NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = W.P.Jones Found 64 matches. 1993KE03 Phys.Rev. C47, 2146 (1993) J.J.Kelly, B.S.Flanders, F.W.Hersman, J.H.Heisenberg, J.Calarco, J.P.Connelly, T.E.Milliman, A.Scott, F.T.Baker, V.Penumetcha, W.P.Jones, G.T.Emery, A.D.Bacher, C.Olmer, M.A.Grimm, M.L.Whiten Neutron Transition Densities from 88Sr(p, p') at E(p) = 200 MeV NUCLEAR REACTIONS 88Sr(polarized p, p'), (polarized p, p), E=200 MeV; measured σ(θ), analyzing power vs θ. 88Sr levels deduced neutron transition densities. Shell model comparison.
doi: 10.1103/PhysRevC.47.2146
1991DI03 Phys.Rev. C43, 1758 (1991) S.Dixit, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, C.E.Hyde-Wright, M.V.Hynes, M.A.Kovash, B.E.Norum, J.J.Kelly, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman, D.J.Millener Structure of 9Be from Proton Scattering at 180 MeV NUCLEAR REACTIONS 9Be(polarized p, p')E=180 MeV; measured proton spectra, σ(θ), analyzing power vs θ. 9Be deduced levels, possible J, π. Other data input. Shell model.
doi: 10.1103/PhysRevC.43.1758
1990CH23 Phys.Rev. C41, 2514 (1990) Q.Chen, J.J.Kelly, P.P.Singh, M.C.Radhakrishna, W.P.Jones, H.Nann Effective Interactions and Nuclear Structure Using 180 MeV Protons. II. 28Si(p, p') NUCLEAR REACTIONS 28Si(polarized p, p'), (polarized p, p), E=180 MeV; measured σ(Ep), σ(θ), analyzing power vs θ; analyzed (e, e') data; deduced density, mass dependences of effective interaction. 28Si levels deduced transition density parameters.
doi: 10.1103/PhysRevC.41.2514
1990KE03 Phys.Rev. C41, 2504 (1990) J.J.Kelly, J.M.Finn, W.Bertozzi, T.N.Buti, F.W.Hersman, C.Hyde-Wright, M.V.Hynes, M.A.Kovash, B.Murdock, P.Ulmer, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman Effective Interactions and Nuclear Structure Using 180 MeV Protons. I. 16O(p, p') NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=180 MeV; measured σ(θ), analyzing power vs θ; deduced density dependence of effective interaction. 16O levels deduced spectroscopic amplitudes.
doi: 10.1103/PhysRevC.41.2504
1990KE04 Phys.Rev. C41, 2525 (1990) J.J.Kelly, Q.Chen, P.P.Singh, M.C.Radhakrishna, W.P.Jones, H.Nann Effective Interactions and Nuclear Structure Using 180 MeV Protons. III. 30Si(p, p') NUCLEAR REACTIONS 30Si(polarized p, p), (polarized p, p'), E=180 MeV; measured σ(Ep), σ(θ), analyzing power vs θ; analyzed (e, e') data. 30Si levels deduced transition densities, Mn/Mp. NUCLEAR STRUCTURE 30Si; calculated neutron, proton transition densities. Shell model.
doi: 10.1103/PhysRevC.41.2525
1990SA27 Phys.Rev. C42, 922 (1990) S.K.Saha, W.W.Daehnick, S.A.Dytman, P.C.Li, J.G.Hardie, G.P.A.Berg, C.C.Foster, W.P.Jones, D.W.Miller, E.J.Stephenson 17O(d(pol), t)16O at 89 MeV; j dependence and particle-hole matrix elements NUCLEAR REACTIONS 17O(polarized d, t), E=89 MeV; measured σ(θ), σ(Et), analyzing power vs θ. 16O levels deduced L, j-transfer, spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.42.922
1990SE13 Nucl.Phys. A518, 536 (1990) A.Sethi, F.T.Baker, G.T.Emery, W.P.Jones, M.A.Grimm, Jr. 194,198Pt(p(pol), p') Reaction and the Interacting Boson Model NUCLEAR REACTIONS 194,198Pt(polarized p, p'), E=135 MeV; measured σ(θ, Ep'), analyzing power vs θ, Ep'. 194,198Pt levels deduced matrix elements. Coupled channels calculations, interacting boson model analysis with, without a g-boson. Polarized protons, enriched targets.
