NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.Ray Found 99 matches. 2011RA04 Nucl.Phys. A854, 89 (2011) L.Ray, for the STAR Collaboration The ridge(s) in STAR
doi: 10.1016/j.nuclphysa.2011.01.002
2000KU08 Prog.Theor.Phys.(Kyoto) 103, 321 (2000) L.Kurth Kerr, B.C.Clark, S.Hama, L.Ray, G.W.Hoffmann Theoretical and Experimental K+ + Nucleus Total and Reaction Cross Sections from the KDP-RIA Model NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, X), E at 450-750 MeV/c; calculated total, reaction σ. 12C(K+, K+), E at 715 MeV/c; calculated σ(θ). Kemmer-Duffin-Petiau equation, relativistic impulse approximation. Comparisons with data.
1997KA22 Phys.Rev. C55, 2533 (1997) G.Kahrimanis, G.Burleson, C.M.Chen, B.C.Clark, K.Dhuga, D.J.Ernst, J.A.Faucett, H.T.Fortune, S.Hama, A.Hussein, M.F.Jiang, K.W.Johnson, L.Kurth Kerr, S.Mathews, J.McGill, C.F.Moore, S.Mordechai, C.L.Morris, J.O'Donnell, M.Snell, M.Rawool-Sullivan, L.Ray, C.Whitley, A.L.Williams Pion-Nucleus Elastic Scattering on 12C, 40Ca, 90Zr, and 208Pb at 400 and 500 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(π+, π+), (π-, π-), E=400, 500 MeV; 90Zr(π+, π+), E=400, 500 MeV; 90Zr(π-, π-), E=400 MeV; measured σ(θ). 208Pb(π+, π+), (π-, π-), E=662.7 MeV; 40Ca(π+, π+), (π-, π-), 12C(π+, π+), E=672.5 MeV; 12C(π-, π-), E=672.5, 486.2 MeV; analyzed σ(θ). Impulse approximation approach.
doi: 10.1103/PhysRevC.55.2533
1996HO08 Phys.Rev. C53, 1974 (1996) G.W.Hoffmann, L.Ray, D.Read, S.Worm, M.L.Barlett, A.A.Green, B.Storm, B.C.Clark, S.Hama, R.L.Mercer Measurement of the Polarization Transfer Parameter D(NN) for 12,13C(p(pol), p(pol)) at 500 MeV NUCLEAR REACTIONS 12,13C(polarized p, p), E=500 MeV; measured polarization transfer parameter D(NN). Non-relativistic DWBA analysis, coupled-channels Dirac, relativistic DWBA analyses.
doi: 10.1103/PhysRevC.53.1974
1996OR02 Phys.Rev. C53, 2086 (1996) Two-Nucleon Potential from Chiral Lagrangians NUCLEAR STRUCTURE 2H; calculated binding energy, μ, electric quadrupole moment, D-state probability, asymptotic D/S ratio. Effective chiral Lagrangian based NN-potential. NUCLEAR REACTIONS 1H(p, p), E ≤ 300 MeV; 1H(n, n), E ≤ 100 MeV; calculated phase shifts, mixing angle vs E. Effective chiral Lagrangian based NN-potential.
doi: 10.1103/PhysRevC.53.2086
1996RA43 Phys.Rev. C54, 2582 (1996) Simulated Bose-Einstein Correlations in Multiplicity Distributions from Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E at 100 GeV/c/nucleon; calculated identical bosons production associated one-, two-body Bose-Einstein correlation functions; deduced three-body correlations quality, relativistic collisions.
doi: 10.1103/PhysRevC.54.2582
1995BR18 Phys.Rev. C52, 807 (1995) E.J.Brash, O.Hausser, W.J.Cummings, M.Bahrami, P.P.J.Delheij, R.S.Henderson, M.C.Vetterli, D.M.Whittal, B.Larson, R.H.Landau, T.Mefford, L.Ray Spin Observables in Elastic Proton Scattering from Polarized 3He NUCLEAR REACTIONS 3He(polarized p, p), E=200, 500 MeV; measured σ(θ), spin observables vs θ; deduced reaction models test related features. Fully microscopic nonrelativistic optical model. Polarized target.
doi: 10.1103/PhysRevC.52.807
1995HA09 Phys.Lett. 343B, 36 (1995) O.Hausser, B.Larson, W.P.Alford, C.Chan, P.P.J.Delheij, R.S.Henderson, K.P.Jackson, R.H.Landau, T.Mefford, C.A.Miller, A.Rahav, L.Ray, A.Trudel, M.C.Vetterli Elastic Scattering of Polarized Protons from Polarized 3He NUCLEAR REACTIONS 3He(polarized p, p), E=200-500 MeV; measured spin correlation parameters, target related asymmetries. Polarized 3He gas target. Nonrelativistic optical, DWIA models.
