NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = W.G.Love Found 84 matches. 2007AR20 Phys.Rev. C 76, 014616 (2007) In-medium full-folding model approach to quasielastic (p, n) charge-exchange reactions NUCLEAR REACTIONS 14C, 48Ca, 90Zr(p, n), E=120, 135 MeV; calculated σ and angular distributions using a coupled-channel extension of the full-folding optical model approach.
doi: 10.1103/PhysRevC.76.014616
2005AR16 Nucl.Phys. A755, 527c (2005) Nuclear halo structure from quasielastic charge-exchange reactions NUCLEAR REACTIONS 48Ca(p, n), E=160 MeV; calculated σ(θ), nuclear density dependence.
doi: 10.1016/j.nuclphysa.2005.03.069
2005NA33 Phys.Rev. C 72, 034603 (2005) Spin structure of spin-1/2 baryon and spinless meson production amplitudes in photonic and hadronic reactions
doi: 10.1103/PhysRevC.72.034603
2004NA23 Phys.Rev. C 70, 012201 (2004) Spin observables and the determination of the parity of Θ+ in photoproduction reaction NUCLEAR REACTIONS 1H(γ, X), E not given; calculated pentaquark production associated polarization observables.
doi: 10.1103/PhysRevC.70.012201
1997BB17 Phys.Rep. 289, 235 (1997) F.T.Baker, L.Bimbot, C.Djalali, C.Glashausser, H.Lenske, W.G.Love, M.Morlet, E.Tomasi-Gustafsson, J.Van de Wiele, J.Wambach, A.Willis The Nuclear Spin Response to Intermediate Energy Protons and Deuterons at Low Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319, 800 MeV; 12C(polarized p, p'), E=318 MeV; 12C, 40Ca(polarized d, d'), E=400 MeV; analyzed σ(E, θ), spin-tranfer observables; deduced collective effects, nuclear spin response related features.
doi: 10.1016/S0370-1573(97)00008-2
1995AR13 Phys.Rev. C52, 301 (1995) H.F.Arellano, F.A.Brieva, W.G.Love In-Medium Full-Folding Optical Model for Nucleon-Nucleus Elastic Scattering NUCLEAR REACTIONS 208Pb, 40Ca(polarized p, p), E=30.3-400 MeV; analyzed σ(θ), analyzing power, spin-rotation function vs θ. 40Ca, 90Zr, 208Pb(n, n), E=4-500 MeV; calculated σ(E). In-medium, full-folding optical model.
doi: 10.1103/PhysRevC.52.301
1994AR17 Phys.Rev. C50, 2480 (1994) H.F.Arellano, F.A.Brieva, W.G.Love Deuteron Effects in Nucleon-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=160-400 MeV; 208Pb(polarized p, p), E=98-400 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced medium effects, higher order corrections role. Full folding model.
doi: 10.1103/PhysRevC.50.2480
1994AU08 Phys.Rev.Lett. 73, 30 (1994) S.M.Austin, N.Anantaraman, W.G.Love Charge Exchange Reactions and the Efficiency of Solar Neutrino Detectors NUCLEAR REACTIONS 37Cl(p, n), E not given; calculated σ(q ≈ 0)/B(GT); deduced implications for solar ν problem.
doi: 10.1103/PhysRevLett.73.30
1994SA10 Phys.Rev. C49, 2254 (1994) Comment on ' Elastic Scattering of 318 MeV 6Li from 12C and 28Si: Unique phenomenological and folding-model potentials ' and the validity of the M3Y effective interaction NUCLEAR REACTIONS 12C(6Li, 6Li), E=210, 318 MeV; analyzed σ(θ) analyses; deduced optical potential, validity of M3Y folding interaction.
doi: 10.1103/PhysRevC.49.2254
1992AR01 Phys.Rev. C45, 759 (1992) Coulomb-Exchange Contribution to Proton-Nucleus Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=19.57-153 MeV; calculated σ(θ). 40Ca(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Momentum space calculations, Coulomb exchange contribution.