doi: 10.1016/0375-9474(90)90145-C
1989BA54 Nucl.Phys. A501, 546 (1989) F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten 192Os(p(pol), p') Reaction at 135 MeV NUCLEAR REACTIONS 192Os(polarized p, p'), E=134.5 MeV; measured σ(θ), analyzing power vs θ; deduced matrix elements for excitation of 4+ states. 192Os levels deduced deformation lengths. Enriched target. Coupled-channels analysis.
doi: 10.1016/0375-9474(89)90147-4
1989KE03 Phys.Rev. C39, 1222 (1989) J.J.Kelly, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, C.Hyde-Wright, M.V.Hynes, M.A.Kovash, B.Murdock, B.E.Norum, B.Pugh, F.N.Rad, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman, W.G.Love, J.A.Carr, F.Petrovich Density Dependence in the Two-Nucleon Effective Interaction at 135 MeV NUCLEAR REACTIONS 16O, 9Be(polarized p, p'), (polarized p, p), E=135 MeV; measured σ(θ), analyzing power vs θ. Local density approximation.
doi: 10.1103/PhysRevC.39.1222
1989RA22 Phys.Rev. C40, 1603 (1989) M.C.Radhakrishna, N.G.Puttaswamy, H.Nann, D.W.Miller, P.P.Singh, W.W.Jacobs, W.P.Jones, E.J.Stephenson Neutron Pickup Strength in 87Sr from the (p(pol), d) Reaction NUCLEAR REACTIONS 87Sr(polarized p, d), E=94.2, 91.8 MeV; measured σ(θ), analyzing power vs θ. 86Sr deduced levels, single particle strengths.
doi: 10.1103/PhysRevC.40.1603
1989SA13 Phys.Rev. C40, 39 (1989) S.K.Saha, W.W.Daehnick, S.A.Dytman, P.C.Li, J.G.Hardie, G.P.A.Berg, C.C.Foster, W.P.Jones, D.W.Miller, E.J.Stephenson 15N(d(pol), t)14N at 89 MeV, j Dependence and p-Shell Matrix Elements NUCLEAR REACTIONS 15N(polarized d, t), E=89 MeV; measured σ(Et), σ(θ), analyzing power vs θ, Et; deduced effective interaction. 14N deduced levels, J, π.
doi: 10.1103/PhysRevC.40.39
1989SE01 Phys.Rev. C39, 749 (1989) R.E.Segel, A.Amusa, D.F.Geesaman, R.D.Lawson, B.Zeidman, C.Olmer, A.D.Bacher, G.T.Emery, C.W.Glover, H.Nann, W.P.Jones, S.Y.van der Werf, R.A.Lindgren Fragmentation of High-Spin Particle-Hole States in 26Mg NUCLEAR REACTIONS 26Mg(polarized p, p'), E=135 MeV; measured σ(θ), A(θ). 26Mg deduced levels, J, π. 28Si deduced levels, J, π, isoscalar, isovector excitation amplitudes. Other data input.
doi: 10.1103/PhysRevC.39.749
1988CO05 Nucl.Phys. A481, 494 (1988) S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones The Spectroscopy of 13C by Inelastic Proton Scattering NUCLEAR REACTIONS 13C(p, p)(p, p'), E=135 MeV; 13C(polarized p, p)(polarized p, p'), E=119 MeV; measured σ(θ), A(θ). Optical model, DWA analyses, density-dependent t-matrices.
doi: 10.1016/0375-9474(88)90342-9
1988NA01 Phys.Rev. C37, 85 (1988) H.Nann, W.W.Jacobs, G.Cravens, A.D.Bacher, W.P.Jones, E.J.Stephenson, R.B.M.Mooy High-Spin States of (1f7/2)-2 Character in 56,58,60,62Co NUCLEAR REACTIONS, MECPD 60,64Ni(polarized d, α), E=79 MeV; measured σ(E, θ), analyzing power vs E, θ. 58,62Co deduced levels, J, π, (1f7/2)-2 transition strength. 56,60Co deduced (1f7/2)-2 transition strength.
doi: 10.1103/PhysRevC.37.85
1988RA01 Phys.Rev. C37, 66 (1988) M.C.Radhakrishna, N.G.Puttaswamy, H.Nann, J.D.Brown, W.W.Jacobs, W.P.Jones, D.W.Miller, P.P.Singh, E.J.Stephenson Proton Occupation Numbers in 206Pb from the (d(pol), 3He) Reaction NUCLEAR REACTIONS, MECPD 206Pb(polarized d, 3He), E=79.4 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 206Pb deduced proton orbital rms radii. 205Tl deduced levels, J, π, spectroscopic strengths. 208,206Pb deduced proton occupation probabilities. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1103/PhysRevC.37.66
1987AN04 Nucl.Phys. A468, 43 (1987) P.R.Andrews, B.M.Spicer, G.G.Shute, V.C.Officer, J.M.R.Wastell, H.Nann, Q.Li, A.D.Bacher, D.L.Friesel, W.P.Jones Spectroscopy of 14C from the 11B(α, p)14C Reaction at 118 MeV NUCLEAR REACTIONS 11B(α, p), E=118.1 MeV; measured σ(Ep), σ(θ); deduced model parameters. 14C deduced levels, J, π. DWBA calculations.