doi: 10.1016/0370-2693(94)01434-E
1995KU11 Nucl.Phys. A585, 335c (1995) L.J.Kurth, B.C.Clark, E.D.Cooper, S.Hama, R.L.Mercer, L.Ray, G.W.Hoffmann Meson-Nucleus Scattering in the KDP Formalism NUCLEAR REACTIONS 12C(K+, K+), E at 800, 715 MeV/c; calculated σ(θ). Kemmer-Duffin-Petiau equation, relativistic impulse approximation.
doi: 10.1016/0375-9474(94)00594-D
1994HO01 Phys.Rev. C49, 630 (1994) G.W.Hoffmann, M.L.Barlett, W.Kielhorn, G.Pauletta, M.Purcell, L.Ray, J.F.Amann, J.J.Jarmer, K.W.Jones, S.Penttila, N.Tanaka, G.Burleson, J.Faucett, M.Gilaini, G.Kyle, L.Stevens, A.M.Mack, D.Mihailidis, T.Averett, J.Comfort, J.Gorgen, J.Tinsley Spin Correlation Measurements for p(pol) + p(pol) Elastic Scattering at 497.5 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=497.5 MeV; measured spin correlation parameter A(00NN); deduced nucleon-nucleon spin-dependent amplitudes constraints. Polarized target.
doi: 10.1103/PhysRevC.49.630
1994KU05 Phys.Rev. C49, 2086 (1994) L.Kurth, B.C.Clark, E.D.Cooper, S.Hama, S.Shim, R.L.Mercer, L.Ray, G.W.Hoffmann Dirac Coupled Channel Calculations for Proton Inelastic Scattering from Spherically Symmetric Nuclei for Projectile Energies of 362, 500, and 800 MeV NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(polarized p, p'), (polarized p, p), E=362, 500, 800 MeV; analyzed σ(θ), analyzing power, other polarization data; deduced model parameters. 40Ca, 90Zr, 208Pb levels deduced deformation lengths, parameters. Phenomenological, relativistic impulse approximation optical potentials.
doi: 10.1103/PhysRevC.49.2086
1994KU23 Phys.Rev. C50, 2624 (1994) L.J.Kurth, B.C.Clark, E.D.Cooper, S.Hama, R.L.Mercer, L.Ray, G.W.Hoffmann Relativistic Impulse Approximation Treatment of the Elastic Scattering of 400 MeV π± on 28Si NUCLEAR REACTIONS 28Si(π+, π+), (π-, π-), E=400 MeV; calculated σ(θ). Relativistic impulse approximation, Kemmer-Duffin-Petiau formalism.
doi: 10.1103/PhysRevC.50.2624
1994OR05 Phys.Rev.Lett. 72, 1982 (1994) Nucleon-Nucleon Potential from an Effective Chiral Lagrangian NUCLEAR REACTIONS 1H, 1n(p, p), E=100 MeV; calculated phase shifts vs E. Potential based on effective chiral Lagrangian.
doi: 10.1103/PhysRevLett.72.1982
1994RA08 Phys.Rev. C49, 2109 (1994) Phenomenological Transition Amplitudes for NN → NΔ at 800 MeV NUCLEAR REACTIONS 1H(polarized p, X), E=800 MeV; analyzed inclusive inelastic scattering data; deduced tensor amplitudes role in NN → NΔ observables.
doi: 10.1103/PhysRevC.49.2109
1993RA05 Phys.Rev. C47, 2990 (1993) Predictions for p(pol) + 13C(pol) Elastic Scattering Based on the Relativistic Impulse Approximation Effective Interaction NUCLEAR REACTIONS 13C(polarized p, p), E=500 MeV; calculated σ(θ), analyzing power, polarization transfer observables vs θ. Relativistic impulse approximation, density dependent nucleon-nucleon effective interaction.
doi: 10.1103/PhysRevC.47.2990
1992RA02 Phys.Rev. C45, 1394 (1992) Nuclear Structure and Medium Effects in p(pol) + 13C(pol) Elastic Scattering NUCLEAR REACTIONS 13C(polarized p, p), E=497.5 MeV; calculated polarization observables. Polarized target, shell model configurations. Pauli blocking.
doi: 10.1103/PhysRevC.45.1394
1991BA45 Phys.Lett. 264B, 21 (1991) M.L.Barlett, R.W.Fergerson, G.W.Hoffmann, J.A.Marshall, L.Ray, J.F.Amann, B.E.Bonner, J.B.McClelland Inclusive Quasielastic Spin Observables for p(pol) + 2H, 12C at 500 MeV NUCLEAR REACTIONS 2H, 12C(polarized p, p), E=500 MeV; measured analyzing power, spin rotation depolarization parameters. Relativistic plane wave impulse approximation calculation.
doi: 10.1016/0370-2693(91)90696-N
1991MI01 Phys.Rev. C43, 801 (1991) V.K.Mishra, S.Hama, B.C.Clark, R.E.Kozack, R.L.Mercer, L.Ray Implications of Various Spin-One Relativistic Wave Equations for Intermediate-Energy Deuteron-Nucleus Scattering NUCLEAR REACTIONS 58Ni(polarized d, d), E=400 MeV; 40Ca(polarized d, d), E=700 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Various spin-one relativistic equations.
