NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.Weisel Found 29 matches. 2015WE07 J.Phys.(London) G42, 085106 (2015) G.J.Weisel, W.Tornow, J.H.Esterline Neutron-deuteron analyzing power data at En = 21 MeV and the energy dependence of the three-nucleon analyzing power puzzle NUCLEAR REACTIONS 2H(polarized n, n), E<30 meV; measured reaction products, En, In; deduced n-d analyzing power. Comparison with Faddeev calculations.
doi: 10.1088/0954-3899/42/8/085106
2014WE04 Phys.Rev. C 89, 054001 (2014) G.J.Weisel, W.Tornow, A.S.Crowell, J.H.Esterline, G.M.Hale, C.R.Howell, P.D.O'Malley, J.R.Tompkins, H.Witala Neutron-deuteron analyzing power data at En = 22.5 MeV NUCLEAR REACTIONS 2H(polarized n, n), [polarized neutrons from 2H(polarized d, n) reaction], E=22.5 MeV; measured E(n), I(n), n-d analyzing power Ay(θ) using ABPIS facility at TUNL. Monte-Carlo simulations. Comparison with Faddeev calculations using several different NN potentials. Discussed three-nucleon analyzing power puzzle.
doi: 10.1103/PhysRevC.89.054001
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
2010WE06 Phys.Rev. C 82, 027001 (2010) G.J.Weisel, R.T.Braun, W.Tornow Corrections for the polarization-dependent efficiency and new neutron-proton analyzing power data at 7.6 MeV NUCLEAR REACTIONS 1H(polarized n, p), E=7.6-12 MeV; analyzed Ay(θ) data using fits to analyzing power data, phase-shift analysis and R-matrix analysis. 2H; deduced polarization-dependent efficiency (PDE) correction; 12C(polarized n, n), E=7.6-12 MeV; deduced a new database.
doi: 10.1103/PhysRevC.82.027001
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
2008TO12 J.Phys.(London) G35, 125104 (2008) W.Tornow, J.H.Esterline, G.J.Weisel Energy dependence of the three-nucleon analyzing power puzzle NUCLEAR REACTIONS 2H(p, p), E < 40 MeV; analyzed energy dependence of analyzing powers.
doi: 10.1088/0954-3899/35/12/125104
2007TO16 Nucl.Phys. A790, 64c (2007) W.Tornow, J.H.Esterline, G.J.Weisel Some recent few-body activities at Tunl NUCLEAR REACTIONS 2H(n, n), E=14-50 MeV; 3He(n, n), E=2.26-5.54 MeV; calculated analyzing powers. R-Matrix and 3N calculations. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.166
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
2003TO20 Phys.Lett. B 574, 8 (2003) W.Tornow, N.G.Czakon, C.R.Howell, A.Hutcheson, J.H.Kelley, V.N.Litvinenko, S.F.Mikhailov, I.V.Pinayev, G.J.Weisel, H.Witala Low-energy photodisintegration of the deuteron and Big-Bang Nucleosynthesis NUCLEAR REACTIONS 2H(polarized γ, np), E=2.39-4.05 MeV; measured En, Ep, photon analyzing power; deduced M1 contribution to total σ. Implications for Big-Bang nucleosynthesis discussed.
doi: 10.1016/j.physletb.2003.08.078
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
2003TO33 Mod.Phys.Lett. A 18, 282 (2003) W.Tornow, N.G.Czakon, C.R.Howell, A.Hutcheson, J.H.Kelley, V.N.Litvinenko, S.Mikhailov, I.V.Pinayev, G.J.Weisel, H.Witala Analyzing power for the photodisintegration of the deuteron between Eγ = 2.4 and 4.0 MeV NUCLEAR REACTIONS 2H(polarized γ, n), E=2.39-4.05 MeV; measured analyzing power. Comparison with model predictions.
doi: 10.1142/S021773230301034X
2000VA25 J.Phys.(London) G26, 1787 (2000) J.M.VanderKam, G.J.Weisel, W.Tornow Analytical Solution of Dispersion Relations for the Nuclear Optical Model
doi: 10.1088/0954-3899/26/12/303
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
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
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
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
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
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
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.
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
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