doi: 10.1016/0375-9474(87)90318-6
1987CU04 Nucl.Phys. A469, 445 (1987) V.R.Cupps, J.D.Brown, C.C.Foster, W.P.Jones, D.W.Miller, H.Nann, P.Schwandt, E.J.Stephenson, J.A.Tostevin The 116Sn(d, p)117Sn l = 0 Reaction Mechanism at Intermediate Energies NUCLEAR REACTIONS 116Sn(d, p), (polarized d, p), E=79.2 MeV; measured σ(θ), A(θ), P(θ); deduced reaction mechanism. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(87)90032-7
1987RE10 Nucl.Phys. A472, 1 (1987) K.Reiner, P.Grabmayr, G.J.Wagner, S.M.Banks, B.G.Lay, V.C.Officer, G.G.Shute, B.M.Spicer, C.W.Glover, W.P.Jones, D.W.Miller, H.Nann, E.J.Stephenson Deeply-Bound Hole States in 57Co and the Spreading of the 1d5/2 Hole Strength Distribution NUCLEAR REACTIONS, MECPD 58Ni(polarized d, 3He), E=80 MeV; measured σ(E(3He)), σ(θ), vector analyzing powers. 57Co deduced levels, J, π, d3/2-d5/2 hole strength distributions.
doi: 10.1016/0375-9474(87)90217-X
1987ST16 Nucl.Phys. A469, 467 (1987) E.J.Stephenson, V.R.Cupps, J.A.Tostevin, R.C.Johnson, J.D.Brown, C.C.Foster, W.P.Jones, D.W.Miller, H.Nann, P.Schwandt The Effects of Far-Side Dominance on the j-Dependence of the Medium Energy 116Sn(d, p)117Sn Reaction NUCLEAR REACTIONS 116Sn(d, p), (polarized d, p), E=79.2 meV; measured σ(E(p), θ), A(E(p), θ); deduced reaction mechanism. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(87)90033-9
1986AN30 Nucl.Phys. A459, 317 (1986) P.R.Andrews, G.G.Shute, B.M.Spicer, S.F.Collins, V.C.Officer, J.M.Wastell, H.Nann, D.W.Devins, Q.Li, W.P.Jones, C.Olmer, A.D.Bacher, G.T.Emery Location of Multiparticle-Multihole Strength in 16N via the 3-Particle Transfer Reaction 13C(α, p)16N at 118 MeV NUCLEAR REACTIONS 13C(α, p), E=118 MeV; measured σ(θ). 16N levels deduced J, π, multiparticle-multihole strength. DWBA analysis, microscopic form factors.
doi: 10.1016/0375-9474(86)90137-5
1986KE05 Phys.Lett. 169B, 157 (1986) J.Kelly, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, M.V.Hynes, C.Hyde-Wright, B.E.Norum, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman, J.A.Carr, F.Petrovich Neutron Transition Density for the Lowest 2+ State of 18O NUCLEAR REACTIONS 16,18O(p, p'), E=135 MeV; measured σ(θ). 18O level deduced neutron transition density.
doi: 10.1016/0370-2693(86)90641-6
1986MI01 Phys.Rev. C33, 22 (1986) D.W.Miller, J.D.Brown, D.L.Friesel, W.W.Jacobs, W.P.Jones, H.Nann, P.Pichardo, J.Q.Yang, P.W.F.Alons, J.J.Kraushaar Energy Dependence of 24Mg(p(pol), d) Cross Section and Analyzing-Power Measurements from 50 to 150 MeV NUCLEAR REACTIONS 24Mg(polarized p, d), E=49.2, 150.3 MeV; measured σ(θ), A(θ). 23Mg levels deduced spectroscopic factors, energy dependence. Enriched targets, detector telescope. Adiabatic distorted wave analysis.