doi: 10.1103/PhysRevC.43.801
1990CO19 Phys.Rev. C42, 659 (1990) 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
1990CO27 Phys.Rev. C42, 2242 (1990) 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
1990HO06 Phys.Rev. C41, 1651 (1990) G.W.Hoffmann, M.L.Barlett, D.Ciskowski, G.Pauletta, M.Purcell, L.Ray, J.F.Amann, J.J.Jarmer, K.W.Jones, S.Pentilla, N.Tanaka, M.M.Gazzaly, J.R.Comfort, B.C.Clark, S.Hama Cross Sections, Analyzing Powers, and Spin-Rotation-Depolarization Observables for 500 MeV Proton Elastic Scattering from 12C and 13C NUCLEAR REACTIONS 12,13C(polarized p, p), E=494 MeV; measured σ(θ), analyzing powers, spin rotation depolarization observables; deduced phenomenological Dirac optical potentials. Calculated retativistic impulse approximation optical potentials, observables.
doi: 10.1103/PhysRevC.41.1651
1990HO22 Phys.Rev.Lett. 65, 3096 (1990) G.W.Hoffmann, M.L.Barlett, W.Kielhorn, G.Pauletta, M.Purcell, L.Ray, J.F.Amann, J.J.Jarmer, K.W.Jones, S.Penttila, N.Tanaka, G.Burleson, J.Faucett, M.Gilaini, G.Kyle, L.Stevens, A.M.Mack, D.Mihailidis, T.Averett, J.Comfort, J.Gorgen, J.Tinsley, B.C.Clark, S.Hama, R.L.Mercer Polarized-Proton Elastic Scattering from Polarized 13C NUCLEAR REACTIONS 13C(polarized p, p), E=497.5 MeV; measured spin correlation parameter, target analyzing power vs θ. Dynamic nuclear polarization technique, polarized, cooled target, enriched ethylene glycol target.
doi: 10.1103/PhysRevLett.65.3096
1990MO04 Phys.Rev. C41, 1279 (1990) M.G.Moshi, C.A.Whitten, Jr., B.Aas, G.Igo, D.Lopiano, L.Ray, K.Jones, M.Gazzaly Analyzing Powers for p(pol) + 208Pb at Large Momentum Transfers NUCLEAR REACTIONS 208Pb(polarized p, p'), E=800 MeV; measured σ(Ep'), analyzing power vs θ. Relativistic, nonrelativistic impulse approximation calculations.
doi: 10.1103/PhysRevC.41.1279
1990RA12 Phys.Rev. C41, 2816 (1990) Effective Interactions for Nucleon-Nucleus Scattering Above 300 MeV NUCLEAR REACTIONS 208Pb, 16O(polarized p, p), E ≈ 300-800 MeV; 40Ca(polarized p, p), E=300-500 MeV; analyzed σ(θ), analyzing power vs θ, polarization observables. Nonrelativistic coupled-channels isobar model, effective interactions.
doi: 10.1103/PhysRevC.41.2816
1990SH26 Phys.Rev. C42, 1592 (1990) S.Shim, B.C.Clark, E.D.Cooper, S.Hama, R.L.Mercer, L.Ray, J.Raynal, H.S.Sherif Comparison of Relativistic and Nonrelativistic Approaches to the Collective Model Treatment of p + 40Ca Inelastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=497.5 MeV; calculated σ(θ), analyzing power, spin rotation function vs θ. Dirac, Schrodinger coupled-channels formalisms.
doi: 10.1103/PhysRevC.42.1592
1989BA62 Phys.Rev. C40, 2697 (1989) M.L.Barlett, G.W.Hoffmann, L.Ray, G.Pauletta, K.H.McNaughton, J.F.Amann, K.W.Jones, J.B.McClelland, M.W.McNaughton, R.Fergerson, D.Lopiano Inclusive and Exclusive Quasielastic p(pol) + 2H Spin Observables at 647 and 800 MeV NUCLEAR REACTIONS 2H(polarized p, p), (polarized p, n), E=647, 800 MeV; measured inclusive, exclusive quasielastic analyzing powers, spin-rotation depolarization observables; deduced free proton-neutron spin-rotation depolarization observables. Liquid deuterium target.
doi: 10.1103/PhysRevC.40.2697
1989KO34 Phys.Rev. C40, 2181 (1989) R.E.Kozack, B.C.Clark, S.Hama, V.K.Mishra, R.L.Mercer, L.Ray Spin-One Kemmer-Duffin-Petiau Equations and Intermediate-Energy Deuteron-Nucleus Scattering NUCLEAR REACTIONS 58Ni(polarized d, d), E=400 MeV; 40Ca(polarized d, d), E=700 MeV; calculated σ(θ), analyzing power vs θ. Phenomenological, microscopic nucleon-nucleus potentials, spin-one Kemmer-Duffin-Petiau equations.
doi: 10.1103/PhysRevC.40.2181
1989RA02 Phys.Rev. C39, 1170 (1989) Antisymmetrization Correction for Nucleon-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O(p, p), E=20.8-49.5 MeV; 40Ca(p, p), E=9.86-76 MeV; calculated potential volumes; deduced three-body antisymmetrization correction.
