NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.Byrd Found 78 matches. 1998HA24 Nucl.Instrum.Methods Phys.Res. A401, 345 (1998) S.S.Hanna, C.J.Martoff, D.Pocanic, K.Wang, R.C.Byrd, C.C.Foster, I.J.van Heerden A Monochromatic Neutron Facility for (n, p) Reactions NUCLEAR REACTIONS 6Li, 13C(n, p), E=118 MeV; measured proton spectra.
doi: 10.1016/S0168-9002(97)00985-6
1996MA58 Phys.Rev. C54, 2767 (1996) C.J.Martoff, S.S.Hanna, D.Pocanic, K.Wang, W.J.Cummings, R.C.Byrd, C.C.Foster Reaction 13C(n, p)13B at 118 MeV NUCLEAR REACTIONS 13C(n, p), E=118 MeV; measured σ(θ), proton spectra; deduced nucleon-nucleon interaction spin-isospin component central part volume integral, (n, p), (p, n) reaction σ universal proportionality energy dependence.
doi: 10.1103/PhysRevC.54.2767
1995PR04 Phys.Rev. C52, 228 (1995) D.L.Prout, C.Zafiratos, T.N.Taddeucci, J.Ullmann, R.C.Byrd, T.A.Carey, P.Lisowski, J.B.McClelland, L.J.Rybarcyk, W.Sailor, W.Amian, M.Braunstein, D.Lind, D.J.Mercer, D.Cooper, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, B.K.Park, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, D.Ciskowski, W.P.Alford Cross Sections and Analyzing Powers for Quasielastic Scattering at 795 and 495 MeV using the (p(pol), n) Reaction NUCLEAR REACTIONS 12C, Pb(polarized p, n), E=495, 795 MeV; measured σ(θ), analyzing power vs energy loss. Models comparison.
doi: 10.1103/PhysRevC.52.228
1994DR10 Nucl.Instrum.Methods Phys.Res. B84, 337 (1994) D.M.Drake, M.Drosg, R.C.Byrd, R.C.Reedy, D.A.Clark, P.A.J.Englert, J.F.Dempsey, S.G.Bobias, L.Harris Experimental and Numerical Simulation of Martian Neutron Distributions
doi: 10.1016/0168-583X(94)95726-6
1994ME07 Phys.Rev. C49, 3104 (1994) D.J.Mercer, J.Rapaport, C.A.Whitten, Jr., D.Adams, R.Byrd, X.Y.Chen, A.Fazely, T.Gaussiran, E.Gulmez, C.Goodman, D.W.Huang, G.Igo, A.Ling, D.Marchlenski, D.Prout, L.Rybarcyk, E.Sugarbaker, T.N.Taddeucci Multipole Decomposition of the 16O(p, n)16F and 18O(p, n)18F Reactions at 494 MeV NUCLEAR REACTIONS 16,18O(p, n), E=494 MeV; measured σ(θ); deduced transition multipole components for ΔL=0, ΔL=1, ΔL ≥ 2. 18,16F deduced Gamow-Teller strength B(GT).
doi: 10.1103/PhysRevC.49.3104
1994TA24 Phys.Rev.Lett. 73, 3516 (1994) T.N.Taddeucci, B.A.Luther, L.J.Rybarcyk, R.C.Byrd, J.B.McClelland, D.L.Prout, S.DeLucia, D.A.Cooper, D.G.Marchlenski, E.Sugarbaker, B.K.Park, T.Sams, C.D.Goodman, J.Rapaport, M.Ichimura, K.Kawahigashi Momentum Dependence of the Nuclear Isovector Spin Responses from (p(pol), n(pol)) Reactions at 494 MeV NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=494 MeV; measured polarization transfer coefficients; deduced longitudinal, transverse isovector spin responses.
doi: 10.1103/PhysRevLett.73.3516
1993AM06 Nucl.Sci.Eng. 115, 1 (1993) W.B.Amian, R.C.Byrd, D.A.Clark, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss Differential Neutron Production Cross Sections for 597-MeV Protons NUCLEAR REACTIONS C, 27Al, Fe, Pb, Ni, B, O, 238U(p, xn), E=597 MeV; measured σ(θn, En). Intranuclear cascade evaporation model.
doi: 10.13182/NSE93-A35517
1993CH13 Phys.Rev. C47, 2159 (1993) X.Y.Chen, T.N.Taddeucci, J.B.McClelland, T.A.Carey, R.C.Byrd, L.J.Rybarcyk, W.C.Sailor, D.J.Mercer, D.L.Prout, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, Y.Wang, W.P.Alford Polarization Transfer in Quasifree (p(pol), n(pol) Reactions at 495 MeV NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=495 MeV; measured σ(θ), analyzing power, polarization transfer coefficient vs energy loss; deduced response functions, residual interaction modifications.
doi: 10.1103/PhysRevC.47.2159
1993ME06 Phys.Rev.Lett. 71, 684 (1993) D.J.Mercer, T.N.Taddeucci, L.J.Rybarcyk, X.Y.Chen, D.L.Prout, R.C.Byrd, J.B.McClelland, W.C.Sailor, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, J.Rapaport Polarization Transfer in (p(pol), n(pol)) Reactions at 318 and 494 MeV and the Effective Interaction NUCLEAR REACTIONS 2H, 12,14C(polarized p, n), E=318, 494 MeV; measured polarization transfer observable; deduced medium effects modification to effective interaction.