doi: 10.1103/PhysRevC.45.759
1991AR03 Phys.Rev. C43, 1875 (1991) H.F.Arellano, F.A.Brieva, W.G.Love, K.Nakayama Comparison of Nucleon-Nucleon Potential Models in a Full-Folding Description of Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300, 400 MeV; analyzed σ(θ), polarization observables data; deduced effective nucleon-nucleon potential dependence. Nonrelativistic full-folding model analysis.
doi: 10.1103/PhysRevC.43.1875
1991AR11 Phys.Rev. C43, 2734 (1991) H.F.Arellano, W.G.Love, F.A.Brieva Starting Energy Dependence of Elastic Scattering Observables in a Full-Folding Model NUCLEAR REACTIONS 16O(polarized p, p), E=135 MeV; 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), polarization observables; deduced starting energy dependence.
doi: 10.1103/PhysRevC.43.2734
1990AR03 Phys.Rev. C41, 2188 (1990); Erratum Phys.Rev. C42, 1782 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Nonrelativistic Full-Folding Model of Nucleon Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=400, 200 MeV; calculated σ(θ), analyzing power, spin-rotation parameter vs momentum transfer. Nonrelativistic full-folding optical potentials.
doi: 10.1103/PhysRevC.41.2188
1990AR11 Phys.Rev. C42, 652 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Role of Nuclear Densities in Nucleon Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 400 MeV; 16O(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced scattering observables sensitivity to density. Full-folding model.
doi: 10.1103/PhysRevC.42.652
1990BR22 Phys.Rev. C42, 2573 (1990) Nonlocal Couplings, Off-Shell Effects, and the Nuclear Response NUCLEAR REACTIONS 40Ca(polarized p, p'), E=100, 300 MeV; calculated inclusive σ, spin-flip probabilities, analyzing powers, σ(θp, Ep'); deduced nonlocal couplings, off-shell effects role. Interacting Fermi gas model.
doi: 10.1103/PhysRevC.42.2573
1989AR05 Phys.Rev.Lett. 63, 605 (1989) H.F.Arellano, F.A.Brieva, W.G.Love Full-Folding-Model Description of Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Full folding model analysis.
doi: 10.1103/PhysRevLett.63.605
1989BA55 Phys.Rev. C40, 1877 (1989) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, K.Jones, W.G.Love, S.Nanda Spin Dipole and Quadrupole Resonances in 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured absolute σ(θ). 40Ca deduced spin quadrupole resonance, spin-dipole strength distribution.
doi: 10.1103/PhysRevC.40.1877
1989BR17 Phys.Rev. C40, R475 (1989) F.P.Brady, T.D.Ford, J.L.Romero, C.M.Castaneda, J.R.Drummond, E.L.Hjort, N.S.P.King, B.McEachern, D.S.Sorenson, Z.Aung, A.Klein, W.G.Love, J.K.Wambach Gamow-Teller and Spin-Dipole Strength in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(θp, Ep). 90Y deduced Gamow-Teller, spin dipole transition strength.
doi: 10.1103/PhysRevC.40.R475
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
1989RA09 Phys.Rev. C39, 1929 (1989) J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).
doi: 10.1103/PhysRevC.39.1929
1988NA04 Phys.Rev. C38, 51 (1988) Effective Interaction for Nucleon-Nucleus Scattering Based on a One-Boson-Exchange Model NUCLEAR REACTIONS 90Zr(p, p), E=121.5 MeV; 12C(polarized p, p), E=200 MeV; 48Ca(polarized p, n), E=134 MeV; 28Si(p, p'), E=134 MeV; calculated σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevC.38.51
1987FO10 Phys.Lett. 195B, 311 (1987) T.D.Ford, J.L.Romero, F.P.Brady, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson, Zin Aung, N.S.P.King, A.Klein, W.G.Love Excitation of Isovector Monopole and Quadrupole Giant Resonances in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(E(p), θ(p)), σ(θ(p)). 90Y deduced isovector monopole, quadrupole giant resonances. RPA-DWA analyses.