doi: 10.1103/PhysRevC.39.1170
1989RA15 Phys.Rev. C40, 237 (1989) Spin-Flip Cross Sections for 13C(p(pol), n(pol))13N(g.s.) at 500 MeV NUCLEAR REACTIONS 13C(polarized p, n), E=500 MeV; calculated σ(θ), polarization, polarization transfer coefficient vs θ. Relativistic DWIA.
doi: 10.1103/PhysRevC.40.237
1988HO01 Phys.Rev. C37, 397 (1988) G.W.Hoffmann, M.L.Barlett, R.W.Fergerson, J.A.Marshall, J.A.McGill, E.C.Milner, L.Ray, J.F.Amann Differential Cross Section and Analyzing Power Measurements for p + p Elastic Scattering at 497.5 MeV NUCLEAR REACTIONS 1H(polarized p, p), (p, p), E ≈ 497.5 MeV; measured σ(θ), analyzing power for (θ(cm)=16°-97°). Phase shift analysis.
doi: 10.1103/PhysRevC.37.397
1988HO05 Phys.Rev. C37, 1307 (1988) G.W.Hoffmann, M.L.Barlett, G.Pauletta, L.Ray, J.F.Amann, K.Jones, J.B.McClelland, R.W.Fergerson, M.M.Gazzaly, B.C.Clark, R.L.Mercer Large Angle p(pol) + 40Ca Elastic Scattering at 497.5 MeV NUCLEAR REACTIONS 40Ca(polarized p, p), E=497.5 MeV; measured σ(θ), analyzing power. Relativistic, nonrelativistic scattering models.
doi: 10.1103/PhysRevC.37.1307
1988KO12 Phys.Rev. C37, 2898 (1988) R.E.Kozack, B.C.Clark, S.Hama, V.K.Mishra, G.Kalbermann, R.L.Mercer, L.Ray Relativistic Deuteron-Nucleus Scattering in the Kemmer-Duffin-Petiau Formalism NUCLEAR REACTIONS 58Ni(d, d), (polarized d, d), E=400 MeV; measured σ(θ), analyzing power vs θ. Kemmer-Duffin-Petiau equations.
doi: 10.1103/PhysRevC.37.2898
1988RA02 Phys.Rev. C37, 224 (1988) L.Ray, G.W.Hoffmann, M.L.Barlett, N.Ottenstein Relativistic Effects in Forward Angle Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O, 40Ca, 208Pb(p, p), E=500, 800 MeV; calculated σ(θ). Relativistic, nonrelativistic scattering models comparison.
doi: 10.1103/PhysRevC.37.224
1988RA08 Phys.Rev. C37, 1169 (1988); Erratum Phys.Rev. C39, 2089 (1989) L.Ray, G.W.Hoffmann, M.L.Barlett, J.D.Lumpe, B.C.Clark, S.Hama, R.L.Mercer Relativistic Impulse Approximation Description of Polarized Proton Elastic Scattering from Polarized 13C NUCLEAR REACTIONS 13C(polarized p, p), E=500 MeV; calculated σ(θ), P(θ), spin observables; deduced target nucleus relativistic effects role. Relativistic dynamics, pseudovector coupling.
doi: 10.1103/PhysRevC.37.1169
1988RA34 Phys.Rev. C38, 2743 (1988) Multiple Scattering Description of Intermediate Energy Deuteron-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca, 58Ni(polarized d, d), E=700 MeV; calculated σ(θ), vector, tensor analyzing powers. Nonrelativistic multiple scattering theory, corrections to Watanabe folding model.
doi: 10.1103/PhysRevC.38.2743
1988SH32 Phys.Rev. C38, 1968 (1988) S.Shim, B.C.Clark, S.Hama, E.D.Cooper, R.L.Mercer, L.Ray, G.W.Hoffmann Dirac Coupled Channels Calculation for p + 40Ca Inelastic Scattering using the Relativistic Impulse Approximation NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=497.5 MeV; calculated σ(θ), analyzing power vs θ. 40Ca levels deduced deformation lengths. Relativistic impulse approximation.
doi: 10.1103/PhysRevC.38.1968
1987BA22 Phys.Rev. C35, 2185 (1987) M.L.Barlett, G.W.Hoffmann, L.Ray Effective Interaction Analysis of 500 MeV (p(pol), p') Excitation of Low-Lying States in 40,48Ca, 90Zr, and 208Pb NUCLEAR REACTIONS 90Zr, 208Pb(polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ. 40,48Ca(polarized p, p'), E=500 MeV; analyzed data. 40,48Ca, 90Zr, 208Pb levels deduced neutron transition densities, neutron, proton multipole moment ratios. DWBA analysis.
doi: 10.1103/PhysRevC.35.2185
1987LU02 Phys.Rev. C35, 1040 (1987) Correlation Effects in the Relativistic Impulse Approximation Treatment of Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O, 40Ca, 208Pb(polarized p, p), E=500, 800 MeV; calculated σ(θ), analyzing power, spin rotation function vs θ. Relativistic impulse approximation, two-body correlations.