doi: 10.1103/PhysRevC.33.22
1986ST06 Phys.Lett. 171B, 358 (1986) E.J.Stephenson, R.C.Johnson, J.A.Tostevin, V.R.Cupps, J.D.Brown, C.C.Foster, J.A.Gering, W.P.Jones, D.A.Low, D.W.Miller, H.Nann, C.Olmer, A.K.Opper, P.Schwandt, J.W.Seubert, S.W.Wissink Inplications of Far-Side Dominance for the Disagreement between Distorted Wave Theory and Well-Matched Intermediate Energy (d, p) Reactions NUCLEAR REACTIONS 116Sn(polarized d, p), E=90 MeV; analyzed σ(θ), analyzing power vs θ. 66Zn(polarized d, p), E=88.1 MeV; measured proton polarization vs θ; deduced far-side dominance insignificance.
doi: 10.1016/0370-2693(86)91420-6
1986VA02 Phys.Lett. 166B, 372 (1986) S.Y.Van Der Werf, N.Blasi, M.N.Harakeh, G.Wenes, A.D.Bacher, G.T.Emery, C.W.Glover, W.P.Jones, H.J.Karwowski, H.Nann, C.Olmer, P.Den Heijer, C.W.De Jager, H.De Vries, J.Ryckebusch, M.Waroquier High-Spin 1p-1h Configurations in 116Sn and Their Fragmentation as seen in the Reactions 116Sn(p(pol), p'), 116Sn(e, e'), 115In(He, d) and 115In(α, t) NUCLEAR REACTIONS 116Sn(polarized p, p'), E=133.8 MeV; measured σ(θ), σ(Ep'), A(θ). 116Sn(e, e'), E=350 MeV; measured σ(E(e)), form factors. 115In(α, t), E=65 MeV; 115In(3He, d), E=50 MeV; measured σ(Et), σ(Ed). 116Sn deduced levels, J, π, L, stretched configuration fragmentation, transition amplitudes. DWBA analysis, shell model comparison.
doi: 10.1016/0370-2693(86)91582-0
1985BA64 Phys.Rev. C32, 2212 (1985) F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten g Bosons and the Third 4+ State in 192Os NUCLEAR REACTIONS 192Os(polarized p, p'), E=135 MeV; measured σ(Ep'), σ(θ). 192Os deduced 4+ states, reduced matrix elements, intruder characteristics.
doi: 10.1103/PhysRevC.32.2212
1985DI12 Nucl.Phys. A441, 189 (1985) S.A.Dickey, J.J.Kraushaar, J.R.Shepard, D.W.Miller, W.W.Jacobs, W.P.Jones The 54Fe(p(pol), d)53Fe and 140Ce(p(pol), d)139Ce Reactions at 122 MeV NUCLEAR REACTIONS 54Fe, 140Ce(polarized p, d), E=121 MeV; measured σ(θ), A(θ). 53Fe, 139Ce levels deduced spectroscopic factors. DWBA analysis. Enriched targets.
doi: 10.1016/0375-9474(85)90029-6
1985NA06 Phys.Rev.Lett. 55, 578 (1985) H.Nann, W.W.Jacobs, J.D.Brown, G.T.Emery, W.P.Jones, E.J.Stephenson Proton Ground-State Correlations in 48Ca NUCLEAR REACTIONS 48Ca(polarized d, α), E=79.4 MeV; measured σ(θ), analyzing power vs θ. 48Ca level deduced large f7/2 proton occupation number. 46K deduced levels, J, π, configuration. DWBA analysis.
doi: 10.1103/PhysRevLett.55.578
1984AL21 Phys.Lett. 145B, 34 (1984) P.W.F.Alons, J.J.Kraushaar, D.W.Miller, J.D.Brown, D.L.Friesel, W.W.Jacobs, W.P.Jones, H.Nann The 24Mg(p, d) Reaction to the (1/2)+ State at 2.36 MeV at Proton Energies from 27 to 185 MeV NUCLEAR REACTIONS 24Mg(p, d), E=27.3-185 MeV; measured σ(θ). 24Mg(polarized p, d), E=49.2-150.3 MeV; measured analyzing power vs θ; deduced optical model parameters. 25Mg levels deduced C2S. Exact finite-range DWBA.
doi: 10.1016/0370-2693(84)90942-0
1984AM04 Nucl.Phys. A413, 255 (1984) K.Amos, W.Bauhoff, I.Morrison, S.F.Collins, R.S.Henderson, B.M.Spicer, G.G.Shute, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones Microscopic and Macroscopic Aspects of 135 MeV Proton Scattering from 16O NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; measured σ(θ). 16O deduced level, tentative J, π. Optical model, DWBA analyses, collective, shell model wave functions, density-dependent t-matricies.