doi: 10.1103/PhysRevLett.71.684
1993ST06 Phys.Rev. C47, 1647 (1993) S.Stamer, W.Scobel, W.B.Amian, R.C.Byrd, R.C.Haight, J.L.Ullmann, R.W.Bauer, M.Blann, B.A.Pohl, J.Bisplinghoff, R.Bonetti Double Differential Cross Sections for Neutron Emission Induced by 256 MeV and 800 MeV Protons NUCLEAR REACTIONS 7Li, 27Al, Zr, Pb(p, xn), E=256, 800 MeV; measured σ(θ, E); deduced reaction mechanism. Intranuclear cascade, statistical multi-step, hybrid models.
doi: 10.1103/PhysRevC.47.1647
1992AM03 Nucl.Instrum.Methods Phys.Res. A313, 452 (1992) W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, G.L.Morgan, C.E.Moss Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 135 and 800 MeV NUCLEAR REACTIONS Pb, 7Li(p, n), E ≤ 800 MeV; measured neutron detection efficiency for E=135-800 MeV; Fe(n, n), E=110-725 MeV; measured total σ. Cylindrical BC418 neutron detector, efficiency calibration.
doi: 10.1016/0168-9002(92)90823-M
1992AM07 Nucl.Sci.Eng. 112, 78 (1992) W.B.Amian, R.C.Byrd, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss, D.A.Clark Differential Neutron Production Cross Sections for 800-MeV Protons NUCLEAR REACTIONS U, B, C, N, O, 27Al, Fe, Cd, W, Pb, 9Be(p, xn), E=800 MeV; measured σ(θ, En). Model comparison, tof.
doi: 10.13182/NSE92-A23953
1992BY01 Nucl.Instrum.Methods Phys.Res. A313, 457 (1992) R.C.Byrd, W.C.Sailor, Y.Yariv, T.A.Carey, A.Gavron Measurements and Calculations of the Gamma Response of Neutron Scintillators RADIOACTIVITY 137Cs(β-); 22Na(β+), (EC); 203Hg(β-); measured detector γ-response. Neutron scintillators, organic scintillator based model simulations.
doi: 10.1016/0168-9002(92)90824-N
1992MC09 Phys.Rev.Lett. 69, 582 (1992) J.B.McClelland, T.N.Taddeucci, X.Y.Chen, W.P.Alford, R.C.Byrd, T.A.Carey, S.DeLucia, C.D.Goodman, E.Gulmez, W.Huang, B.Luther, D.G.Marchlenski, D.J.Mercer, D.L.Prout, J.Rapaport, L.J.Rybarcyk, W.Sailor, E.Sugarbaker, Y.Wang, C.Whitten, Jr. Quasifree Polarization-Transfer Measurements in the (p(pol), n(pol)) Reaction at 495 MeV NUCLEAR REACTIONS 2H, C, Ca(polarized p, n), E=495 MeV; measured polarization transfer variables, complete set; deduced longitudinal to spin-transverse responses ratio. Distorted waves, RPA nuclear response.
doi: 10.1103/PhysRevLett.69.582
1992VI06 Phys.Rev. C46, 410 (1992) S.E.Vigdor, W.W.Jacobs, L.D.Knutson, J.Sowinski, C.Bloch, P.L.Jolivette, S.W.Wissink, R.C.Byrd, C.Whiddon Charge Symmetry Breaking in n(pol)-p(pol) Scattering at 183 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=183 MeV; measured spin-correlation C(NN) vs θ; deduced charge symmetry breaking evidence. High precision, polarized target.
doi: 10.1103/PhysRevC.46.410
1991KN02 Phys.Rev.Lett. 66, 1410 (1991) L.D.Knutson, S.E.Vigdor, W.W.Jacobs, J.Sowinski, P.L.Jolivette, S.W.Wissink, C.Bloch, C.Whiddon, R.C.Byrd Charge-Symmetry Violation in Neutron-Proton Elastic Scattering at E(n) = 183 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=183 MeV; measured analyzing powers, difference; deduced charge symmetry violation evidence.
doi: 10.1103/PhysRevLett.66.1410
1991PE02 Phys.Rev. C43, 2336 (1991) R.S.Pedroni, R.C.Byrd, G.M.Honore, C.R.Howell, R.L.Walter Scattering of Polarized and Unpolarized Neutrons from 93Nb from 8 to 17 MeV and Optical Model Descriptions NUCLEAR REACTIONS 93Nb(polarized n, n), (n, n), E=8-17 MeV; measured σ(E, θ), analyzing power vs E, θ; deduced optical model parameters. Pulsed beam, tof.
doi: 10.1103/PhysRevC.43.2336
1991TA13 Nucl.Phys. A527, 393c (1991) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.D.Goodman, E.Gulmez, W.Huang, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker Cross Section and Analyzing Power for Quasifree (p, n) Reactions NUCLEAR REACTIONS 12C(polarized p, n), E=494, 795 MeV; measured σ(θ), analyzing power; deduced quasifree neutron knockout. Relativistic fermi gas model.
doi: 10.1016/0375-9474(91)90128-S
1990JA17 J.Phys.(Paris), Colloq.C-6, 511 (1990) W.W.Jacobs, L.D.Knutson, S.E.Vigdor, J.G.Sowinski, P.L.Jolivette, S.W.Wissink, C.Bloch, R.C.Byrd, C.Whiddon Charge Symmetry Breaking in n-p Scattering at 183 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=183 MeV; measured spin-dependent asymmetry vs θ. Meson-exchange calculations. Polarized target.
