NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.L.Walter Found 156 matches. Showing 1 to 100. [Next]2012AL15 Phys.Rev. C 86, 034603 (2012) M.A.Al-Ohali, J.P.Delaroche, C.R.Howell, M.M.Nagadi, A.A.Naqvi, W.Tornow, R.L.Walter, G.J.Weisel Neutron scattering from 28Si and 32S from 8.0 to 18.9 MeV, dispersive optical model analyses, and ground-state correlations NUCLEAR REACTIONS 28Si(n, n), E=15.4, 18.9 MeV; 32S(n, n), E=8.0, 9.9, 11.9, 13.9, 15.4, 16.9, 18.9 MeV; measured E(n), I(n), TOF, σ(E, θ), total σ(E), Ay(θ); deduced optical model potentials parameters by nucleon-nucleus dispersive optical model (DOM) analysis in the continuum and bound-state regions. 28Si(n, n), E=2.45-65.0; 32S(n, n), E=3.0-40.0 MeV; analyzed σ(E, θ) and Ay(θ) data from previous experiments by DOM. 28Si, 32S(n, n), E=2-160 MeV; analyzed total σ(E) by DOM. 28Si, 32S; deduced neutron and proton binding energies, occupation probabilities, root-mean-square radii, spectroscopic factors, and compared with variational multiparticle multihole configuration mixing (mp-mh CM) shell-model calculation using the Gogny D1S effective force.
doi: 10.1103/PhysRevC.86.034603
2010WE01 Phys.Rev. C 81, 024003 (2010) G.J.Weisel, W.Tornow, B.J.Crowe III, A.S.Crowell, J.H.Esterline, C.R.Howell, J.H.Kelley, R.A.Macri, R.S.Pedroni, R.L.Walter, H.Witala Neutron-deuteron analyzing power data at 19.0 MeV NUCLEAR REACTIONS 2H(polarized n, n), E(n)=19.0 MeV; measured analyzing powers; Monte Carlo simulation. Polarized neutrons produced in 2H(polarized d, n)3He reaction and neutron polarization measured in 4He(polarized n, n) reaction. Comparison with a three-body Faddeev calculation.
doi: 10.1103/PhysRevC.81.024003
2010ZH34 Phys.Rev. C 82, 024601 (2010) Z.Zhou, X.Ruan, Y.Du, B.Qi, H.Tang, H.Xia, R.L.Walter, R.T.Braun, C.R.Howell, W.Tornow, G.J.Weisel, M.Dupuis, J.P.Delaroche, Z.Chen, Z.Chen, Y.Chen Differential cross section for neutron scattering from 209Bi at 37 MeV and the weak particle-core coupling NUCLEAR REACTIONS 209Bi(n, n), (n, n')E=37 MeV, [neutrons produced in 3H(d, n)]; measured neutron spectra, cross sections, σ(θ), TOF method. Optical model analysis of σ(θ) data. Optical-model (OM) + DWBA calculations with weak particle-core coupling for computing (n, n) and (n, n') cross sections.
doi: 10.1103/PhysRevC.82.024601
2008BR01 Phys.Lett. B 660, 161 (2008) R.T.Braun, W.Tornow, C.R.Howell, D.E.Gonzalez Trotter, C.D.Roper, F.Salinas, H.R.Setze, R.L.Walter, G.J.Weisel Neutron-proton analyzing power at 12 MeV and inconsistencies in parametrizations of nucleon-nucleon data NUCLEAR REACTIONS 1H(polarized n, n), E=12 MeV; measured analyzing power Ay(θ) and compared with various model predictions.
doi: 10.1016/j.physletb.2007.12.039
2008CH14 Phys.Rev. C 77, 054002 (2008) Q.Chen, C.R.Howell, T.S.Carman, W.R.Gibbs, B.F.Gibson, A.Hussein, M.R.Kiser, G.Mertens, C.F.Moore, C.Morris, A.Obst, E.Pasyuk, C.D.Roper, F.Salinas, H.R.Setze, I.Slaus, S.Sterbenz, W.Tornow, R.L.Walter, C.R.Whiteley, M.Whitton Measurement of the neutron-neutron scattering length using the π-d capture reaction NUCLEAR REACTIONS 2H(π-, nγ)n, E=20 MeV; measured neutron time-of-flight spectra, Eγ, Iγ, nγ-coin, neutron-neutron scattering length.
doi: 10.1103/PhysRevC.77.054002
2006GO11 Phys.Rev. C 73, 034001 (2006) D.E.Gonzalez Trotter, F.Salinas Meneses, W.Tornow, C.R.Howell, Q.Chen, A.S.Crowell, C.D.Roper, R.L.Walter, D.Schmidt, H.Witala, W.Glockle, H.Tang, Z.Zhou, I.Slaus Neutron-deuteron breakup experiment at En = 13 MeV: Determination of the 1S0 neutron-neutron scattering length ann NUCLEAR REACTIONS 2H(n, 2n), E=13 MeV; measured En, nn-coin, σ(θ(1), θ(2)); deduced neutron-neutron scattering length, no significant three-nucleon force effects. Comparison with model predictions and previous measurements.