doi: 10.1016/0375-9474(84)90375-0
1984NA24 Phys.Rev. C30, 1509 (1984) H.Nann, W.W.Jacobs, A.D.Bacher, J.D.Brown, G.D.Cravens, G.T.Emery, W.P.Jones, E.J.Stephenson, B.A.Brown High-Spin ((πf7/2)2(νf7/2)-1) Configuration, Two-Particle - One-Hole States in 49Ti NUCLEAR REACTIONS 51V(polarized d, α), E=79.4 MeV; measured σ(θ), σ(Eα), analyzing power vs E, θ. 49Ti deduced levels, L, configurations. DWBA analysis.
doi: 10.1103/PhysRevC.30.1509
1984OL01 Phys.Rev. C29, 361 (1984) C.Olmer, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, H.Nann, P.Schwandt, S.Yen, T.E.Drake, R.J.Sobie Energy Dependence of Inelastic Proton Scattering to One-Particle One-Hole States in 28Si NUCLEAR REACTIONS 28Si(polarized p, p), (polarized p, p'), E=80, 100, 134, 180 MeV; measured σ(θ) vs E, analyzing power vs θ, E; deduced optical potential parameters, momentum transfer, energy dependences. DWIA analysis.
doi: 10.1103/PhysRevC.29.361
1983BA57 Nucl.Phys. A410, 180 (1983) W.Bauhoff, S.F.Collins, R.S.Henderson, G.G.Shute, B.M.Spicer, V.C.Officer, K.A.Amos, I.Morrison, D.W.Devins, D.L.Friesel, W.P.Jones Density-Dependent Forces and Large-Basis Structure Models in the Analyses of 12C(p, p') Reactions at 135 MeV NUCLEAR REACTIONS 12C(p, p'), (p, p), E=135 MeV; measured σ(θ). Optical model, DWBA analyses, density-dependent t-matrices.
doi: 10.1016/0375-9474(83)90198-7
1983KR02 Nucl.Phys. A394, 118 (1983) J.J.Kraushaar, J.R.Shepard, D.W.Miller, W.W.Jacobs, W.P.Jones, D.W.Devins The 13C(p(pol), d)12C and 208Pb(p(pol), d)207Pb Reactions at 123 MeV NUCLEAR REACTIONS 13C, 208Pb(polarized p, d), E=123 MeV; measured σ(θ), A(θ). 12C, 207Pb levels deduced S. DWBA analysis. Enriched targets.
doi: 10.1016/0375-9474(83)90165-3
1983NA01 Phys.Rev. C27, 1073 (1983) H.Nann, D.W.Miller, W.W.Jacobs, D.W.Devins, W.P.Jones, Li Qing-Li Systematics of (p(pol), d) Analyzing Powers at 94 MeV NUCLEAR REACTIONS 60Ni, 86Sr, 208Pb(polarized p, d), E=94 MeV; measured analyzing power vs θ; deduced optical model parameters, transferred nucleon j-dependence.
doi: 10.1103/PhysRevC.27.1073
1983NA09 Phys.Rev. C28, 642 (1983) H.Nann, D.W.Miller, W.W.Jacobs, D.W.Devins, W.P.Jones, A.G.M.van Hees 1f7/2 Neutron Hole Strength in 59Ni with the 60Ni(p(pol), d)59Ni Reaction at 94 MeV NUCLEAR REACTIONS 60Ni(polarized p, d), E=94 MeV; measured σ(Ed), σ(θ), analyzing power vs θ, Ed. 59Ni deduced levels, J, π, C2S. Enriched target. DWBA analysis, shell model comparison.
doi: 10.1103/PhysRevC.28.642
1983NA12 Nucl.Phys. A406, 81 (1983) H.Nann, W.W.Jacobs, A.D.Bacher, W.P.Jones, Li Qing-Li, E.J.Stephenson (f7/2)-27, 0 Configuration High-Spin States in 60Co Strongly Excited in the 62Ni(d(pol), α) Reaction NUCLEAR REACTIONS 62Ni(polarized d, α), E=78 MeV; measured σ(θ), A(θ). 60Co deduced levels, L, J, π. Enriched target.
doi: 10.1016/0375-9474(83)90285-3
1983SI13 Nucl.Phys. A405, 205 (1983) R.H.Siemssen, C.C.Foster, W.W.Jacobs, W.P.Jones, D.W.Miller, M.Saber, F.Soga Vector Analyzing Powers for Valence and Inner Shell Pickup in the 116Sn(d(pol), t)115Sn and 116Sn(d(pol), 3He)115In Reactions NUCLEAR REACTIONS 116Sn(polarized d, t), (polarized d, 3He), E=50 MeV; measured σ(E, θ), A(E, θ). 115Sn deduced valence, deeply bound hole states. 115In levels deduced J, π. DWBA analysis. Enriched targets, vector polarized beams.
