NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.J.Thompson Found 46 matches. 2001IL02 Astrophys.J.Suppl.Ser. 134, 151 (2001) C.Iliadis, J.M.D'Auria, S.Starrfield, W.J.Thompson, M.Wiescher Proton-Induced Thermonuclear Reaction Rates for A = 20-40 Nuclei NUCLEAR REACTIONS 20,21,22Ne, 20,21,22,23Na, 22,23,24,25,26Mg, 23,24,25,26,27Al, 26,27,28,29,30Si, 27,28,29,30,31P, 30,31,32,33,34S, 31,32,33,34,35Cl, 34,35,36Ar, 35,36,37,38,39K, 39,40Ca(p, γ), E=low; 23Na, 27Al, 31P, 35Cl, 39K(p, α), E=low; compiled, analyzed astrophysical reaction rates.
doi: 10.1086/320364
1999IL01 Astrophys.J. 524, 434 (1999) C.Iliadis, P.M.Endt, N.Prantzos, W.J.Thompson Explosive Hydrogen Burning of 27Si, 31S, 35Ar, and 39Ca in Novae and X-Ray Bursts NUCLEAR REACTIONS 27Si, 31S, 35Ar, 39Ca(p, γ), E not given; calculated astrophysical reaction rates vs temperature.
doi: 10.1086/307778
1999TH03 Nucl.Phys. A647, 259 (1999) Error Analysis for Resonant Thermonuclear Reaction Rates NUCLEAR REACTIONS 32S, 39Ca(p, γ), E not given; analyzed resonance data; deduced reaction rates, uncertainties. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(98)00617-4
1993CR01 Phys.Rev. C47, 2690 (1993) E.R.Crosson, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos Probing α-Particle Wave Functions Using (d(pol), α) Reactions NUCLEAR REACTIONS 50Ti, 58Ni(polarized d, α), E=16, 22 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced α-particle D-state role. Exact finite-range DWBA analysis.
doi: 10.1103/PhysRevC.47.2690
1992BO14 Phys.Rev. C45, 2824 (1992) J.E.Bowsher, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson, J.A.Tostevin Effects of 6Li Excitation in 64Zn(d(pol), 6Li)60Ni at Low Energies NUCLEAR REACTIONS 64Zn(polarized d, 6Li), E=16.4 MeV; measured σ(θ), analyzing power vs θ; deduced 6Li levels role in reaction mechanism, model parameters. Vector, tensor polarized beam. Finite-range, coupled-channel Born approximation analysis.
doi: 10.1103/PhysRevC.45.2824
1992CR01 Phys.Rev. C45, R492 (1992) E.R.Crosson, R.K.Das, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos Probing α-Particle Wave Functions by (d, α) Tensor Analyzing Powers NUCLEAR REACTIONS 58Ni(polarized d, α), E=22 MeV; 50Ti(polarized d, α), E=16 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 4He deduced D-state parameters. DWBA analysis, realistic interactions.
doi: 10.1103/PhysRevC.45.R492
1992WI13 Nucl.Phys. A549, 223 (1992) J.F.Wilkerson, T.M.Mooney, R.E.Fauber, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson Isospin-Nonconserving Particle Decays in Light Nuclei NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar(polarized p, p), E ≈ resonance; 23Na, 31P(polarized p, p), (polarized p, α), 24Mg, 28Si(α, α), 20Ne(polarized p, p), E=6.4-7.7 MeV; measured σ(θ, E), analyzing power vs E, θ; deduced σ(E). 13N, 17F, 24Na, 25Al, 29P, 33S, 37K, 24Mg, 32S, 28Si deduced resonance parameters, isospin-nonconservation probabilities. Enriched targets, ion-implanted targets, polarized and unpolarized beams.
doi: 10.1016/0375-9474(92)90041-H
1991VA14 Phys.Rep. 201, 57 (1991) R.L.Varner, W.J.Thompson, T.L.McAbee, E.J.Ludwig, T.B.Clegg A Global Nucleon Optical Model Potenital
doi: 10.1016/0370-1573(91)90039-O
1990MC03 Nucl.Phys. A509, 39 (1990) T.L.McAbee, W.J.Thompson, H.Ohnishi Spin-Spin Interactions in Nucleon-Nucleus Scattering NUCLEAR REACTIONS 27Al, 59Co, 93Nb(n, n), E=10-60 MeV; calculated spin-spin σ(E). DWBA, nucleon-nucleus spin-spin interactions.