doi: 10.1103/PhysRevC.73.034001
2005RO29 Phys.Rev. C 72, 024605 (2005) C.D.Roper, W.Tornow, R.T.Braun, Q.Chen, A.Crowell, D.Gonzalez Trotter, C.R.Howell, F.Salinas, R.Setze, R.L.Walter, Z.Chen, H.Tang, Z.Zhou Measurements of Ay(θ) for 12C(n, n)12C from En = 2.2 to 8.5 MeV NUCLEAR REACTIONS 12C(polarized n, n), E=2.2-8.5 MeV; measured Ay(θ). Comparison with previous data and model predictions.
doi: 10.1103/PhysRevC.72.024605
2005SE05 Phys.Rev. C 71, 034006 (2005) H.R.Setze, C.R.Howell, W.Tornow, R.T.Braun, D.E.Gonzalez Trotter, A.H.Hussein, R.S.Pedroni, C.D.Roper, F.Salinas, I.Slaus, B.Vlahovic, R.L.Walter, G.Mertens, J.M.Lambert, H.Witala, W.Glockle Cross-section measurements of neutron-deuteron breakup at 13.0 MeV NUCLEAR REACTIONS 2H(n, n), (n, 2n), E=13 MeV; measured En, nn-coin, σ(θ1, θ2) for seven exit-channel configurations. Comparison with model predictions.
doi: 10.1103/PhysRevC.71.034006
2004CH62 J.Phys.(London) G30, 1847 (2004) Z.Chen, R.L.Walter, W.Tornow, G.J.Weisel, C.R.Howell A dispersive optical model for n + 120Sn from -15 to +80 MeV and properties of neutron single-particle and single-hole states NUCLEAR REACTIONS 120Sn(n, n), E=9.9-24 MeV; analyzed σ(θ), Ay(θ); Sn(n, X), E=5-80 MeV; analyzed total σ; deduced dispersive optical model parameters. 120Sn deduced neutron single-particle and single-hole states binding energies, spectroscopic factors.
doi: 10.1088/0954-3899/30/12/007
2004NA40 Phys.Rev. C 70, 064604 (2004) M.M.Nagadi, G.J.Weisel, R.L.Walter, J.P.Delaroche, P.Romain Spin-spin interaction between polarized neutrons and polarized 27Al, 59Co, and 93Nb from dispersive optical model and coupled-channel analyses NUCLEAR REACTIONS 27Al, 59Co, 93Nb(polarized n, n'), E=0.1-80 MeV; analyzed σ(θ), Ay(θ), total σ; deduced model parameters, spin-spin interaction Coupled-channels and dispersive optical model analyses.
doi: 10.1103/PhysRevC.70.064604
2003NA27 Phys.Rev. C 68, 044610 (2003) M.M.Nagadi, C.R.Howell, W.Tornow, G.J.Weisel, M.A.Al-Ohali, R.T.Braun, H.R.Setze, Z.Chen, R.L.Walter, J.P.Delaroche, P.Romain Dispersive optical-model and coupled-channels descriptions of neutron scattering from 27Al and 59Co up to 80 MeV NUCLEAR REACTIONS 27Al, 59Co(polarized n, n), E=15 MeV; measured σ(θ), Ay(θ). 59Co(n, n), E=10-19 MeV; measured σ(θ). 2H(polarized d, n), E not given; measured neutron polarization. 27Al, 59Co(n, n), E=0.1-80 MeV; compiled, analyzed σ, σ(θ), Ay(θ); deduced optical model parameters. Dispersive optical model and coupled-channels model analysis.
doi: 10.1103/PhysRevC.68.044610
2003NE01 Phys.Lett. 552B, 29 (2003) E.M.Neidel, W.Tornow, D.E.Gonzalez Trotter, C.R.Howell, A.S.Crowell, R.A.Macri, R.L.Walter, G.J.Weisel, J.Esterline, H.Witala, B.J.Crowe III, R.S.Pedroni, D.M.Markoff A new twist to the long-standing three-nucleon analyzing power puzzle NUCLEAR REACTIONS 2H(polarized n, n), E=1.2, 1.9 MeV; measured Ay(θ); deduced possible electromagnetic effect. Comparison with theory, proton scattering data.