doi: 10.1016/0375-9474(83)90568-7
1983ST06 Phys.Rev. C28, 134 (1983) E.J.Stephenson, J.C.Collins, C.C.Foster, D.L.Friesel, W.W.Jacobs, W.P.Jones, M.D.Kaitchuck, P.Schwandt, W.W.Daehnick Polarized Deuteron Elastic Scattering at 79 MeV and the Effects of Breakup Channel Coupling NUCLEAR REACTIONS 58Ni(polarized d, d), E=79 MeV; measured σ(θ), vector, tensor analyzing power vs θ. Folding model, deuteron breakup channel coupling.
doi: 10.1103/PhysRevC.28.134
1982BA38 Nucl.Phys. A386, 45 (1982) F.T.Baker, A.Scott, W.G.Love, J.A.Mowrey, W.P.Jones, J.D.Wiggins A Comparison of t-Matrix and G-Matrix Analyses for the 207Pb(p, p') Reaction at E(p) = 95 MeV NUCLEAR REACTIONS 207Pb(p, p'), E=95 MeV; measured σ(Ep', θ). 207Pb deduced levels, β(L). Semi-microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(82)90400-6
1982CO08 Nucl.Phys. A380, 445 (1982) S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, I.Morrison, K.A.Amos, D.W.Devins, D.L.Friesel, W.P.Jones A Study of the 13C(p, p') Reactions at 135 MeV NUCLEAR REACTIONS 13C(p, p), (p, p'), E=135 MeV; measured σ(θ). 13C levels deduced possible configuration. Optical model, DWBA analyses.
doi: 10.1016/0375-9474(82)90570-X
1982MI10 Phys.Rev. C26, 1793 (1982) D.W.Miller, W.W.Jacobs, D.W.Devins, W.P.Jones 24Mg(p(pol), d) Analyzing-Power Measurements at 95 MeV NUCLEAR REACTIONS 24Mg(polarized p, d), E=94.8 MeV; measured A(θ). 23Mg levels deduced J, π, deep hole configuration. Enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.26.1793
1982NA05 Phys.Lett. 109B, 175 (1982) H.Nann, W.W.Jacobs, A.D.Bacher, G.Cravens, W.P.Jones, E.J.Stephenson Spin Determinations from the 58Ni(d(pol), α)56Co Reaction at 80 MeV NUCLEAR REACTIONS 58Ni(polarized d, α), E=80 MeV; measured vector analyzing power vs θ. 56Co levels deduced J. Zero-range DWBA analysis.
doi: 10.1016/0370-2693(82)90747-X
1982RI05 Aust.J.Phys. 35, 9 (1982); Corrigendum Aust.J.Phys. 35, 351 (1982) L.Rikus, S.F.Collins, K.A.Amos, B.M.Spicer, G.G.Shute, I.Morrison, V.C.Officer, R.Smith, D.W.Devins, D.L.Friesel, W.P.Jones Excitation of the 9.50 MeV (9/2+) States of 13C in Intermediate Energy Scattering Experiments NUCLEAR REACTIONS 13C(p, p'), E=135 MeV; measured σ(θ). 13C state deduced total angular momentum transfer, configuration. Microscopic DWBA analysis.
1981BE06 Phys.Lett. 99B, 213 (1981) F.E.Bertrand, J.R.Beene, C.E.Bemis, Jr., E.E.Gross, D.J.Horen, J.R.Wu, W.P.Jones Measurement of the Fission Decay of the Giant Quadrupole Resonance in 238U NUCLEAR REACTIONS, Fission 238U(α, α'F), E=152 MeV; measured σ(Eα', θ), α(fragment)-coin, fission probability vs excitation energy. 238U deduced Γf/Γ for GQR, possible K conservation.
doi: 10.1016/0370-2693(81)91110-2
1981DE19 Phys.Rev. C24, 59 (1981) D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, I.D.Svalbe, R.S.Henderson, W.E.Dollhopf 40Ca(d, 3He)39K Reaction at 76 MeV NUCLEAR REACTIONS 40Ca(d, 3He), E=76 MeV; measured σ(θ, E(3He)). 39K deduced levels, J, π, L, C2S. Enriched targets. DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.24.59
1981HE21 Nucl.Phys. A372, 117 (1981) R.S.Henderson, S.F.Collins, B.M.Spicer, G.G.Shute, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones The Scattering of 136 MeV Protons from 6Li NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=136 MeV; measured σ(θ). Optical model, DWBA analyses.