doi: 10.1016/0375-9474(90)90375-V
1987VA01 Phys.Lett. 185B, 6 (1987) R.L.Varner, T.B.Clegg, T.L.McAbee, W.J.Thompson Global Parameterization of the Nucleon-Nucleus Scattering Potential NUCLEAR REACTIONS 40Ca, 54Fe, 58,60Ni, 65Cu, 116,120Sn, 208Pb(n, n), (polarized n, n), E=10-26 MeV; 114,112Cd, 116,118,120,122Sn(p, p), (polarized p, p), E=16-65 MeV; 60,62,64Ni, 89Y, 90Zr(p, p), (polarized p, p), E=65 MeV; analyzed σ(θ), analyzing power data; deduced new optical potential parameters.
doi: 10.1016/0370-2693(87)91518-8
1984BU23 Phys.Rev. C30, 742 (1984) B.L.Burks, R.E.Anderson, Y.Aoki, B.C.Karp, E.J.Ludwig, W.J.Thompson, R.L.Varner 81Kr-81Br Ground-State Mass Difference and Implications for Calibration of a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 82Kr(d, t), (d, 3He), E=17 MeV; measured σ(Et), σ(E(3He)); deduced Q-value difference. 81Kr, 81Br deduced mass difference.
doi: 10.1103/PhysRevC.30.742
1984KA33 Phys.Rev.Lett. 53, 1619 (1984) B.C.Karp, E.J.Ludwig, W.J.Thompson, F.D.Santos α-Particle D-State Components from (d, α) Analyzing Powers NUCLEAR REACTIONS 89Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), analyzing power vs θ. 4He deduced D-state parameter. Exact finite-range DWBA analysis.
doi: 10.1103/PhysRevLett.53.1619
1983WI15 Phys.Rev.Lett. 51, 2269 (1983) J.F.Wilkerson, R.E.Anderson, T.B.Clegg, E.J.Ludwig, W.J.Thompson Isospin and Isobar Components in Light Nuclei NUCLEAR REACTIONS 28Si(polarized p, p), E=8.011-8.026 MeV; measured σ(θ), A(θ). 29P levels deduced proton isospin-mixing amplitudes. Other data analysis.
doi: 10.1103/PhysRevLett.51.2269
1981WI03 Nucl.Phys. A362, 8 (1981) J.E.Willis, T.B.Clegg, M.D.Kaitchuk, E.J.Ludwig, W.J.Thompson A Polarized Beam Study of the 207Pb(d, t)206Pb Reaction NUCLEAR REACTIONS 207Pb(polarized d, t), E=15 MeV; measured σ(θ), A(θ). 206Pb levels deduced L, J, π, S. Enriched target, DWBA analysis.
doi: 10.1016/0375-9474(81)90667-9
1980HA08 Phys.Rev. C21, 906 (1980) R.A.Hardekopf, R.F.Haglund, Jr., G.G.Ohlsen, W.J.Thompson, L.R.Veeser Polarized Triton Elastic Scattering at 17 MeV NUCLEAR REACTIONS 40Ca, 46Ti, 48Ti, 54,56Fe, 58,60Ni, 68Zn, 90,94Zr, 116Sn, 140Ce, 208Pb(polarized t, t), E =17 MeV; measured σ(θ), Ay(θ). Optical-model analysis.
doi: 10.1103/PhysRevC.21.906
1980TH05 Phys.Rev.Lett. 45, 703 (1980) W.J.Thompson, J.F.Wilkerson, T.B.Clegg, J.M.Feagin, E.J.Ludwig, E.Merzbacher Atomic-Excitation Effects on Nuclear Reactions NUCLEAR REACTIONS 12C(polarized p, p), E=14.226-14.236 MeV; measured σ(E, θ), analyzing power vs E, θ. 13N resonance deduced Γ, Γp, atomic excitation effects.
doi: 10.1103/PhysRevLett.45.703
1979FE02 Phys.Lett. 81B, 107 (1979) J.M.Feagin, E.Merzbacher, W.J.Thompson Q Values of β+-Decay, (p, n) and (3He, t) Reactions NUCLEAR STRUCTURE 10C, 14O, 26Al, 34Cl, 38K, 42Sc, 46V, 50Mn, 54Co; calculated effects of atomic excitation on Q in superallowed β+ decay, Q in (p, n), (3He, t) leading to these nuclei.