doi: 10.1016/S0370-2693(02)03106-4
2003TO32 Mod.Phys.Lett. A 18, 258 (2003) W.Tornow, E.M.Neidel, D.E.Gonzalez Trotter, C.R.Howell, A.S.Crowell, R.A.Macri, R.L.Walter, G.J.Weisel, J.Esterline, H.Witala, B.J.Crowe III, R.S.Pedroni, D.M.Markoff Electromagnetic effects and the long-standing three-nucleon analyzing power puzzle NUCLEAR REACTIONS 2H(polarized n, n), E=1.2, 1.9 MeV; measured Ay(θ); deduced electromagnetic effects.
doi: 10.1142/S0217732303010314
2001GO17 Nucl.Phys. A684, 701c (2001) D.E.Gonzalez Trotter, W.Tornow, C.R.Howell, R.L.Walter Neutron-Deuteron Analyzing Power at En = 2.0 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=2.0 MeV; measured Ay(θ). Comparisons with proton data, model predictions.
doi: 10.1016/S0375-9474(01)00466-3
2001ZH09 Nucl.Phys. A684, 545c (2001) Z.Zhou, A.S.Crowell, J.Deng, W.Glockle, C.R.Howell, H.Kamada, B.Qi, R.A.Macri, X.Ruan, H.Tang, R.L.Walter, H.Witala The Space-Star Anomaly in nd Breakup at 25 MeV NUCLEAR REACTIONS 2H(n, np), E=25 MeV; measured nn-coin, σ(θ). Comparison with model predictions.
doi: 10.1016/S0375-9474(01)00389-X
1999GO22 Phys.Rev.Lett. 83, 3788 (1999) D.E.Gonzalez Trotter, F.Salinas, Q.Chen, A.S.Crowell, W.Glockle, C.R.Howell, C.D.Roper, D.Schmidt, I.Slaus, H.Tang, W.Tornow, R.L.Walter, H.Witala, Z.Zhou New Measurement of the 1S0 Neutron-Neutron Scattering Length using the Neutron-Proton Scattering Length as a Standard NUCLEAR REACTIONS 2H(n, np), E ≈ 13 MeV; measured neutron spectra, proton spectra, σ(θ(n), θ(p)); deduced nn and np scattering lengths.
doi: 10.1103/PhysRevLett.83.3788
1999WE06 Phys.Rev. C59, 1189 (1999) Sensitivity Tests on Parameters of the Nucleon-Nucleus Dispersive Optical Model NUCLEAR REACTIONS 208Pb(n, X), E < 80 MeV; analyzed σ, σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevC.59.1189
1998HO08 Nucl.Phys. A631, 692c (1998) C.R.Howell, H.R.Setze, W.Tornow, R.T.Braun, W.Glockle, A.H.Hussein, J.M.Lambert, G.Mertens, C.D.Roper, F.Salinas, I.Slaus, D.E.Gonzalez Trotter, B.Vlahovic, R.L.Walter, H.Witala Implications of the Space-Star Anomaly in nd Breakup NUCLEAR REACTIONS 2H(n, np), E=13.0 MeV; measured σ(φ(12), θ(n1), θ(n2)); deduced space-star configuration anomaly.
doi: 10.1016/S0375-9474(98)00093-1
1998HO24 Phys.Lett. 444B, 252 (1998) C.R.Howell, Q.Chen, T.S.Carman, A.Hussein, W.R.Gibbs, B.F.Gibson, G.Mertens, C.F.Moore, C.Morris, A.Obst, E.Pasyuk, C.D.Roper, F.Salinas, I.Slaus, S.Sterbenz, W.Tornow, R.L.Walter, C.R.Whitley, M.Whitton Toward a Resolution of the Neutron-Neutron Scattering-Length Issue NUCLEAR REACTIONS 2H(π-, nγ), E not given; measured En, nγ(θ); deduced neutron-neutron scattering length. TOF.
doi: 10.1016/S0370-2693(98)01386-0
1998TO06 Nucl.Phys. A631, 421c (1998) W.Tornow, T.S.Carman, Q.Chen, W.R.Gibbs, B.F.Gibson, D.E.Gonzalez Trotter, C.R.Howell, A.H.Hussein, G.Mertens, C.F.Moore, C.Morris, A.Obst, E.Pasyuk, C.D.Roper, F.Salinas, D.Schmidt, H.R.Setze, I.Slaus, S.Sterbenz, H.Tang, R.L.Walter, C.R.Whitley, H.Witala, Z.Zhou Scattering Length Measurements from Radiative Pion Capture and Neutron-Deuteron Breakup NUCLEAR REACTIONS 2H(π-, 2n), E not given; 2H(n, np), E=13 MeV; measured nn, np scattering lengths; deduced no three-nucleon force effects.