doi: 10.1103/PhysRevC.35.1040
1987LU04 Phys.Lett. 186B, 263 (1987) Virtual N(N-Bar) Pair Processes as a Relativistic Correction to Second-Order Multiple Scattering Theory NUCLEAR REACTIONS 16O, 40Ca, 208Pb(polarized p, p), E=800 MeV; calculated spin rotation parameter, analyzing power vs θ. Nonrelativistic, multiple scattering theory.
doi: 10.1016/0370-2693(87)90291-7
1987RA03 Phys.Rev. C35, 1072 (1987) Nucleon-Nucleon Scattering with Isobar Degrees of Freedom NUCLEAR REACTIONS 1n(p, p), 1H(n, n), E=0-1 GeV; calculated phase shifts; deduced short range phenomenological interactions. Isobar degrees of freedom.
doi: 10.1103/PhysRevC.35.1072
1986FE01 Phys.Rev. C33, 239 (1986) R.W.Fergerson, M.L.Barlett, G.W.Hoffmann, J.A.Marshall, E.C.Milner, G.Pauletta, L.Ray, J.F.Amann, K.W.Jones, J.B.McClelland, M.Gazzaly, G.J.Igo Spin-Rotation Parameter Q for 800 MeV Proton Elastic Scattering from 16O, 40Ca, and 208Pb NUCLEAR REACTIONS 16O, 40Ca, 208Pb(polarized p, p), E=800 MeV; measured spin rotation parameter vs θ. Relativistic, nonrelativistic microscopic optical model.
doi: 10.1103/PhysRevC.33.239
1986LU01 Phys.Rev. C33, 665 (1986) Model-Independent Error Analysis of K+-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca, 208Pb(K+, K+), E=442, 991 MeV; analyzed data. Model independent error analysis.
doi: 10.1103/PhysRevC.33.665
1986MA52 Phys.Rev. C34, 1433 (1986) J.A.Marshall, M.L.Barlett, R.W.Fergerson, G.W.Hoffmann, E.C.Milner, L.Ray, J.F.Amann, B.E.Bonner, J.B.McClelland Determination of Proton-Nucleon Analyzing Powers and Spin-Rotation-Depolarization Parameters at 500 MeV NUCLEAR REACTIONS 1,2H(polarized p, p), (polarized p, p'), E=500 MeV; measured analyzing powers, spin-rotation depolarization parameters vs θ. Liquid targets, plastic scintillators. Phase shift solutions.
doi: 10.1103/PhysRevC.34.1433
1986RA05 Phys.Rev.Lett. 56, 2465 (1986) L.Ray, G.W.Hoffmann, M.L.Barlett, J.J.Jarmer, B.C.Clark, R.E.Kozack, R.L.Mercer, G.R.Burleson, S.Hama Sensitivity of p(pol) + A(pol) Elastic Spin Observables to Relativistic Aspects of Nuclear Structure NUCLEAR REACTIONS 13C(polarized p, p), E=500 MeV; calculated σ(θ), polarization, other parameters vs θ; deduced relativistic effects role.
doi: 10.1103/PhysRevLett.56.2465
1985BA30 Phys.Rev. C32, 239 (1985) M.L.Barlett, G.W.Hoffmann, J.A.McGill, B.Hoistad, L.Ray, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland Proton-Nucleon Spin-Rotation and -Depolarization Parameters at 800 MeV NUCLEAR REACTIONS 1H, 1n(polarized p, p), E=800 MeV; measured spin polarization, depolarization parameters vs θ. Liquid deuterium target.
doi: 10.1103/PhysRevC.32.239
1985BA38 Phys.Lett. 158B, 289 (1985) M.L.Barlett, G.W.Hoffmann, L.Ray Nonrelativistic Distorted Wave Born Approximation Predictions for 500 MeV (p(pol), p(pol)') Spin-Rotation Observables NUCLEAR REACTIONS 40Ca, 208Pb(polarized p, p'), E=500 MeV; calculated spin rotation parameter vs θ; deduced phenomenological effective interaction role. Nonrelativistic DWBA.
doi: 10.1016/0370-2693(85)91185-2
1985CL03 Phys.Rev.Lett. 55, 592 (1985) B.C.Clark, S.Hama, G.R.Kalbermann, R.L.Mercer, L.Ray Relativistic Impulse Approximation for Meson-Nucleus Scattering in the Kemmer-Duffin-Petiau Formalism NUCLEAR REACTIONS 40Ca(K+, K+), (π+, π+), E at 800 MeV/c; calculated meson-nucleus potentials, σ(θ). Relativistic impulse approximation.
doi: 10.1103/PhysRevLett.55.592
1985CO07 Phys.Rev. C31, 1412 (1985) 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
1985RA02 Phys.Rev. C31, 538 (1985); Erratum Phys.Rev. C34, 2353 (1986) Relativistic and Nonrelativistic Impulse Approximation Descriptions of 300-1000 MeV Proton + Nucleus Elastic Scattering NUCLEAR REACTIONS 40,48Ca, 208Pb(p, p), (polarized p, p), E=0.3-1 GeV; calculated σ(θ), analyzing power, spin rotation parameters vs θ; deduced effective, isotopic neutron density differences, scalar densities. Relativistic, nonrelativistic impulse approximation.