doi: 10.1016/0370-2693(79)90499-4
1977EC03 Phys.Rev. C16, 1020 (1977) J.S.Eck, D.O.Elliott, W.J.Thompson, F.T.Baker Nuclear Shapes of 24Mg and 28Si by Inelastic Scattering of 12C and 16,18O NUCLEAR REACTIONS 28Si, 24Mg(12C, 12C), (12C, 12C'), E=25, 30 MeV; 24Mg(16O, 16O), (16O, 16O'), 28Si(18O, 18O), (18O, 18O'), E=36 MeV; 28Si(16O, 16O), (16O, 16O'), E=33, 36, 38 MeV; measured σ(θ); deduced optical model parameters. 24Mg, 28Si deduced β.
doi: 10.1103/PhysRevC.16.1020
1977TH03 Phys.Lett. 67B, 151 (1977) Potential and Charge Deformations in Light Nuclei NUCLEAR STRUCTURE 12C, 20Ne, 24Mg, 28Si; analyzed quadrupole, hexadecapole potential deformations, electromagnetic moments.
doi: 10.1016/0370-2693(77)90089-2
1976HA28 Phys.Rev.Lett. 37, 553 (1976) R.F.Haglund, Jr., J.M.Bowen, W.J.Thompson Run Tests as Predictors of Intermediate Structure in the Continuum NUCLEAR REACTIONS 26Mg(polarized p, p), E=5-10 MeV; calculated A(E).
doi: 10.1103/PhysRevLett.37.553
1976IK01 Phys.Rev.Lett. 36, 1357 (1976) P.G.Ikossi, W.J.Thompson, T.B.Clegg, W.W.Jacobs, E.J.Ludwig Systematics of Isospin Mixing in Proton Elastic Scattering from Light Nuclei NUCLEAR REACTIONS 24Mg, 28Si, 32S(p, p); measured σ(E). 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca deduced systematics of isospin mixing in elastic p-scattering.
doi: 10.1103/PhysRevLett.36.1357
1976IK03 Nucl.Phys. A274, 1 (1976); Erratum Nucl.Phys. A279, 532 (1977) P.G.Ikossi, T.B.Clegg, W.W.Jacobs, E.J.Ludwig, W.J.Thompson Isospin-Forbidden T=3/2 Resonances in 25Al, 29P and 33Cl, and the Systematics of Isospin Mixing NUCLEAR REACTIONS 24Mg(p, p), E=5.65-6.25 MeV; 32S(polarized p, p), E=3-3.8 MeV; 28Si(polarized p, p), E=5.6-5.9 MeV; measured σ(E, θ), A(E, θ); deduced optical model parameters. 33Cl, 29P, 25Al, 21Na deduced resonance parameters, reduced widths. Enriched targts, polarized, unpolarized beams.
doi: 10.1016/0375-9474(76)90223-2
1976TH06 Phys.Lett. 62B, 245 (1976) Compound-Nucleus Effects in Nucleon Depolarization NUCLEAR REACTIONS 14N(polarized p, p), E=16.15 MeV; analyzed depolarization.
doi: 10.1016/0370-2693(76)90065-4
1976TH16 Phys.Lett. 65B, 309 (1976) Compound-Nucleus Effects in Spin-Spin Cross Sections NUCLEAR REACTIONS 59Co(polarized n, n), E < 3 MeV; calculated low energy region spin-spin σ.
doi: 10.1016/0370-2693(76)90228-8
1975EC01 Nucl.Phys. A237, 83 (1975) The Proton Optical-Model Potential Near the Coulomb Barrier NUCLEAR REACTIONS 197Au(p, p), E=10, 11 MeV; 209Bi, 208Pb(p, p), E=11-14 MeV; measured σ(θ); deduced optical-model parameters. 209Bi, 208Pb deduced energy dependence of real volume depth.
doi: 10.1016/0375-9474(75)90464-9
1975EC03 Phys.Rev.Lett. 35, 973 (1975) J.S.Eck, J.H.Johnson, D.O.Elliott, W.J.Thompson Optical-Model Analysis of N + C and C + C Elastic Scattering NUCLEAR REACTIONS 12C(14N, 14N), E=15.0-25.0 MeV; measured σ(E, θ).
doi: 10.1103/PhysRevLett.35.973
1975EC04 Nucl.Phys. A255, 157 (1975) J.S.Eck, W.J.Thompson, K.A.Eberhard, J.Schiele, W.Trombik Systematics of Backward-Angle Elastic Alpha Scattering NUCLEAR REACTIONS 32,34S, 36,38,40Ar, 39,41K, 40,42,44,48Ca, 48,50Ti, 51V, 50Cr, 56,58Fe, 59Co, 58,60,62,64Ni, 63,65Cu, 64,66,68,70Zn, 90Zr(α, α), E=15-40 MeV; calculated backward-angle enhancement.