1990KN02 Nucl.Phys. A508, 185c (1990) L.D.Knutson, S.E.Vigdor, W.W.Jacobs, J.Sowinski, P.L.Jolivette, S.W.Wissink, C.Bloch, C.Whiddon, R.C.Byrd A Test of Charge Symmetry in n-p Scattering at E(n) = 183 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=183 MeV; measured asymmetry, analyzing power difference; deduced charge symmetry breaking evidence. Polarized target.
doi: 10.1016/0375-9474(90)90474-Z
1990SC14 Phys.Rev. C41, 2010 (1990) W.Scobel, M.Trabandt, M.Blann, B.A.Pohl, B.R.Remington, R.C.Byrd, C.C.Foster, R.Bonetti, C.Chiesa, S.M.Grimes Preequilibrium (p, n) Reaction as a Probe for the Effective Nucleon-Nucleon Interaction in Multistep Direct Processes NUCLEAR REACTIONS 27Al, 90Zr, 208Pb(p, xn), E=120-160 MeV; measured σ(En, θ); deduced effective NN-interaction strength.
doi: 10.1103/PhysRevC.41.2010
1990SO13 J.Phys.(Paris), Colloq.C-6, 395 (1990) J.Sowinski, W.W.Jacobs, L.D.Knutson, S.E.Vigdor, P.L.Jolivette, S.W.Wissink, C.Bloch, R.C.Byrd, M.Minty, E.J.Stephenson, J.Templon, C.Whiddon Spin Observables in Nucleon-Nucleon Scattering Near 180 MeV NUCLEAR REACTIONS 1H(polarized n, p), (polarized p, p), E=180 MeV; measured analyzing power, spin correlation parameter vs θ. Phase shift, model analyses.
1990SU12 Phys.Rev.Lett. 65, 551 (1990) E.Sugarbaker, D.Marchlenski, T.N.Taddeucci, L.J.Rybarcyk, J.B.McClelland, T.A.Carey, R.C.Byrd, C.D.Goodman, W.Huang, J.Rapaport, D.Mercer, D.Prout, W.P.Alford, E.Gulmez, C.A.Whitten, D.Ciskowski Isovector Effective Interactions from 14C(p, n)14N Studies between 500 and 800 MeV NUCLEAR REACTIONS 14C(p, n), E=494, 644, 795 MeV; measured σ(θ=0°); deduced effective nucleon interaction components.
doi: 10.1103/PhysRevLett.65.551
1990TA11 Phys.Rev. C41, 2548 (1990) T.N.Taddeucci, W.P.Alford, M.Barlett, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, C.A.Goulding, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker, C.A.Whitten, Jr. Zero-Degree Cross Sections for the 7Li(p, n)7Be(g.s.+0.43-MeV) Reaction in the Energy Range 80-795 MeV NUCLEAR REACTIONS 7Li(p, n), E=80-795 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.41.2548
1990TA15 Phys.Rev. C42, 935 (1990) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, E.Sugarbaker, I.J.Van Heerden, C.A.Whitten, Jr. Gamow-Teller Transition Strengths from the 11B(p, n)11C Reaction in the Energy Range 160-795 MeV NUCLEAR REACTIONS 11B(p, n), E=160-795 MeV; measured σ(En, θ=0°). 11C levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.42.935
1989AM03 Nucl.Instrum.Methods Phys.Res. A281, 353 (1989) W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, C.E.Moss Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 30 and 200 MeV NUCLEAR REACTIONS 7Li(p, n), E not given; measured neutron spectra; deduced detector efficiency. Tof, BC418 detector.
doi: 10.1016/0168-9002(89)91333-8
1989BY02 Nucl.Instrum.Methods Phys.Res. A274, 494 (1989) Neutron Detection Efficiency for NE213 and BC501 Scintillators at Energies between 25 and 200 MeV NUCLEAR REACTIONS 7Li(p, n), E=29.2-200.2 MeV; measured σ(θn, En), θ=0°; deduced detector efficiency.
doi: 10.1016/0168-9002(89)90180-0
1989GU02 Phys.Rev. C39, 405 (1989) P.P.Guss, R.C.Byrd, C.R.Howell, R.S.Pedroni, G.Tungate, R.L.Walter, J.P.Delaroche Optical Model Description of the Neutron Interaction with 116Sn and 120Sn Over a Wide Energy Range NUCLEAR REACTIONS 120Sn(polarized n, n), (polarized n, n'), E=10-17 MeV; 116Sn(polarized n, n), (polarized n, n'), E=10, 14 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 120,116Sn levels deduced neutron, proton multipole deformation parameters.
doi: 10.1103/PhysRevC.39.405
1989PI06 Phys.Rev. C39, 1679 (1989) W.K.Pitts, H.O.Meyer, L.C.Bland, J.D.Brown, R.C.Byrd, M.Hugi, H.J.Karwowski, P.Schwandt, A.Sinha, J.Sowinski, I.J.van Heerden 2H(d(pol), γ)4He Reaction at E(d) = 95 MeV NUCLEAR REACTIONS 2H(polarized d, γ), E=95 MeV; measured σ(θ), vector, tensor analyzing power vs θ.