doi: 10.1016/S0375-9474(98)00040-2
1997AL27 Nucl.Instrum.Methods Phys.Res. A396, 388 (1997) M.A.Al-Ohali, A.Aksoy, A.Coban, J.M.Hanly, P.D.Felsher, C.R.Howell, W.Tornow, F.Salinas, R.L.Walter Determination of the Neutron Detection Efficiency of an NE213 Scintillator for E(n) = 2.5 to 1.6 MeV using the 2H(d, n)3He Reaction
doi: 10.1016/S0168-9002(97)00701-8
1997FE06 Phys.Rev. C56, 38 (1997) P.D.Felsher, C.R.Howell, W.Tornow, M.L.Roberts, J.M.Hanly, G.J.Weisel, M.Al Ohali, R.L.Walter, I.Slaus, J.M.Lambert, P.A.Treado, G.Mertens, A.C.Fonseca, A.Soldi, B.Vlahovic Analyzing Power Measurements for the d(pol) + d → d + p + n Breakup Reaction at 12 MeV NUCLEAR REACTIONS 2H(polarized d, nd), E=12 MeV; measured d, p, n spectra, σ(θ1, θ2) vs arc length, vector, tensor analyzing powers vs (θ1, θ2, arc length); deduced contributions from nucleon-nucleon P interactions. Impulse approximation calculations.
doi: 10.1103/PhysRevC.56.38
1996SE14 Phys.Lett. 388B, 229 (1996) H.R.Setze, C.R.Howell, W.Tornow, R.T.Braun, W.Glockle, A.H.Hussein, J.M.Lambert, G.Mertens, C.D.Roper, F.Salinas, I.Slaus, D.E.Gonzalez Trotter, B.Vlahovic, R.L.Walter, H.Witala Verification of the Space-Star Anomaly in nd Breakup NUCLEAR REACTIONS 2H(n, np), E=1-15 MeV; measured σ(θ1, θ2) vs arc length, total energy spectra, space-star, coplanar-star configurations; deduced space-star configuration related anomaly evidence.
doi: 10.1016/S0370-2693(96)01069-6
1996WE10 Phys.Rev. C54, 2410 (1996) G.J.Weisel, W.Tornow, C.R.Howell, P.D.Felsher, M.AlOhali, M.L.Roberts, R.K.Das, R.L.Walter, G.Mertens Analyzing Power Measurements for 209Bi(n, n) at 6 and 9 MeV and Consistent Dispersive Optical-Model Analyses for n + 209Bi and n + 208Pb from -20 to +80 MeV NUCLEAR REACTIONS 209Bi(polarized n, n), E=6, 9 MeV; measured neutron spectra, σ(θ), analyzing power vs θ. 209Bi(polarized n, n), E=1-80 MeV; 208Pb(polarized n, n), E=0.1-40 MeV; analyzed σ, σ(θ), analyzing power vs θ data; deduced model parameters. 209Pb deduced two-particle, two-hole states binding energies, occupation probabilities, spectroscopic factors, rms radii. Consistent dispersive optical model.
doi: 10.1103/PhysRevC.54.2410
1995CH39 Phys.Rev. C52, 1702 (1995) Z.P.Chen, W.Tornow, R.L.Walter Phase-Shift Analysis of Neutron-209Bi Scattering and Its Comparison to Neutron-208Pb Scattering NUCLEAR REACTIONS 209Bi(polarized n, n), E=1.5-14 MeV; analyzed σ(θ), analyzing power vs θ; deduced resonance structure features. Comparison to 208Pb+n system, phase shift analysis.
doi: 10.1103/PhysRevC.52.1702
1995HO24 Nucl.Instrum.Methods Phys.Res. B99, 316 (1995) C.R.Howell, H.R.Setze, R.T.Braun, D.E.Gonzalez Trotter, A.H.Hussein, C.D.Roper, F.Salinas, I.Slaus, W.Tornow, B.Vlahovic, R.L.Walter, G.Mertens, J.M.Lambert, H.Witala Probing the Three-Nucleon Force using Nucleon-Deuteron Breakup Reactions NUCLEAR REACTIONS 2H(n, X), E=13 MeV; measured σ(θ1, θ2) vs arc length in space-star, coplanar-star configurations following target breakup; deduced implications related to 3N-forces.
doi: 10.1016/0168-583X(94)00680-6
1994AK08 Nucl.Instrum.Methods Phys.Res. A337, 486 (1994) A.Aksoy, A.Coban, A.A.Naqvi, F.Z.Khiari, J.M.Hanly, C.R.Howell, W.Tornow, P.D.Felsher, M.A.Al-Ohali, R.L.Walter Response-Function Measurement of an NE213 Scintillator using the 2H(d, n)3He Reaction
doi: 10.1016/0168-9002(94)91118-5
1993CH23 J.Phys.(London) G19, 877 (1993) Z.M.Chen, K.Baird, C.R.Howell, M.L.Roberts, W.Tornow, R.L.Walter Neutron Scattering from 12C between 15.6 and 17.3 MeV NUCLEAR REACTIONS 12C(n, n), (n, n'), E=15.57-17.29 MeV; measured σ(θ); deduced potential parameters. Optical-model, coupled-channels approach. Other data anlayzed.