doi: 10.1103/PhysRevC.31.538
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
1984CL05 Phys.Rev. C30, 314 (1984) B.C.Clark, S.Hama, E.Sugarbaker, M.A.Franey, R.L.Mercer, L.Ray, G.W.Hoffmann, B.D.Serot Relativistic Description of (p, n) Reactions to the Isobaric Analog State NUCLEAR REACTIONS 90Zr(polarized p, p), (polarized p, n), E=160, 500 MeV; calculated σ(θ), analyzing power vs θ, spin rotation function vs θ; deduced proton-nucleus optical potential parameters. Lane model, relativistic generalization.
doi: 10.1103/PhysRevC.30.314
1984CL11 Phys.Rev.Lett. 53, 1423 (1984) B.C.Clark, S.Hama, J.A.McNeil, R.L.Mercer, L.Ray, B.D.Serot, D.A.Sparrow, K.Stricker-Bauer Relative Impulse-Approximation Calculation of p(bar)-Nucleus Elastic Scattering NUCLEAR REACTIONS 12C(p-bar, p-bar), (polarized p-bar, p-bar), E=46.8 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Relativistic impulse approximation.
doi: 10.1103/PhysRevLett.53.1423
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
1984RA18 Phys.Rev. C30, 1593 (1984) Large Angle Proton + 208Pb Elastic Scattering at 800 MeV NUCLEAR REACTIONS 208Pb(p, p), E=800 MeV; calculated σ(θ); deduced channel coupling role. Relativistic, nonrelativistic impulse approximations.
doi: 10.1103/PhysRevC.30.1593
1983BA05 Phys.Rev. C27, 682 (1983) M.L.Barlett, G.W.Hoffmann, J.A.McGill, B.Hoistad, L.Ray, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland, G.S.Blanpied, R.A.Arndt Forward-Angle Elastic and Quasielastic Proton-Nucleon Cross Sections and Analyzing Powers at 0.8 GeV NUCLEAR REACTIONS 1H(p, p), (polarized p, p), E=800 MeV; measured σ(θ), analyzing power vs θ. 2H(polarized p, 2p), (polarized p, pn), E=800 MeV; measured analyzing power vs θ, quasielastic scattering; deduced proton nucleus amplitudes. Liquid hydrogen, deuterium, CH, CH2 targets. 40Ca(polarized p, p), E=800 MeV; analyzed σ(θ), analyzing power data; deduced medium correction effects. Kerman-McManus-Thaler formalism, amplitude input from present data.
doi: 10.1103/PhysRevC.27.682
1983CL04 Phys.Rev.Lett. 50, 1644 (1983) B.C.Clark, S.Hama, R.L.Mercer, L.Ray, B.D.Serot Dirac-Equation Impulse Approximation for Intermediate-Energy Nucleon-Nucleus Scattering NUCLEAR REACTIONS 40Ca, 208Pb(polarized p, p), E=497, 800 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.
doi: 10.1103/PhysRevLett.50.1644
1983CL05 Phys.Rev. C28, 1421 (1983) B.C.Clark, S.Hama, R.L.Mercer, L.Ray, G.W.Hoffmann, B.D.Serot Energy Dependence of the Relativistic Impulse Approximation for Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=181-1040 MeV; calculated σ(θ), analyzing power, spin rotation power vs θ. Relativistic, nonrelativistic impulse approximation.
doi: 10.1103/PhysRevC.28.1421
1983MC04 Phys.Rev. C27, 2123 (1983) J.A.McNeil, L.Ray, S.J.Wallace Impulse Approximation NN Amplitudes for Proton-Nucleus Interactions NUCLEAR REACTIONS 40Ca(p, p), E=800 MeV; calculated σ(θ). 40Ca(polarized p, p), E=500 MeV; calculated analyzing power vs θ. Impulse approximation, invariant nucleon-nucleon amplitudes.
doi: 10.1103/PhysRevC.27.2123
1983RA12 Phys.Rev. C27, 2133 (1983) 800 MeV Protons as Probes of Neutron Transition Densities NUCLEAR REACTIONS 208Pb(p, p'), E=800 MeV; analyzed σ(θ). 208Pb level deduced neutron transition density. DWBA analysis, first-order optical potential model. Multipole moment error analysis, sensitivity analysis.
doi: 10.1103/PhysRevC.27.2133
1983RA13 Phys.Rev. C27, 2143 (1983) Proton Isotonic Density Differences from 0.8 GeV Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 48Ca, 54Fe(polarized p, p), E=0.8 GeV; analyzed σ(θ), analyzing power vs θ. 54Fe, 48Ca deduced proton density differences. Local, spin-dependent second order Kerman-McManus-Thaler optical potential, isovector terms, medium effects, subshell corrections.