doi: 10.1103/PhysRevC.39.1679
1989RA09 Phys.Rev. C39, 1929 (1989) J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).
doi: 10.1103/PhysRevC.39.1929
1989TR01 Phys.Rev. C39, 452 (1989); Erratum Phys.Rev. C39, 2089 (1989) M.Trabandt, W.Scobel, M.Blann, B.A.Pohl, R.C.Byrd, C.C.Foster, R.Bonetti, S.M.Grimes Preequilibrium Neutron Emission in the Reactions 90Zr, 208Pb(p, xn) with 80 MeV Projectiles NUCLEAR REACTIONS 90Zr, 208Pb(p, xn), E=80 MeV; measured σ(E(n), θ(n)). Model calculations.
doi: 10.1103/PhysRevC.39.452
1988HO12 Phys.Rev. C38, 1552 (1988) C.R.Howell, R.S.Pedroni, G.M.Honore, K.Murphy, R.C.Byrd, G.Tungate, R.L.Walter Scattering of Polarized and Unpolarized Nucleons from 28Si NUCLEAR REACTIONS 28Si(polarized n, n), (polarized n, n'), (n, n), (n, n'), E=8-17 MeV; measured σ(En), analyzing power vs θ, σ(θ); deduced model parameters. 28Si levels deduced multipole moments, B(λ). Analyzed other data.
doi: 10.1103/PhysRevC.38.1552
1988PE20 Phys.Rev. C38, 2052 (1988) R.S.Pedroni, C.R.Howell, G.M.Honore, H.G.Pfutzner, R.C.Byrd, R.L.Walter, J.P.Delaroche Energy Dependence of the Deformed Optical Potential for Neutron Scattering from 54,56Fe and 58,60Ni up to 80 MeV NUCLEAR REACTIONS 54Fe, 58Ni(polarized n, n), (polarized n, n'), E=10, 14, 17 MeV; 56Fe, 60Ni(polarized n, n), (polarized n, n'), E=10 MeV; measured analyzing power vs θ. 54Fe, 58Ni(n, n), (n, n'), E=17 MeV; measured σ(θ); deduced deformation parameters for central, real spin-orbit potentials. Coupled channels calculations.
doi: 10.1103/PhysRevC.38.2052
1988PI01 Phys.Rev. C37, 1 (1988) W.K.Pitts, H.O.Meyer, L.C.Bland, J.D.Brown, R.C.Byrd, M.Hugi, H.J.Karwowski, P.Schwandt, A.Sinha, J.Sowinski, I.J.van Heerden, A.Arriaga, F.D.Santos 1H(d(pol), γ)3He Reaction at E(d) = 95 MeV NUCLEAR REACTIONS, MECPD 1H(polarized d, γ), E=95 MeV; measured σ(θ), analyzing power vs θ. 3He deduced D- to S- state asymptotic normalization ratio.
doi: 10.1103/PhysRevC.37.1
1988WA24 Phys.Rev. C38, 2478 (1988) K.Wang, C.J.Martoff, D.Pocanic, W.J.Cummings, S.S.Hanna, R.C.Byrd, C.C.Foster Reaction 6Li(n, p)6He at 118 MeV NUCLEAR REACTIONS 6Li(n, p), E=118 MeV; measured σ(θ); deduced Gamow-Teller resonance, sum rule. DWBA analyses. Intrinsic germanium detectors, enriched target.
doi: 10.1103/PhysRevC.38.2478
1987FA03 Phys.Lett. 185B, 321 (1987) M.Fatyga, R.C.Byrd, K.Kwiatkowski, W.G.Wilson, L.W.Woo, V.E.Viola, Jr., H.J.Karwowski, J.Jastrzebski, W.Skulski Source Properties of Intermediate Mass Fragments Emitted in the 270 MeV 3He + 232Th Reaction NUCLEAR REACTIONS 232Th(3He, X), (3He, F), E=270 MeV; measured fission probability following intermediate mass fragmentation; deduced reaction mechanism. ΔE-E telescopes.
doi: 10.1016/0370-2693(87)91007-0
1987KR10 Phys.Lett. 189B, 299 (1987) D.Krofcheck, E.Sugarbaker, A.J.Wagner, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, C.Gaarde, D.J.Horen, T.Carey, T.N.Taddeucci Gamow-Teller Strength Distribution in 81Kr and the Consequences for a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 81Br(p, n), E=190, 200 MeV; measured σ(En). 81Kr transitions deduced Gamow-Teller transition strength distribution. Tof.
doi: 10.1016/0370-2693(87)91436-5
1987PO18 Can.J.Phys. 65, 687 (1987) D.Pocanic, K.Wang, C.J.Martoff, S.S.Hanna, R.C.Byrd, C.C.Foster, D.L.Friesel, J.Rapaport First (n, p) Measurements with the Indiana University Cyclotron Facility NUCLEAR REACTIONS 6Li(n, p), E=118 MeV; measured σ(Ep), σ(θp). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152. 1987SA02 Phys.Rev. C35, 344 (1987) H.Sakai, T.A.Carey, J.B.McClelland, T.N.Taddeucci, R.C.Byrd, C.D.Goodman, D.Krofcheck, L.J.Rybarcyk, E.Sugarbaker, A.J.Wagner, J.Rapaport Cross Section and Transverse Polarization Transfer for the 2H(p, n)2p Reaction at 160 MeV NUCLEAR REACTIONS, MECPD 2H(p, n), E=160 MeV; measured σ(En, θ), transverse polarization coefficient. Plastic scintillators. Impulse approximation analysis.