doi: 10.1016/0375-9474(81)90090-7
1981NA13 Phys.Rev. C24, 1984 (1981) H.Nann, A.D.Bacher, W.W.Jacobs, W.P.Jones, E.J.Stephenson High-Spin States in 56,58Co with the 58,60Ni(d, α)56,58Co Reaction NUCLEAR REACTIONS 58,60Ni(d, α), E=80 MeV; measured σ(θ). 56,58Co levels deduced L, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.24.1984
1981SC11 Nucl.Phys. A366, 91 (1981) A.Scott, F.T.Baker, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. 207Pb(p, p') Measurements at 135 and 61 MeV, the Effective Interaction and Core Polarization NUCLEAR REACTIONS 207Pb(p, p'), E=134.8 MeV; measured σ(Ep', θ). 207Pb deduced levels, deformation β(L). Enriched target. Microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(81)90489-9
1981SI07 Phys.Lett. 103B, 323 (1981) R.H.Siemssen, W.P.Jones, W.W.Jacobs, C.C.Foster, D.W.Miller, M.Saber, F.Soga On the 'Missing' Deep-Hole Strength in 115Sn NUCLEAR REACTIONS 116Sn(d, t), E=50 MeV; measured σ(Et, θ). 115Sn deduced gross structure peaks, ΣC2S, L, 1g9/2, 2p1/2, 2p3/2, 1f5/2 subshell strength. Enriched target. DWBA calculations.
doi: 10.1016/0370-2693(81)90234-3
1981WU02 Phys.Rev. C24, 500 (1981) J.R.Wu, J.R.Beene, C.E.Bemis, Jr., F.E.Bertrand, E.E.Gross, D.J.Horen, W.P.Jones Fission Probability of 239U at High Excitation Measured with the 238U(α, 3Hef) Reaction NUCLEAR REACTIONS, Fission 238U(α, 3HeF), E=152 MeV; measured σ(θ(3He), E(3He)), σ(θ(3He), E(3He), fragment θ), 3He(fragment)(fragment)-coin; deduced reaction mechanism. 239U deduced fission probability vs excitation energy.
doi: 10.1103/PhysRevC.24.500
1981YE01 Phys.Lett. 105B, 421 (1981) S.Yen, R.J.Sobie, T.E.Drake, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, C.Olmer, P.Schwandt, W.G.Love, F.Petrovich Analyzing Powers for the Proton Excitation of High-Spin States in 28Si: A new look at the effective interaction NUCLEAR REACTIONS 28Si(polarized p, p'), E=135 MeV; measured σ(θ), analyzing power vs θ; deduced effective interaction characteristics. DWIA.
doi: 10.1016/0370-2693(81)91196-5
1980AD01 Phys.Lett. 91B, 23 (1980) G.S.Adams, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, W.G.Love, F.Petrovich Inelastic Excitation of Normal Parity Levels in 208Pb by 135 MeV Protons NUCLEAR REACTIONS 208Pb(p, p'), E=135.2 MeV; measured σ(θ). DWBA analysis, deformed spin-orbit term.
doi: 10.1016/0370-2693(80)90653-X
1980BA46 Phys.Lett. B97, 58 (1980) A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, G.S.Adams, F.Petrovich, W.G.Love Excitation of High-Spin Unnatural Parity States in 208Pb from the (p, p') Reaction at 135 MeV NUCLEAR REACTIONS 208Pb(p, p'), E=135 MeV; measured σ(Ep, θ). 208Pb deduced levels, J, π, configuration. DWIA, configuration mixing effects.
doi: 10.1016/0370-2693(80)90546-8
1980BE50 Phys.Rev. C22, 1832 (1980) F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles NUCLEAR REACTIONS 208Pb, 120Sn, 90Zr, 58Ni, 46Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). 46Ti, 58Ni, 90Zr, 120Sn, 208Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.
doi: 10.1103/PhysRevC.22.1832
1980KE14 Phys.Rev.Lett. 45, 2012 (1980) J.Kelly, W.Bertozzi, T.N.Buti, F.W.Hersman, C.Hyde, M.V.Hynes, B.Norum, F.N.Rad, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman, W.G.Love, F.Petrovich Signatures of Density Dependence in the Two-Nucleon Effective Interaction near 150 MeV NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; 12C(p, p'), E=122, 185 MeV; 40Ca(p, p'), E=185 MeV; analyzed σ(θ), polarization P(θ); deduced effective two-nucleon interaction density dependence. Distorted wave approximation, effective interaction averaged potentials.