doi: 10.1016/0375-9474(75)90155-4
1974IK01 Nucl.Phys. A225, 481 (1974) P.G.Ikossi, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson A Study of Isobaric Analogue Resonances in 71Ga NUCLEAR REACTIONS 70Zn(polarized p, p), E=3.6-6.4 MeV; measured σ(E, θ), A(E, θ). 71Ga deduced resonances, J, π, level-width, S.
doi: 10.1016/0375-9474(74)90355-8
1974TR06 Phys.Rev.Lett. 33, 229 (1974) T.A.Trainor, T.B.Clegg, W.J.Thompson Isospin-Forbidden Proton Partial Width in 41Sc and Similar A = 4n + 1 Nuclei NUCLEAR REACTIONS 40Ca(polarized p, p), (p, p), E=4975-4981 keV; measured σ(E, θ), A(E, θ). 41Sc deduced J, π, p-width, resonances.
doi: 10.1103/PhysRevLett.33.229
1973DA26 Phys.Rev.Lett. 31, 949 (1973) S.K.Datta, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson Comparison of Vector Analyzing Powers in (d, d) with Those (d, 3He) and (d, t) l = 0 Transfer Reactions NUCLEAR REACTIONS 14N, 30Si(polarized d, t), (polarized d, d), 32S(polarized d, d), (polarized d, 3He), E=15 MeV; measured analyzing power A(θ).
doi: 10.1103/PhysRevLett.31.949
1973ED02 Phys.Rev. C8, 456 (1973) S.Edwards, D.Robson, T.L.Talley, W.J.Thompson, M.F.Werby Multi-Interaction, Finite-Range, Two-Mode, DWBA Analyses of Direct Nuclear Reactions NUCLEAR REACTIONS 2H(α, t), E=82 MeV; 9Be(p, α), E=6 MeV; 6Li(3He, p), E=17 MeV; measured nothing, calculated σ(θ), level-width.
doi: 10.1103/PhysRevC.8.456
1973IK04 Bull.Am.Phys.Soc. 18, 254, BB10 (1973), See Keyno. 1973IKZY P.G.Ikossi, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson Cross Sections and Polarizations for Isobaric Analog Resonances in 71Ga
1973MC08 Nucl.Phys. A204, 321 (1973) G.S.McNeilly, W.J.Thompson, W.I.Van Rij, N.P.Heydenburg Reaction Mechanism Studies in 24Mg(α, α'γ)24Mg NUCLEAR REACTIONS 24Mg(α, α'γ), E=16.65 MeV; measured reaction-plane double differential cross sections. DWBA plus Hauser-Feshbach, coupled-channels plus Hauser-Feshbach analyses of (α, α1γ). Thick enriched target.
doi: 10.1016/0375-9474(73)90276-5
1973VO02 Nucl.Phys. A204, 529 (1973); Erratum Nucl.Phys. A217, 628 (1973) H.J.Votava, T.B.Clegg, E.J.Ludwig, W.J.Thompson Proton Scattering from 9Be between 6 and 30 MeV and the Structure of 9Be NUCLEAR REACTIONS 9Be(p, p0), (p, p2); measured σ(θ), E=13.0, 14.0, 15.0, 21.35, 30.3 MeV; measured vector polarization analyzing power A(θ), E=8.0, 11.0, 12.0, 13.0, 15.0 MeV; measured σ(E, θ), θ(lab)=86.9°, 120°, 140°, 160°, 6 < E < 15 MeV. 9Be(p, d0)8Be; measured σ(θ), E=13.0, 14.0, 15.0, 21.35, 30.3 MeV; measured A(θ), E=8.0, 11.0, 12.0, 13.0, 15.0 MeV. Natural target. 9Be deduced deformation parameter.
doi: 10.1016/0375-9474(73)90393-X
1972AH06 Nucl.Phys. A191, 137 (1972) C.E.Ahlfeld, G.E.Assousa, R.A.Lasalle, W.J.Thompson, H.A.Van Rinsvelt, N.P.Heydenburg Angular Correlation Studies for α-Particle Excitation of the 1.78 MeV 2+ State in 28Si NUCLEAR REACTIONS 28Si(α, α1γ), E=10, 12, 14, 18 MeV; measured in-plane correlations αγ(θ). 28Si(α, α'), E=18 MeV; measured σ(E, θ). 28Si deduced deformation parameter. Natural target.