doi: 10.1103/PhysRevC.35.344
1987SO16 Phys.Lett. 199B, 341 (1987) J.Sowinski, R.C.Byrd, W.W.Jacobs, S.E.Vigdor, C.Whiddon, S.W.Wissink, L.D.Knutson, P.L.Jolivette A Measurement of the Spin Correlation Parameter C(NN)(θ) in n-p Scattering at 181 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=181 MeV; measured spin correlation parameter. Model comparison.
doi: 10.1016/0370-2693(87)90930-0
1987TA13 Nucl.Phys. A469, 125 (1987) T.N.Taddeucci, C.A.Goulding, T.A.Carey, R.C.Byrd, C.D.Goodman, C.Gaarde, J.Larsen, D.Horen, J.Rapaport, E.Sugarbaker The (p, n) Reaction as a Probe of Beta Decay Strength NUCLEAR REACTIONS 12,14C, 42Ca, 28Si, 90Zr, 208Pb, 7Li, 54Fe(p, n), E=50-200 MeV; measured σ(Ep, θ=0°). 12,14N, 42Sc, 28P, 90Nb, 208Bi, 7Be, 54Co deduced reaction population, B(GT) proportionality.
doi: 10.1016/0375-9474(87)90089-3
1986HO05 Phys.Rev. C33, 1129 (1986) G.M.Honore, W.Tornow, C.R.Howell, R.S.Pedroni, R.C.Byrd, R.L.Walter, J.P.Delaroche Coupled-Channel Analysis of Nucleon Scattering from 40Ca up to 80 MeV NUCLEAR REACTIONS 40Ca(n, n), (n, n'), (polarized n, n), (polarized n, n'), E=11-17 MeV; measured σ(θ), analyzing power vs θ; deduced potential parameters, geometries, energy dependences. 40Ca levels deduced deformation.
doi: 10.1103/PhysRevC.33.1129
1986HO20 Phys.Rev. C34, 825 (1986) G.M.Honore, R.S.Pedroni, C.R.Howell, H.G.Pfutzner, R.C.Byrd, G.Tungate, R.L.Walter Differential Cross Sections and Analyzing Powers for Neutron Elastic Scattering from 89Y between 8 and 17 MeV NUCLEAR REACTIONS 89Y(polarized n, n), E=8-17 MeV; measured σ(θ), A(θ); deduced spherical optical model parameters.
doi: 10.1103/PhysRevC.34.825
1986MU07 Nucl.Phys. A455, 525 (1986) K.Murphy, R.C.Byrd, C.E.Floyd, P.P.Guss, R.L.Walter Measurements of σ(θ) and A(y)(θ) for the 9Be(p, n)9B Reaction and Lane Model Analysis for the 9Be + Nucleon System NUCLEAR REACTIONS 9Be(polarized p, n), E=8-17.57 MeV; measured σ(θ), A(θ); 9Be(p, p), 9Be(p, n), 9Be(n, n), E=11-17 MeV; analyzed data; deduced potential parameters. Lane model calculations, complex isovector spin-orbit potential, Coulomb correction terms.
doi: 10.1016/0375-9474(86)90320-9
1986MU08 Radiat.Eff. 92, 219 (1986) K.Murphy, R.C.Byrd, C.R.Howell, R.L.Walter Nucleon Scattering from 11B and 10B NUCLEAR REACTIONS 11B(n, n), E=10-17 MeV; measured σ(θ). 11B(polarized n, n), E=10, 15 MeV; measured analyzing power vs θ. 11B(p, n), (polarized p, n), E=12.77-17.22 MeV; measured σ(θ), analyzing power vs θ. 11B(p, p), E=10-17 MeV; measured σ(θ); deduced potential parameters. Lane model analysis.
doi: 10.1080/00337578608208326
1986TA05 Phys.Rev. C33, 746 (1986) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker Spin-Flip Decomposition of the Spectrum for 90Zr(p, n) at E(p) = 160 MeV NUCLEAR REACTIONS 90Zr(polarized p, n), E=160 MeV; measured σ(θ=0°), transverse polarization transfer. 90Nb deduced ΔL=0, ΔL=1 resonance excitations, transition strengths.
doi: 10.1103/PhysRevC.33.746
1985GO02 Phys.Rev.Lett. 54, 877 (1985); Erratum Phys.Rev.Lett. 54, 2060 (1985) C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker, T.N.Taddeucci Measurements of Gamow-Teller Strength Distributions in Masses 13 and 15 NUCLEAR REACTIONS 13C, 15N(polarized p, n), E=160 MeV; measured σ(θ), spin-flip probabilities. 13N, 15O deduced quenched Gamow-Teller transition strengths. Shell model comparison.