doi: 10.1103/PhysRevC.27.2143
1983RA16 Phys.Lett. 124B, 309 (1983) Deformation Correlation Effects in the 154Sm-144Sm Neutron Density Difference NUCLEAR REACTIONS 144,154Sm(p, p), E=800 MeV; analyzed σ(θ). 154,144Sm deduced neutron isotopic density, rms radius differences. Second-order Kerman-McManus-Thaler optical potential, deformation correlation effects.
doi: 10.1016/0370-2693(83)91460-0
1983RA20 Phys.Rev. C28, 506 (1983) Isovector Correction to the Kerman, McManus, and Thaler Formalism NUCLEAR REACTIONS 12C, 40,48Ca, 90Zr, 208Pb(p, p), E=150-1000 MeV; 12C, 40Ca, 208Pb(π, π), E=50, 180 MeV; calculated isovector corrections to optical potentials. Kerman-McManus-Thaler, Watson multiple scattering theories.
doi: 10.1103/PhysRevC.28.506
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1981BL07 Phys.Rev. C23, 2599 (1981) G.S.Blanpied, G.W.Hoffmann, M.L.Barlett, J.A.McGill, S.J.Greene, L.Ray, O.B.Van Dyck, J.Amann, H.A.Thiessen Large Angle Scattering of 0.8 GeV Protons from 12C NUCLEAR REACTIONS 12C(p, p'), E=800 MeV; measured σ(θ). 12C deduced charge density multipole moments M(E2), M(E4). Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.23.2599
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
1981HO26 Phys.Rev.Lett. 47, 1436 (1981) G.W.Hoffmann, L.Ray, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner, K.K.Seth, D.Barlow, M.Bosko, S.Iversen, M.Kaletka, A.Saha, D.Smith Elastic Scattering of 500-MeV Polarized Protons from 40,48Ca, 90Zr, and 208Pb, and Breakdown of the Impulse Approximation at Small Momentum Transfer NUCLEAR REACTIONS 40,48Ca, 90Zr, 208Pb(polarized p, p), E=500 MeV; measured σ(θ), A(θ); deduced impulse approximation breakdown. Second-order. Kerman-McManus-Thaler optical potential.
doi: 10.1103/PhysRevLett.47.1436
1981HU04 Phys.Rev.Lett. 47, 315 (1981) D.A.Hutcheon, J.M.Cameron, R.P.Liljestrand, P.Kitching, C.A.Miller, W.J.McDonald, D.M.Sheppard, W.C.Olsen, G.C.Neilson, H.S.Sherif, D.K.McDaniels, J.R.Tinsley, L.W.Swenson, P.Schwandt, C.E.Stronach, L.Ray Elastic Scattering of 400-MeV Protons by 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), E=400 MeV; measured σ(θ), A(θ). Second-order Kerman-McManus-Thaler optical model analysis.
doi: 10.1103/PhysRevLett.47.315
1981PA22 Phys.Lett. 106B, 470 (1981) G.Pauletta, G.Adams, M.M.Gazzaly, G.J.Igo, A.T.M.Wang, A.Rahbar, A.Wriekat, L.Ray, G.W.Hoffmann, M.Barlett, J.Amann Elastic Scattering of 0.8 GeV Polarized Protons from 46,48Ti NUCLEAR REACTIONS 46,48Ti(polarized p, p), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced neutron density distribution. Kerman-McManus-Thaler formalism.
doi: 10.1016/0370-2693(81)90259-8
1981RA02 Phys.Rev. C23, 828 (1981) L.Ray, G.W.Hoffmann, M.Barlett, J.McGill, J.Amann, G.Adams, G.Pauletta, M.Gazzaly, G.S.Blanpied Proton Elastic Scattering from 40,42,44,48Ca at 800 MeV NUCLEAR REACTIONS 40,42,44,48Ca(p, p), E=800 MeV; measured σ(θ); analyzed analyzing power data. 40,42,44,48Ca deduced neutron, isotopic density differences. Second-order Kerman-McManus-Thaler optical potential.
doi: 10.1103/PhysRevC.23.828
1981RA10 Phys.Lett. 102B, 88 (1981) Spin-Orbit Deformation Effects in (p, p') from Non-Spherical Nuclei at Intermediate Energies NUCLEAR REACTIONS 24Mg, 154Sm(p, p'), (polarized p, p'), E=0.8 GeV; calculated σ(θ), analyzing power vs θ. Multistep processes, deformed spin-orbit potential, coupled-channels analysis.
doi: 10.1016/0370-2693(81)91036-4
1980BA30 Phys.Rev. C22, 1168 (1980) M.L.Bartlett, J.A.McGill, L.Ray, M.M.Bartlett, G.W.Hoffmann, N.M.Hintz, G.S.Kyle, M.A.Franey, G.Blanpied Proton Scattering from 154Sm and 176Yb at 0.8 GeV NUCLEAR REACTIONS 154Sm, 176Yb(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 154Sm, 176Yb levels deduced deformation lengths. DWBA, coupled channel analysis, rotational model. Enriched targets.