doi: 10.1088/0954-3899/19/6/008
1993HO24 Phys.Rev. C48, 2855 (1993) C.R.Howell, P.D.Felsher, W.Tornow, M.L.Roberts, J.M.Hanly, G.J.Weisel, M.Al Ohali, R.L.Walter, I.Slaus, J.M.Lambert, P.A.Treado, G.Mertens Novel Probe of Charge Symmetry Breaking: Deuteron-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(polarized d, pd), (polarized d, nd), (polarized d, np), E=12 MeV; measured vector, tensor analyzing power vs θ; deduced breakup reaction suitability as charge symmetry breaking probe.
doi: 10.1103/PhysRevC.48.2855
1993WA25 Nucl.Instrum.Methods Phys.Res. B79, 282 (1993) R.L.Walter, G.J.Weisel, R.K.Das, W.Tornow, C.R.Howell The Dispersive Optical Model for n + 208Pb and n + 209Bi NUCLEAR REACTIONS 209Bi(polarized n, n), E=9-26 MeV; analyzed σ(θ), analyzing power vs θ. 208Pb(n, n), E ≤ 80 MeV; analyzed σ(E). Dispersive optical model.
doi: 10.1016/0168-583X(93)95344-5
1992CH28 Phys.Rev. C46, 1019 (1992) Z.P.Chen, W.Tornow, R.L.Walter Phase-Shift Analysis of Neutron-208Pb Scattering and Mean-Field Studies NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=4-30 MeV; analyzed σ(θ), σ, analyzing power data; deduced overlapping resonances role. Phase shift method, comparison with dispersion relation based mean field studies.
doi: 10.1103/PhysRevC.46.1019
1992TO01 Phys.Rev. C45, 459 (1992) W.Tornow, C.R.Howell, R.L.Walter, I.Slaus Coulomb Effects in Three-Nucleon Scattering Versus Charge-Symmetry Breaking in the 3P Nucleon-Nucleon Interactions NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), E=5-8.5 MeV; analyzed analyzing power data; deduced Coulomb, charge symmetry breaking effects relative importance.
doi: 10.1103/PhysRevC.45.459
1992WE10 Phys.Rev. C46, 1599 (1992) G.J.Weisel, W.Tornow, C.R.Howell, P.D.Felsher, M.Al Ohali, Z.P.Chen, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Neutron-Proton Analyzing Power Data between 7.6 and 18.5 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=7.6-18.5 MeV; measured analyzing power vs θ. Comparison with theory.
doi: 10.1103/PhysRevC.46.1599
1991HO26 Nucl.Instrum.Methods Phys.Res. B56/57, 459 (1991) C.R.Howell, W.Tornow, H.G.Pfutzner, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, G.Mertens, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Neutron-Deuteron Elastic Scattering and Breakup Reactions Below 20 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=12 MeV; 2H(n, X), E=13 MeV; compiled, reviewed analyzing power vs θ, σ(θ1, θ2) vs arc length data for breakup.
doi: 10.1016/0168-583X(91)96070-2
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
1991RO05 Phys.Rev. C44, 2006 (1991) M.L.Roberts, P.D.Felsher, G.J.Weisel, Z.Chen, C.R.Howell, W.Tornow, R.L.Walter, D.J.Horen Measurement of A(y)(θ) for n + 208Pb from 6 to 10 MeV and the Neutron-Nucleus Interaction Over the Energy Range from Bound States at - 17 MeV Up to Scattering at 40 MeV NUCLEAR REACTIONS 208Pb(polarized n, n), (polarized n, n'), E=6-10 MeV; measured analyzing power vs E, θ, σ(θ); deduced optical model parameters. Hartree-Fock potential, dispersive terms of nuclear mean field, single-particle, single-hole energies.
doi: 10.1103/PhysRevC.44.2006
1991TO05 Phys.Lett. 257B, 273 (1991) W.Tornow, C.R.Howell, M.Alohali, Z.P.Chen, P.D.Felsher, J.M.Hanly, R.L.Walter, G.Weisel, G.Mertens, I.Slaus, H.Witala, W.Glockle The Low-Energy Neutron-Deuteron Analyzing Power and the 3P0,3P1, 3P2 Interactions of Nucleon-Nucleon Potentials NUCLEAR REACTIONS 2H(polarized n, n), E=5-8.5 MeV; measured analyzing power vs θ; deduced nucleon-nucleon interaction features.