doi: 10.1103/PhysRevLett.54.877
1985GU09 Nucl.Phys. A438, 187 (1985) P.P.Guss, R.C.Byrd, C.E.Floyd, C.R.Howell, K.Murphy, G.Tungate, R.S.Pedroni, R.L.Walter, J.P.Delaroche, T.B.Clegg Cross Sections and Analyzing Powers for Fast-Neutron Scattering to the Ground and First Excited States of 58Ni and 60Ni NUCLEAR REACTIONS 58,60Ni(n, n), (polarized n, n), (n, n'), E=8-14 MeV; measured σ(θ), analyzing power vs θ; deduced p, n deformation parameters. Optical model, coupled-channels analysis.
doi: 10.1016/0375-9474(85)90124-1
1985KR10 Phys.Rev.Lett. 55, 1051 (1985) D.Krofcheck, E.Sugarbaker, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, I.J.Van Heerden, C.Gaarde, J.S.Larsen, D.J.Horen, T.N.Taddeucci Gamow-Teller Strength Function in 71Ge via the (p, n) Reaction at Medium Energies NUCLEAR REACTIONS 71Ga(p, n), E=120, 200 MeV; measured σ(En), σ(θ, En); deduced neutrino capture σ corrections in 71Ga detector. 71Ge deduced Gamow-Teller strength function, transition strength fragmentation.
doi: 10.1103/PhysRevLett.55.1051
1985TA23 Nucl.Instrum.Methods 241, 448 (1985) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, T.A.Carey, D.J.Horen, J.Rapaport, E.Sugarbaker A Neutron Polarimeter for (p, n) Measurements at Intermediate Energies NUCLEAR REACTIONS 14C(polarized p, n), E=80, 120, 160 MeV; measured transverse polarization transfer, σ(En). Large volume, large acceptance neutron polarimeter, plastic scintillator.
doi: 10.1016/0168-9002(85)90597-2
1985TO02 J.Phys.(London) G11, 379 (1985) W.Tornow, R.L.Walter, R.C.Byrd Phase-Shift-Analysis Approach to Elastic Neutron Scattering from 12C between 9 and 12 MeV NUCLEAR REACTIONS 12C(polarized n, n), E=8.91-12 MeV; measured σ(θ), analyzing power vs θ, phase shifts, σ(E). 13C levels deduced J, π.
doi: 10.1088/0305-4616/11/3/016
1984BY03 Nucl.Phys. A427, 36 (1984) R.C.Byrd, C.E.Floyd, K.Murphy, P.P.Guss, R.L.Walter The Analyzing Power for Neutron Scattering from 9Be at 9 to 17 MeV NUCLEAR REACTIONS 9Be(polarized n, n), E=9-17 MeV; measured analyzing power vs θ, σ(θ); deduced Legendre coefficients. Spherical, coupled-channels optical model, imaginary spin-orbit term.
doi: 10.1016/0375-9474(84)90137-4
1983BY01 Nucl.Phys. A399, 94 (1983) R.C.Byrd, C.E.Floyd, P.P.Guss, K.Murphy, R.L.Walter Cross-Section Measurement and Lane Model Analysis for the 9Be(p, n)9B Reaction NUCLEAR REACTIONS 9Be(p, n), E=8.15-15.68 MeV; measured σ(E, θ). 9Be(p, n), E=2-30 MeV; 9Be(p, p), (p, n), (n, n), E=8-16 MeV; analyzed data. Legendre coefficient, Lane model, coupled-channels calculations.
doi: 10.1016/0375-9474(83)90596-1
1983BY02 Nucl.Phys. A404, 29 (1983) R.C.Byrd, P.W.Lisowski, W.Tornow, R.L.Walter Comparison of Polarization and Analyzing Power for the 9Be(p, n)9Be Reaction NUCLEAR REACTIONS 9Be(p, n), (polarized p, n), E=2.7, 2.9, 8.1, 9.1, 10 MeV; measured P(θ), A(θ) vs E. Compared to previous measurements.
doi: 10.1016/0375-9474(83)90412-8
1983BY03 Nucl.Phys. A410, 29 (1983) R.C.Byrd, W.Tornow, P.W.Lisowski, K.Murphy, R.l.Walter Comparison of Polarization and Analyzing Power for the 15N(p, n)15O Reaction NUCLEAR REACTIONS 15N(polarized p, n), E=3.7-12 MeV; measured A(E, θ), P(E, θ); deduced σ(E, θ), Legendre coefficients, spin-flip asymmetry. Comparison to previous P(θ) measurements.
doi: 10.1016/0375-9474(83)90399-8
1983DE35 Phys.Rev. C28, 1410 (1983) J.P.Delaroche, C.E.Floyd, P.P.Guss, R.C.Byrd, K.Murphy, G.Tungate, R.L.Walter Complex Spin-Orbit Potential for 208Pb(n, n)208Pb at 10 MeV NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=10 MeV; measured σ(θ), A(θ); deduced complex spin-orbit potential. Spherical optical model calculations.
doi: 10.1103/PhysRevC.28.1410
1983FL07 Phys.Rev. C28, 1498 (1983) C.E.Floyd, P.P.Guss, R.C.Byrd, K.Murphy, R.L.Walter, J.P.Delaroche Spin-Orbit Potential Properties Derived from Measurements of Analyzing Powers for Neutron Scattering from 54Fe and 65Cu NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=10, 14 MeV; 54Fe(polarized n, n'), E=10 MeV; measured analyzing power vs θ; deduced deformed complex spin-orbit potential parameters. Coupled-channels analysis.