doi: 10.1103/PhysRevLett.45.2012
1980PE02 Phys.Lett. 91B, 27 (1980) F.Petrovich, W.G.Love, G.S.Adams, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller Microscopic Description of Normal Parity Excitations in the 208Pb(p, p') Reaction at 135 MeV and the Shape of the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 208Pb(p, p'), E=135 MeV; calculated σ(θ); deduced shape of nucleon-nucleon interaction. Microscopic DWIA, central, spin-orbit interactions.
doi: 10.1016/0370-2693(80)90654-1
1980SC21 Phys.Rev.Lett. 45, 1315 (1980) A.Scott, F.T.Baker, M.A.Grimm, Jr., J.H.Johnson, V.Penumetcha, R.C.Styles, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. Shapes of Measured (p(pol), p') Analyzing Powers at 160 MeV for Proton States in 90Zr and Neutron States in 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p'), E=160 MeV; measured analyzing power vs θ; deduced spin-orbit potential parameters. 90,92Zr levels deduced configurations, β. DWIA, free nucleon-nucleon t-matrix.
doi: 10.1103/PhysRevLett.45.1315
1979DE35 Aust.J.Phys. 32, 323 (1979) D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, I.D.Svalbe, V.C.Officer, R.S.Henderson, B.M.Spicer, G.G.Shute The 12C(p, 2p)11B Reaction at 100 MeV NUCLEAR REACTIONS 12C(p, 2p), E=100 MeV; measured pp-coin, pp(θ). 11B levels deduced excitation mechanism. Symmetric, asymmetric geometry. DWIA calculations.
doi: 10.1071/PH790323
1979HE09 Aust.J.Phys. 32, 411 (1979) R.S.Henderson, B.M.Spicer, I.D.Svalbe, V.C.Officer, G.G.Shute, D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard 4- Particle-Hole States in 16O NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; measured σ(Ep, θ). 16O levels deduced J, π, T, configuration. QDDM spectrograph.
doi: 10.1071/PH790411
1979MI15 Phys.Rev. C20, 2008 (1979) D.W.Miller, W.P.Jones, D.W.Devins, R.E.Marrs, J.Kehayias Hole States Excited by the 24Mg(p, d)23Mg Reaction at 95 MeV NUCLEAR REACTIONS 24Mg(p, d), E=94.8 MeV; measured σ(θ). 23Mg levels deduced L, J, π, S. DWBA analysis.
doi: 10.1103/PhysRevC.20.2008
1978LO01 Phys.Lett. 73B, 277 (1978) W.G.Love, A.Scott, F.T.Baker, W.P.Jones, J.D.Wiggins, Jr. A Test of the DWIA at 135 MeV Using the 207Pb(p, p') Reaction NUCLEAR REACTIONS 207Pb(p, p'), E=135 MeV; calculted σ(θ).
doi: 10.1016/0370-2693(78)90513-0
1978RO09 Phys.Rev.Lett. 40, 1439 (1978) P.G.Roos, N.S.Chant, D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, R.S.Henderson, I.D.Svalbe, B.M.Spicer, V.C.Officer, G.G.Shute Experimental Test of the Factorization Approximation in the Reaction 40Ca(p, 2p)39K at 148.2 MeV NUCLEAR REACTIONS 40Ca(p, 2p), E=148.2 MeV; measured σ. 39K levels deduced S. DWIA analysis.
doi: 10.1103/PhysRevLett.40.1439
1977AD04 Phys.Rev.Lett. 38, 1387 (1977) G.S.Adams, A.D.Bacher, G.T.Emery, W.P.Jones, R.T.Kouzes, D.W.Miller, A.Picklesimer, G.E.Walker Excitation of High-Spin 'Particle-Hole' States in 28Si and 24Mg by Inelastic Proton Scattering at Large Momentum Transfer NUCLEAR REACTIONS 24Mg, 28Si(p, p'), E=135 MeV; measured σ(Ep', θ). 24Mg, 28Si deduced resonances, J, π, T.
doi: 10.1103/PhysRevLett.38.1387
1971JO16 Phys.Rev. C4, 580 (1971) W.P.Jones, L.W.Borgman, K.T.Hecht, J.Bardwick, W.C.Parkinson Nuclear Structure of the N = 82 Isotones NUCLEAR REACTIONS 139La, 140Ce, 141Pr(3He, d), (d, 3He), E=44, 29 MeV; measured σ(Ed, θ), σ(E(3He), θ(3He)). 138Ba, 139La, 140Ce, 141Pr, 142Nd deduced levels, L(p), S.
doi: 10.1103/PhysRevC.4.580
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