doi: 10.1016/0370-2693(91)91892-Y
1990HO14 Nucl.Instrum.Methods Phys.Res. A290, 424 (1990) C.R.Howell, W.Tornow, H.G.Pfutzner, A.Li, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, A.Naqvi, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Techniques for Vector Analyzing Power Measurements of the 2H(n(pol), np)n Breakup Reaction at Low Energies NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured σ(En), vector analyzing power. High accuracy, breakup reaction.
doi: 10.1016/0168-9002(90)90560-S
1990PE05 Phys.Rev. C41, 2929 (1990) R.S.Pedroni, C.R.Howell, R.L.Walter Analyzing Power Measurements for Elastic Scattering of 17 MeV Neutrons from 120Sn NUCLEAR REACTIONS 120Sn(polarized n, n), E=17 MeV; measured A(y)(θ). Enriched target. Coupled-channels calculations, optical model predictions test.
doi: 10.1103/PhysRevC.41.2929
1990TO14 Few-Body Systems 8, 11 (1990) Sensitivity of n-p Scattering Observables to Charge-Independence Breaking of the 3P N-N Phase Shifts NUCLEAR REACTIONS 1H(polarized n, n), E=10, 25 MeV; calculated σ(θ), analyzing power, other polarization observables vs θ; deduced charge-independence breaking features.
doi: 10.1007/BF01078872
1990WE13 J.Phys.(Paris), Colloq.C-6, 515 (1990) G.J.Weisel, W.Tornow, C.R.Howell, P.D.Felsher, M.Alohali, Z.P.Chen, R.L.Walter, J.M.Lambert, P.A.Treado Neutron-Proton Analyzing Power Data at 7.6, 12.0, 14.1, 16.0, 18.5 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=7.6-18.5 MeV; measured analyzing power vs θ, spin correlation coefficient.
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
1989LI26 Chin.J.Nucl.Phys. 11, No.3, 1 (1989) A.Li, H.G.Pfutzner, C.R.Howell, R.L.Walter Measurements of Analyzing Power Ay(θ) for Neutron Elastic Scattering from 14N and 16O NUCLEAR REACTIONS 16O, 14N(polarized n, n), E=5-17 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. Other data analysis, optical model.
1989TO06 Nucl.Instrum.Methods Phys.Res. B40/41, 470 (1989) W.Tornow, C.R.Howell, R.L.Walter Few-Body Physics Investigated through Polarized Neutron Experiments in A ≤ 3 Systems at TUNL NUCLEAR REACTIONS 1H(polarized n, n), E=16.9 MeV; 2H(polarized n, n), E=10, 14.1 MeV; analyzed analyzing power data; deduced nucleon-nucleon interaction dependence.
doi: 10.1016/0168-583X(89)91023-9
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
1988HO14 Phys.Rev.Lett. 61, 1565 (1988) C.R.Howell, W.Tornow, I.Slaus, P.D.Felsher, M.L.Roberts, H.G.Pfutzner, Anli Li, K.Murphy, R.L.Walter, J.M.Lambert, P.A.Treado, H.Witala, W.Glockle, T.Cornelius Rigorous Calculations and Measurements of A(y)(θ) for n + d Elastic-Scattering and Breakup Processes NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured vector analyzing power vs θ. Three-nucleon calculations.
doi: 10.1103/PhysRevLett.61.1565
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
1988TO01 J.Phys.(London) G14, 49 (1988) W.Tornow, C.R.Howell, H.G.Pfutzner, M.L.Roberts, P.D.Felsher, Z.M.Chen, M.Al Ohali, G.J.Weisel, R.L.Walter, A.A.Naqvi Analysing Power for 12C(n(pol), n0, 1)12C and Evaluation of n-12C Scattering at 18.2 MeV NUCLEAR REACTIONS 12C(polarized n, n), (polarized n, n'), E=18.2 MeV; measured σ(θ), analyzing power vs θ; deduced reaction σ, 12C recoil kerma factors. Optical model, coupled channel, phase shift analyses.
doi: 10.1088/0305-4616/14/1/009
1988TO07 Phys.Rev. C37, 2326 (1988) W.Tornow, C.R.Howell, M.L.Roberts, P.D.Felsher, Z.M.Chen, R.L.Walter, G.Mertens, I.Slaus Low-Energy Neutron-Proton Analyzing Power and the New Bonn Potential and Paris Potential Predictions NUCLEAR REACTIONS 1H(polarized n, n), E=16.9 MeV; measured A(θ), backward angles. Instrumental effect corrections to published data, nucleon-nucleon calculations comparison. 2H(polarized d, n), E=14.1 MeV; measured A(θ), small angles.