doi: 10.1103/PhysRevC.28.1498
1983GU03 Nucl.Phys. A395, 1 (1983) P.P.Guss, K.Murphy, R.C.Byrd, C.E.Floyd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power for the 2H(d, n)3He(g.s.) Reaction from 5.5 to 11.5 MeV NUCLEAR REACTIONS 2H(polarized d, n), E=5.5, 7, 8.5, 10, 11.5 MeV; measured A(θ). Report discrepancies with previous measurements. Polynomial expansions analysis.
doi: 10.1016/0375-9474(83)90085-4
1983TO06 Phys.Rev. C27, 2439 (1983) W.Tornow, R.C.Byrd, C.R.Howell, R.S.Pedroni, R.L.Walter Measurements of Analyzing Power for 2H(n(pol), n)2H Scattering at 14.1 MeV and Comparisons to 2H(p(pol), p)2H NUCLEAR REACTIONS 2H(polarized n, n), E=14.1 MeV; measured analyzing power vs θ; deduced Coulomb effects. Faddeev calculations.
doi: 10.1103/PhysRevC.27.2439
1983WO02 Nucl.Phys. A394, 139 (1983) E.Woye, W.Tornow, G.Mack, C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power A(y)(θ) for 12C(n, n0, 1)12C between 8.9 and 14.9 MeV Neutron Energy NUCLEAR REACTIONS 12C(n, n), (n, n'), E=8.9-14.9 MeV; measured A(E, θ); deduced optical potential parameters. 12C level deduced quadrupole deformation.
doi: 10.1016/0375-9474(83)90167-7
1982FL01 Phys.Rev. C25, 1682 (1982) C.E.Floyd, P.P.Guss, K.Murphy, C.R.Howell, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Analyzing Powers for Neutron Elastic Scattering at Forward Angles NUCLEAR REACTIONS 40Ca, 54Fe, 65Cu, 120Sn, 208Pb(polarized n, n), E=14 MeV; measured A(θ).
doi: 10.1103/PhysRevC.25.1682
1982GU02 Phys.Rev. C25, 2854 (1982) P.P.Guss, C.E.Floyd, K.Murphy, C.R.Howell, R.S.Pedroni, G.M.Honore, H.G.Pfutzner, G.Tungate, R.C.Byrd, R.L.Walter, J.P.Delaroche Spin-Orbit Deformations Deduced from Analyzing Powers for Inelastic Neutron Scattering from 54Fe, 56Fe, 58Ni, 120Sn, and 208Pb NUCLEAR REACTIONS 54,56Fe, 58,60Ni, 120Sn, 208Pb(polarized n, n'), E=10 MeV; measured A(θ). 54,56Fe, 58,60Ni, 120Sn, 208Pb level deduced spin-orbit to Coulomb deformation parameter ratio. Coupled-channels analysis.
doi: 10.1103/PhysRevC.25.2854
1982TO06 Phys.Rev.Lett. 49, 312 (1982) W.Tornow, C.R.Howell, R.C.Byrd, R.S.Pedroni, R.L.Walter Analyzing Power Measurements for 2H(n(pol), n)2H Scattering at 10 MeV Compared to Few-Nucleon Calculations and Data for 2H(p(pol), p)2H Scattering NUCLEAR REACTIONS 2H(polarized n, n), E=10 MeV; measured analyzing power vs θ; deduced differences from p-d data, implications for three-body calculations.
doi: 10.1103/PhysRevLett.49.312
1982TO11 Nucl.Phys. A385, 373 (1982) W.Tornow, E.Woye, G.Mack, C.E.Floyd, K.Murphy, P.P.Guss, S.A.Wender, R.C.Byrd, R.L.Walter, T.B.Clegg, H.Leeb Analyzing Power and Differential Cross Section at 9.9, 11.9 and 13.9 MeV for Ca(n, n)Ca NUCLEAR REACTIONS 40Ca(polarized n, n), E=9.9, 11.9, 13.9 MeV; measured A(E, θ), σ(E, θ); deduced optical model parameters, Coulomb correction terms. Optical potential analysis, l-dependence, Fourier-Bessel expansion of the real central potential.
doi: 10.1016/0375-9474(82)90093-8
1981BY01 Nucl.Phys. A351, 189 (1981) R.C.Byrd, C.E.Floyd, K.Murphy, P.P.Guss, R.L.Walter, S.R.Cotanch Measurement and Lane-Model Analysis of Cross Sections for the 13C(p, n)13N and 15N(p, n)15O Reactions NUCLEAR REACTIONS 13C(p, n), E=10.1-16.75 MeV; 15N(p, n), E=9.05-15.62 MeV; measured σ(Ep, θ). Lane Model analysis.
doi: 10.1016/0375-9474(81)90440-1
1981FL04 Phys.Rev.Lett. 47, 1042 (1981) C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Determination of the Spin-Orbit Interaction for Neutron-Nucleus Scattering NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=14 MeV; measured σ(θ), A(θ); deduced neutron-nucleus spin-orbit interaction. Optical model.
doi: 10.1103/PhysRevLett.47.1042
1981LI23 Phys.Rev. C24, 1852 (1981) P.W.Lisowski, R.C.Byrd, G.Mack, W.Tornow, R.L.Walter, T.B.Clegg, F.D.Santos Polarization Transfer in (d(pol), n(pol)) Reactions on Light Nuclei at θ = 0° NUCLEAR REACTIONS 12C, 14N, 16O, 28Si(polarized d, n), E=5-15 MeV; measured polarization transfer. 12C(d, n), E=6-14 MeV; measured σ(θ=0°). DWBA analysis.