doi: 10.1016/0375-9474(72)90598-2
1972AS03 Nucl.Phys. A182, 193 (1972) G.E.Assousa, C.E.Ahlfeld, R.A.LaSalle, W.I.Van Rij, H.A.Van Rinsvelt, W.J.Thompson, N.P.Heydenburg Reaction-Plane and Spin-Flip Angular Correlations in the Reactions 12C(tau, tau1γ4. 43)12C and 12C(→, α1γ4. 43)12C NUCLEAR REACTIONS 12C(3He, 3He'γ)12C, E=17 MeV; measured reaction-plane, 90° correlations; spin-flip probability extracted; coupled-channels analysis. 12C(α, α'γ)12C, E=19 MeV; measured reaction-plane correlations.
doi: 10.1016/0375-9474(72)90210-2
1972TH18 Part.Nucl. 4, 38 (1972) Cluster Effects in Elastic a Scattering Using a New α-α Interaction NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; analyzed cluster effects.
1972VO17 Phys.Lett. 41B, 405 (1972) Excited-State-Threshold Resonance Effects in 9Be(p, p0)9Be and 9Be(p, n)9B NUCLEAR REACTIONS 9Be(p, p), (p, n), E=6-8 MeV; analyzed σ(E); deduced excited state-threshold resonance effects. 10B deduced resonance parameters.
doi: 10.1016/0370-2693(72)90661-2
1971LU13 Part.Nucl.2, 107 (1971) E.J.Ludwig, W.J.Thompson, H.J.Votava Nuclear Scattering Potentials for Composite Projectiles
1971TH16 Particles and Nuclei 2, 47 (1971) On α-Cluster Effects in Elastic α Scattering from Nuclei Near A = 40 NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; calculated σ(θ); examined α-cluster effects.
1971WE07 Nucl.Phys. A169, 81 (1971) M.F.Werby, S.Edwards, W.J.Thompson Optical Model Analysis of 9Be(p, p0)9Be Cross Sections and Polarizations from 6 MeV to 30 MeV NUCLEAR REACTIONS 9Be(p, p), E=6-30 MeV; measured nothing; analyzed σ(E;θ), P(E;θ); deduced optical model parameters.
doi: 10.1016/0375-9474(71)90561-6
1970HE21 Nucl.Phys. A151, 33 (1970) W.R.Hering, H.Becker, C.A.Wiedner, W.J.Thompson Experimental Determination of the Normalization for (α, t) Reactions and Comparison with the Theoretical Normalization Factor NUCLEAR REACTIONS 205Tl(α, t), E=20-25 MeV; measured absolute σ(E;Et, θ). 206Pb ground state deduced reaction normalization, S. Enriched target.
doi: 10.1016/0375-9474(70)90965-6
1968HA07 Nucl.Phys. A109, 329(1968) O.Hausser, A.Richter, W.Von Witsch, W.J.Thompson Direct and Compound Nuclear Reaction Mechanisms in 26Mg(p, p)26Mg NUCLEAR REACTIONS 26Mg(p, p'), E=8.3-14 MeV; measured σ(E;Ep', θ); deduced direct reaction contribution. 27Al levels deduced level-width, cross-, auto-correlations. Enriched target.
doi: 10.1016/0375-9474(68)90597-6
1968TH07 Phys.Rev. 173, 975 (1968); Erratum Phys.Rev. C7, 1273 (1973) W.J.Thompson, J.L.Adams, D.Robson Neutron Spectroscopic Factors from Isobaric Analog States NUCLEAR REACTIONS 90Zr(p, p), E=5.7-7.0 MeV; 92Zr(p, p), (p, n), E=5.8-6.3 MeV; measured σ(E). 91,93Nb deduced isobar analog resonances, level-width, spreading widths.
doi: 10.1103/PhysRev.173.975
1967TH03 Nucl.Phys. A98, 228(1967) W.J.Thompson, G.E.Crawford, R.H.Davis Ambiguities in the Optical-Model Analysis of Alpha-Particle Scattering NUCLEAR REACTIONS 24Mg(α, α), (α, α'), E=10.8 MeV; measured σ(θ); deduced optical model parameters. Reanalysis of data.
doi: 10.1016/0375-9474(67)90136-4
1967TH06 Nucl.Phys. A105, 678(1967) W.J.Thompson, S.Edwards, T.Tamura Coupled Channel Analysis of Proton Scattering from 19F NUCLEAR REACTIONS 19F(p, p), 19F(p, p') E=4.26, 5.96, 6.87 MeV; measured σ(Ep, θ), σ(Ep', θ).
doi: 10.1016/0375-9474(67)90544-1
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