doi: 10.1103/PhysRevC.37.2326
1987HO09 Few-Body Systems 2, 19 (1987) C.R.Howell, W.Tornow, K.Murphy, H.G.Pfutzner, M.L.Roberts, Anli Li, P.D.Felsher, R.L.Walter, I.Slaus, P.A.Treado, Y.Koike Comparisons of Vector Analyzing-Power Data and Calculations for Neutron-Deuteron Elastic Scattering from 10 to 14 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=10, 12, 14.1 MeV; measured analyzing powers vs θ. Polarized neutron facilities, other data input. Faddeev calculations.
doi: 10.1007/BF01078989
1987TO03 J.Phys.(London) G13, 177 (1987) The Level Structure of 13C around E(x) = 20 MeV Studied by Polarised Neutron Scattering from 12C NUCLEAR REACTIONS 12C(polarized n, n), E=15.55-17.35 MeV; measured analyzing power vs θ. 13C deduced levels, J, π. Phase shift analysis.
doi: 10.1088/0305-4616/13/2/007
1987TO07 Phys.Rev. C35, 1578 (1987) W.Tornow, C.R.Howell, H.G.Pfutzner, M.L.Roberts, P.D.Felsher, Z.M.Chen, R.L.Walter Search for a Purported Resonance in 13C at 20 MeV via Analyzing Power Measurements of 12C(n, n) NUCLEAR REACTIONS 12C(polarized n, n), E=15.6-16.5 MeV; measured σ(En), analyzing power vs E, θ. Compared to phase-shift prediction.
doi: 10.1103/PhysRevC.35.1578
1986DE17 Radiat.Eff. 94, 227 (1986) J.P.Delaroche, G.M.Honore, W.Tornow, R.L.Walter Coupled-Channel Analysis of Nucleon Scattering from 40Ca NUCLEAR REACTIONS 40Ca(polarized n, n), (polarized n, n'), E=10-17 MeV; measured σ(θ), A(θ); deduced potential parameter characteristics. Coupled-channels analysis, other data input.
doi: 10.1080/00337578608208380
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
1986MA38 Phys.Rev. C34, 384 (1986) Analyzing Power of 27Al(n(pol), n(pol)0) at 14 and 17 MeV and the Isospin Dependence of the Optical Model Potential NUCLEAR REACTIONS 27Al(polarized n, n), E=14, 17, 11 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters, isospin dependence, σ. 27Al(polarized p, p), E=19, 23 MeV; analyzed σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevC.34.384
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
1986WA29 Radiat.Eff. 95, 73 (1986) A Global Optical Model for Neutron Scattering for A > 53 and 10 MeV < E < 80 MeV NUCLEAR STRUCTURE A=54-208; calculated σ(θ), A(θ) for neutron scattering, E=10-80 MeV. Global optical model.
doi: 10.1080/00337578608208670
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
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
1983DE17 Phys.Rev. C27, 2385 (1983) J.P.Delaroche, P.P.Guss, C.E.Floyd, R.L.Walter, W.Tornow Sensitivity of Neutron Scattering Properties to the Coupling to Giant Resonances NUCLEAR REACTIONS 208Pb, 116,120Sn(polarized n, n), (polarized n, n'), E=10 MeV; 40Ca(polarized n, n), (polarized n, n'), E=12 MeV; analyzed σ(θ), analyzing power vs θ; deduced giant resonance coupling effects. Coupled-channels model.
doi: 10.1103/PhysRevC.27.2385
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
1982DA05 Nucl.Sci.Eng. 80, 388 (1982) J.H.Dave, C.R.Gould, L.W.Seagondollar, C.R.Howell, R.S.Pedroni, F.O.Purser, R.L.Walter Neutron Elastic and Inelastic Scattering Cross Sections for Carbon-13 between 10 and 18 MeV NUCLEAR REACTIONS 13C(n, n), (n, n'), E=10-18 MeV; measured σ(θ), σ(En). Legendre polynomial, optical model analyses.
doi: 10.13182/NSE82-A19823
1982DE45 Nucl.Phys. A390, 541 (1982) J.P.Delaroche, S.M.El-Kadi, P.P.Guss, C.E.Floyd, R.L.Walter Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. (II). Scattering and Nuclear Structure Effects from Coupled Channels Calculations NUCLEAR REACTIONS 54,56Fe, 63,65Cu(n, n), (n, n'), E=8, 10, 12, 14 MeV; measured σ(θ). 54,56Fe, 63,65Cu levels deduced deformation parameters. Coupled-channels calculations.
doi: 10.1016/0375-9474(82)90282-2
1982EL09 Nucl.Phys. A390, 509 (1982) S.M.El-Kadi, C.E.Nelson, F.O.Purser, R.L.Walter, A.Beyerle, C.R.Gould, L.W.Seagondollar Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. (I). Measurements from 8 to 14 MeV and a Spherical Optical Model Analysis NUCLEAR REACTIONS 54,56Fe, 63,65Cu(n, n), (n, n'), E=8, 10, 12, 14 MeV; measured σ(θ); deduced new spherical optical potential parameters. Compared to earlier global potential parametrizations.