doi: 10.1103/PhysRevC.24.1852
1981MU01 Nucl.Phys. A355, 1 (1981) K.Murphy, R.C.Byrd, P.P.Guss, C.E.Floyd, R.L.Walter The 15N(p, n)15O Reaction below 9.3 MeV NUCLEAR REACTIONS 15N(p, n), E=5.5-9.3 MeV; measured σ(θ); deduced total σ, compared to previous measurements.
doi: 10.1016/0375-9474(81)90128-7
1981TO12 Nucl.Phys. A371, 235 (1981) W.Tornow, R.C.Byrd, P.W.Lisowski, R.L.Walter, T.R.Donoghue Comparison of Analyzing Power and Polarization in the Reaction 3H(p, n)3H (II). New Polarization Results below 4 Mev NUCLEAR REACTIONS 3H(p, n), E=2-3.8 MeV; measured P(θ, E). Charge symmetry interpretation.
doi: 10.1016/0375-9474(81)90066-X
1981TO15 Nucl.Instrum.Methods 190, 523 (1981) W.Tornow, E.Woye, G.Mack, R.L.Walter, C.E.Floyd, P.P.Guss, R.C.Byrd Small-Angle Neutron Polarization for the 2H(d(pol), n(pol))3He Reaction near E(d) = 8 MeV NUCLEAR REACTIONS 2H(polarized d, n), E=8 MeV; measured P(θn).
doi: 10.1016/0029-554X(81)90952-6
1980LI03 Nucl.Phys. A334, 45 (1980) P.W.Lisowski, R.C.Byrd, R.L.Walter, T.B.Clegg Polarization Transfer of the 2H(p, n)2p Reactions at θ = 0° NUCLEAR REACTIONS 2H(polarized p, n), E=10.6-15.1 MeV; measured transverse polarization coefficient.
doi: 10.1016/0375-9474(80)90138-4
1980MA33 Nucl.Phys. A345, 241 (1980) G.Mack, R.C.Byrd, P.W.Lisowski, R.L.Walter The Analyzing Power A(θ) for the 9Be(p(pol), n)9B Reaction from 8 to 15 MeV NUCLEAR REACTIONS 9Be(polarized p, n), E=8.1-15 MeV; measured analyzing power A(E, θ). Lane optical model calculations.
doi: 10.1016/0375-9474(80)90422-4
1980TO02 Nucl.Phys. A340, 34 (1980) W.Tornow, P.W.Lisowski, R.C.Byrd, R.L.Walter Analyzing Power Measurements for n-p Scattering between 13.5 and 16.9 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=13.5-16.9 MeV; measured A(θ); deduced spin-orbit phase parameters.
doi: 10.1016/0375-9474(80)90321-8
1979BY01 Phys.Rev.Lett. 43, 260 (1979) R.C.Byrd, R.L.Walter, S.R.Cotanch Detailed Study of the Lane Potential: Multichannel and Polarization Constraints NUCLEAR REACTIONS 9Be(p, p), (n, n), (p, n), E=10-16 MeV; calculated σ(θ), P(θ); deduced evidence for symmetry spin-orbit interaction. Lane-potential, multichannel constraints.
doi: 10.1103/PhysRevLett.43.260
1978TO03 Nucl.Phys. A296, 23 (1978) W.Tornow, P.W.Lisowski, R.C.Byrd, R.L.Walter The Analyzing Power A(y)(θ) for the Elastic Scattering of 12 MeV Neutrons from Deuterons NUCLEAR REACTIONS 2H(polarized n, n), E=12 MeV; measured A(θ), θ=30°-120°; compared to 2H(polarized p, p) reaction. C6D6 target.
doi: 10.1016/0375-9474(78)90411-6
1977TO16 Phys.Rev.Lett. 39, 915 (1977) W.Tornow, P.W.Lisowski, R.C.Byrd, R.L.Walter Discrepancies between Global Nucleon-Nucleon Phase Shifts and New Data For n-p Scattering at 16.9 MeV NUCLEAR REACTIONS 1H(polarized n, n), E ≈ 16.9 MeV; measured A(θ).
doi: 10.1103/PhysRevLett.39.915
1976DO07 Phys.Rev.Lett. 37, 981 (1976) T.R.Donoghue, S.M.A.Doyle, H.W.Clark, L.J.Dries, J.L.Regner, W.Tornow, R.C.Byrd, P.W.Lisowski, R.L.Walter Equality of Analyzing Power and Polarization in the Reaction 3H(p, n)3He NUCLEAR REACTIONS 3H(polarized p, n), E < 4 MeV; measured A(θ). 3H(p, n), E < 4 MeV; measured P(θ).
doi: 10.1103/PhysRevLett.37.981
1976TO03 Phys.Rev. C13, 2080 (1976) W.Tornow, S.E.Skubic, R.C.Byrd, P.W.Lisowski, R.L.Walter Remeasurement of p(y) for the 2H(d, n)3He Reaction and its Bearing on The Reported f-Wave Admixture of the Lowest 2- State in 4He NUCLEAR REACTIONS 2H(d, n), E=2.44 MeV; measured neutron polarization.
doi: 10.1103/PhysRevC.13.2080
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