC.53.2862
1996KE09 Phys.Rev. C54, 1267 (1996) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, B.G.Schmidt, V.Hnizdo 6Li(pol) + 12C Inelastic Scattering at 30 and 50 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30, 50 MeV; measured iT11(θ), T20(θ), T21(θ), T22(θ), σ(θ). 6Li(12C, 12C), E=100 MeV; measured σ(θ); deduced optical model parameters. 6Li, 12C levels deduced deformation length parameters. Coupled channels method.
doi: 10.1103/PhysRevC.54.1267
1995JE03 Phys.Rev. C52, 1295 (1995) J.K.Jewell, O.J.Tekyi-Mensah, P.D.Cottle, J.Doring, P.V.Green, J.W.Holcomb, G.D.Johns, T.D.Johnson, K.W.Kemper, P.L.Kerr, S.L.Tabor, P.C.Womble, V.A.Wood Negative-Parity States Near the Yrast Line in 144Nd NUCLEAR REACTIONS 130Te(18O, 4n), E=85 MeV; measured Eγ, Iγ, DCO ratios. 144Nd deduced levels, J, π, configurations. Hyperpure detectors.
doi: 10.1103/PhysRevC.52.1295
1995KE10 Phys.Rev. C52, 1924 (1995) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, D.Robson, B.G.Schmidt Tensor Effects in 6Li(pol) + 12C Scattering NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=30, 50 MeV; 4He(polarized 6Li, α), E=50 MeV; measured σ(θ), complete set of analyzing powers; deduced optical model parameters.
doi: 10.1103/PhysRevC.52.1924
1995ME02 Phys.Rev. C51, 651 (1995) A.J.Mendez, K.W.Kemper, P.V.Green, P.L.Kerr, E.G.Myers, E.L.Reber, D.Robson Analyzing Powers for the 12C(6Li(pol), α)14N(*) Reaction at 33 MeV NUCLEAR REACTIONS 12C(polarized 6Li, α), E=33 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 14N levels deduced configurations, spectroscopic amplitudes. DWBA, finite-range deuteron cluster factor.
doi: 10.1103/PhysRevC.51.651
1994JE03 Z.Phys. A348, 69 (1994) J.K.Jewell, O.J.Tekyi-Mensah, P.D.Cottle, J.Doring, P.V.Green, J.W.Holcomb, G.D.Johns, J.L.Johnson, T.D.Johnson, K.W.Kemper, P.L.Kerr, S.L.Tabor, P.C.Womble, V.A.Wood Possible π(h311/2g-17/2) States in 144Nd NUCLEAR REACTIONS 130Te(18O, 4n), E=85 MeV; measured γγ-coin, Iγ(θ), DCO ratios. 144Nd deduced high-spin levels, J, π, configuration.
doi: 10.1007/BF01291659
1994KE02 Phys.Lett. 321B, 183 (1994) K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, E.L.Reber, K.Rusek, G.Tungate J Dependence in 12C(6Li(pol), 3He) NUCLEAR REACTIONS 12C(polarized 6Li, 3He), E=34 MeV; measured σ(θ), σ(E(3He)), iT11(θ); deduced model parameters. 15N level deduced possible J, π. Coupled-channels Born approximation, cluster transfer.
doi: 10.1016/0370-2693(94)90461-8
1994ME04 Nucl.Phys. A567, 655 (1994) A.J.Mendez, P.V.Green, K.W.Kemper, P.L.Kerr, E.G.Myers, E.L.Reber, B.G.Schmidt An Absolute Standard for 6Li Vector Analyzing Powers NUCLEAR REACTIONS 12C(polarized 6Li, d), E=33 MeV; measured σ(θ), Eα, tensor analyzing power vs θ; deduced 6Li vector analyzing power absolute standard.
doi: 10.1016/0375-9474(94)90030-2
1994RE01 Phys.Rev. C49, R1 (1994) E.L.Reber, K.W.Kemper, P.V.Green, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt Spin-Orbit and Tensor Potentials from Polarized 6Li Scattering NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=30 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced model parameters, tensor potential need.
doi: 10.1103/PhysRevC.49.R1
1994RE15 Phys.Rev. C50, 2917 (1994) E.L.Reber, K.W.Kemper, P.V.Green, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 12C at 30 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 6Li, 12C levels deduced deformation lengths. Coupled-channels analysis.
doi: 10.1103/PhysRevC.50.2917
1994TE05 Phys.Rev. C50, R1759 (1994) O.J.Tekyi-Mensah, P.D.Cottle, J.Doring, P.V.Green, J.W.Holcomb, G.D.Johns, J.L.Johnson, T.D.Johnson, K.W.Kemper, P.L.Kerr, S.L.Tabor, P.C.Womble, V.A.Wood Weak Coupling in 143Nd NUCLEAR REACTIONS 130Te(18O, 5n), E=85 MeV; measured γγ-coin, DCO ratios. 143Nd deduced high-spin levels, J, π. Weak coupling model.
doi: 10.1103/PhysRevC.50.R1759
1993ME11 Nucl.Instrum.Methods Phys.Res. A329, 37 (1993) A.J.Mendez, E.G.Myers, K.W.Kemper, P.L.Kerr, E.L.Reber, B.G.Schmidt Determination of the On-Target Polarization of an Optically-Pumped Polarized Lithium Ion Beam NUCLEAR REACTIONS 12C(polarized 6Li, α), E=33 MeV; measured σ(Eα), on-target t20(θ) for beam. Optically pumped polarized lithium ion source.
doi: 10.1016/0168-9002(93)90920-D
1993MY01 Nucl.Instrum.Methods Phys.Res. A334, 271 (1993) E.G.Myers, A.J.Mendez, K.W.Kemper, P.L.Kerr, E.L.Reber, B.G.Schmidt Transport of Polarized Ions Through a Tandem-Superconducting-Linac Heavy-Ion Accelerator NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=20 MeV; measured on target beam polarization variation; deduced beam polarization loss mechanisms.
doi: 10.1016/0168-9002(93)90784-F
1993RE04 Phys.Rev. C47, 2190 (1993) E.L.Reber, K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, N.M.Clarke Analyzing Powers for 9Be(6Li(pol), 6He)9B NUCLEAR REACTIONS 9Be(polarized 6Li, 6He), E=32 MeV; measured σ(θ), vector, tensor analyzing powers vs θ. 9B levels deduced spectroscopic amplitudes. Shell model.
doi: 10.1103/PhysRevC.47.2190
1993RE08 Phys.Rev. C48, 285 (1993) E.L.Reber, K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 9Be at 32 MeV NUCLEAR REACTIONS 9Be(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=32 MeV; measured vector, tensor analyzing power vs θ; deduced optical potential constraints, parameters. Coupled-channels calculations.
doi: 10.1103/PhysRevC.48.285
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