doi: 10.1016/0375-9474(82)90281-0
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
1982GL02 Nucl.Sci.Eng. 80, 256 (1982) S.G.Glendinning, S.El-Kadi, C.E.Nelson, R.S.Pedroni, F.O.Purser, R.L.Walter, A.G.Beyerle, C.R.Gould, L.W.Seagondollar, P.Thambidurai Elastic and Inelastic Neutron Cross Sections for Boron-10 and Boron-11 NUCLEAR REACTIONS 10B(n, n), E=8-14 MeV; 11B(n, n), (n, n'), E=8, 9, 9.7, 9.9, 11-14 MeV; measured σ(θ); deduced integrated σ(E). Legendre polynomial analysis.
doi: 10.13182/NSE82-A21429
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
1976LI03 Nucl.Phys. A259, 61 (1976) P.W.Lisowski, T.C.Rhea, R.L.Walter, C.E.Busch, T.B.Clegg Scattering of Polarized Neutrons from 3He NUCLEAR REACTIONS 3He(polarized n, n), E=8.0, 12.0, 17.1 MeV; measured P(θ). 3He(n, n), 1 < E < 23.7 MeV; analyzed, parameterized σ(θ), P(θ), total σ in terms of complex phase shifts.
doi: 10.1016/0375-9474(76)90495-4
1976LI08 Nucl.Phys. A264, 188 (1976) P.W.Lisowski, R.L.Walter, C.E.Busch, T.B.Clegg Polarization Transfer Effects in (p, n) Reactions on Light Nuclei at θ = 0° NUCLEAR REACTIONS 9Be, 11B, 13C(polarized p, n), E=7-15 MeV; measured transverse polarization transfer coefficients.
doi: 10.1016/0375-9474(76)90427-9
1976LI15 Phys.Rev.Lett. 37, 809 (1976) P.W.Lisowski, R.L.Walter, G.G.Ohlsen, R.A.Hardekopf Reaction 3H(d, n)4He as a Calibrated Polarized Neutron Source and the Analyzing Power of 4He(n, n)4He from 20 to 30 MeV NUCLEAR REACTIONS 4He(polarized n, n), E=20-30 MeV; measured A(E, θ). 3H(d, n) calibrated polarized neutron source.
doi: 10.1103/PhysRevLett.37.809
1976OH02 Phys.Rev. C14, 1688 (1976) G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.V.Poore, R.L.Walter, P.W.Lisowski Polarized Triton Experiments on the Five-Nucleon System NUCLEAR REACTIONS 2H(polarized t, n), E=10.5 MeV; measured A(θ), polarization P(θ), polarization transfer coefficient. 2H(polarized t, n), E=5.4-15.7 MeV; measured polarization transfer coefficient. 2H(polarized t, t), E=10.5 MeV; measured A(θ).
doi: 10.1103/PhysRevC.14.1688
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
1975LI08 Nucl.Phys. A242, 298 (1975) P.W.Lisowski, R.L.Walter, C.E.Busch, T.B.Clegg Polarization Transfer in the 2H(d, n)3He Reaction at θ = 0° NUCLEAR REACTIONS 2H(d, n), 1 MeV < E < 15 MeV; measured transverse polarization transfer coefficient, tensor analyzing power A.
doi: 10.1016/0375-9474(75)90050-0
1973FE03 Z.Phys. 260, 271 (1973) M.Feil, W.von Oertzen, H.G.Bohlen, A.Gamp, R.L.Walter, B.Kohlmeyer Structures in the Excitation Functions for Compound Reactions in the 12C + 14C System NUCLEAR REACTIONS 14C(12C, 12C), (12C, α), (12C, t), (12C, d), E=Coulomb barrier;measured σ(E). 14C, 22,23,24Ne deduced levels.
doi: 10.1007/BF01396019
1973GA14 Z.Phys. 261, 283 (1973) A.Gamp, W.von Oertzen, H.G.Bohlen, M.Feil, R.L.Walter, N.Marquardt Elastic Scattering of 15N on 19F, 19F on 18O and 19F on 16O at Low Energies and Elastic Transfer NUCLEAR REACTIONS 16O(19F, 15N), (19F, 16O), (19F, 19F), (19F, 20Ne), 18O(19F, 18O), (19F, 19F), E=27-36 MeV; 19F(15N, 12C), (15N, 17O), (15N, 19F), E=23-29 MeV; measured σ(E(12C, 15N, 16O, 17O, 18O, 19F, 20Ne), θ). 16,18O, 19F, 20Ne deduced levels.
doi: 10.1007/BF01399327
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