doi: 10.1103/PhysRevC.22.1168
1980HO09 Phys.Rev. C21, 1488 (1980) G.W.Hoffman, L.Ray, M.Barlett, 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 0.8 GeV p + 208Pb Elastic Scattering and the Quantity Δr(np) NUCLEAR REACTIONS 208Pb(p, p), E=0.8 GeV; measured σ(θ); deduced neutron, proton rms radius difference. Microscopic optical model analysis.
doi: 10.1103/PhysRevC.21.1488
1980RA13 Phys.Rev. C22, 1454 (1980) L.Ray, G.W.Hoffmann, R.M.Thaler Coulomb Interaction in Multiple Scattering Theory NUCLEAR REACTIONS 208Pb(p, p), E=0.8 GeV; calculated σ(θ). Multiple scattering theories, Coulomb correction.
doi: 10.1103/PhysRevC.22.1454
1979AD03 Phys.Rev.Lett. 43, 421 (1979) G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.R.Smith, M.Gazzaly, L.Ray, W.G.Love, F.Petrovich Microscopic Description of 800-MeV Polarized-Proton Scattering from 16O NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), A(θ). Microscopic impulse approximation analysis.
doi: 10.1103/PhysRevLett.43.421
1979BL04 Phys.Rev. C20, 1490 (1979) G.Blanpied, N.M.Hintz, G.S.Kyle, J.W.Palm, R.Liljestrand, M.Barlett, C.Harvey, G.W.Hoffmann, L.Ray, D.G.Madland Proton Scattering from 24Mg at 0.8 GeV NUCLEAR REACTIONS 24Mg(p, p'), E=0.8 GeV; measured σ(θ). 24Mg levels deduced deformation length. Optical model, DWBA, coupled-channels, symmetric, asymmetric rotator model analyses.
doi: 10.1103/PhysRevC.20.1490
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
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
1979RA14 Phys.Rev. C19, 1855 (1979); Erratum Phys.Rev. C20, 1212 (1979) Neutron Isotopic Density Differences Deduced from 0.8 GeV Polarized Proton Elastic Scattering NUCLEAR REACTIONS 40,48Ca, 58,64Ni, 116,124Sn, 208Pb(p, p), E=0.8 GeV; calculated σ(θ); deduced neutron density distributions, radii. Kerman, McManus, Thaler optical potential with target nucleon correlation, electromagnetic corrections.
doi: 10.1103/PhysRevC.19.1855
1979RA15 Phys.Lett. 83B, 275 (1979) L.Ray, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Kyle, N.M.Hintz, M.A.Oothoudt, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, R.M.Rolfe, C.A.Whitten, Jr. Coupled-Channels Effects in 0.8 GeV Proton Inelastic Scattering from 58Ni NUCLEAR REACTIONS 58Ni(p, p'), E=0.8 GeV; calculated σ(θ). Coupled channel, DWBA calculations with multistep, multiphonon mixing.
doi: 10.1016/0370-2693(79)91106-7
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
1979RA27 Phys.Rev. C20, 1857 (1979) Proton-Nucleus Total Cross Sections in the Intermediate Energy Range NUCLEAR REACTIONS 12C, 16O, 27Al, 56Fe, 63,65Cu, 72,74Ge, 127I, 208Pb(p, p), (p, n), (p, X), E=100-2200 MeV; calculated total, reaction σ(E). Kerman, McManus, Thaler optical potential, target nucleon correlation.
doi: 10.1103/PhysRevC.20.1857
1979RA33 Phys.Rev. C20, 2403 (1979) Neutron Densities and the Single Particle Structure of Several Even-Even Nuclei from 40Ca to 208Pb NUCLEAR STRUCTURE 40,48Ca, 58,64Ni, 116,124Sn, 208Pb; calculated proton, neutron one-body densities. Summed squares of single particle functions, nonlocal potentials, nonorthogonal effects.
doi: 10.1103/PhysRevC.20.2403
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
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
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
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
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
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
1978RA20 Phys.Lett. 79B, 182 (1978) '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
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
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
1977RA07 Phys.Rev. C16, 340 (1977) '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
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
1976RA06 Phys.Rev. C13, 1367 (1976) 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
1976RA11 Phys.Rev. C13, 2366 (1976) Exact Finite-Range Coupled-Channels Born Approximation Analysis of 13C-Induced Reactions NUCLEAR REACTIONS 28Si(13C, 12C), E=36 MeV; calculated σ(θ). Exact finite-range CCBA with surface transparent potential.
doi: 10.1103/PhysRevC.13.2366
1975BL09 Phys.Rev. C12, 1726 (1975) G.Blanpied, R.Liljestrand, J.Lynch, J.McIntyre, L.Ray, G.W.Hoffmann Neutron Resonances in 24Na via the (d, p) Reaction NUCLEAR REACTIONS 23Na(d, p), E=11 MeV; measured σ(Ep, θ). 24Na deduced levels, L, J, π, S. DWBA analysis.
doi: 10.1103/PhysRevC.12.1726
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
1975RA13 Phys.Lett. 56B, 318 (1975) 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
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
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