doi: 10.1016/0370-2693(87)90023-2
1987LO13 Phys.Rev.Lett. 59, 1401 (1987) W.G.Love, K.Nakayama, M.A.Franey Isovector Couplings for Nucleon Charge-Exchange Reactions at Intermediate Energies NUCLEAR REACTIONS 14C(p, n), E=60-450 MeV; calculated σ(θ=0°) vs E; deduced nucleon-nucleon interaction isovector component features.
doi: 10.1103/PhysRevLett.59.1401
1986KL01 Phys.Rev.Lett. 56, 700 (1986) Antinucleon Charge-Exchange Reaction as a Probe of Longitudinal Spin Excitations NUCLEAR REACTIONS 90Zr(p-bar, n-bar), E=175 MeV; calculated σ; deduced longitudinal spin excitation probe selectivity. 90Zr(p-bar, p-bar'), E=175 MeV; calculated longitudinal, isovector transition potentials.
doi: 10.1103/PhysRevLett.56.700
1986KL02 Phys.Rev. C33, 1920 (1986) Polarization Transfer and Spin-Parity Composition of the Charge-Exchange Continuum NUCLEAR REACTIONS 90Zr(polarized p, n), E=120, 160, 500 MeV; 48,40Ca(polarized p, n), E=135 MeV; calculated transverse polarization coefficient, spin-flip σ(θ=0°); deduced natural parity spin-flip strength.
doi: 10.1103/PhysRevC.33.1920
1985KL01 Phys.Rev. C31, 710 (1985) Continuum Charge-Exchange Spectra and the Quenching of Gamow-Teller Strength NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(θ, En), θ<10°. 90Nb deduced Gamow-Teller transition strength characteristics. Charge exchange, Hartree-Fock RPA, Skyrme interaction.
doi: 10.1103/PhysRevC.31.710
1984AU10 Phys.Rev. C30, 736 (1984) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love Reply to '' Comment on ' (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances ' '' NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; calculated IAS, isovector monopole resonance excitation σ(θ=0°); deduced medium corrections role.
doi: 10.1103/PhysRevC.30.736
1984DO15 Phys.Lett. 143B, 45 (1984) C.B.Dover, M.A.Franey, W.G.Love, M.E.Sainio, G.E.Walker Antinucleon-Nucleus Inelastic Scattering and the Spin Dependence of the N(bar)N Annihilation Potential NUCLEAR REACTIONS 12C(p-bar, p-bar'), E=175 MeV; calculated σ(θ), polarization; deduced nucleon-antinucleon annihilation potential.
doi: 10.1016/0370-2693(84)90801-3
1984LO04 Phys.Rev. C29, 2135 (1984) Implications of Spin-Current Couplings for P ± A in Inelastic Proton Scattering NUCLEAR REACTIONS 90Zr(polarized p, p'), E=200 MeV; 12C(polarized p, p'), E=150 MeV; calculated polarization, analyzing power differences vs θ; deduced spin, current coupling role. DWIA.
doi: 10.1103/PhysRevC.29.2135
1984LO10 J.Phys.(Paris), Colloq.C4, 231 (1984); See 1984Lo20 Effective Interactions and the Excitation of Giant Resonances
1984LO20 J.Phys.(Paris), Colloq.C-4, 231 (1984) Effective Interactions and the Excitation of Giant Resonances NUCLEAR REACTIONS 12C(p, p'), E=120, 200, 398, 800 MeV; 208Pb(p, p'), E=135, 334, 800 MeV; 90Zr(p, p'), E=201 MeV; 90Zr(p, n), E=120 MeV; calculated σ(θ). Free nucleon-nucleon t-matrix.
1983AU05 Phys.Rev. C28, 280 (1983) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances NUCLEAR REACTIONS 90Zr, 40Ca, 120Sn, 208Pb(p, n), E=120, 800 MeV; calculated σ(θ) for isovector giant monopole resonance excitation. DWIA, RPA based charge exchange transition densities.
doi: 10.1103/PhysRevC.28.280
1983BA06 Nucl.Phys. A393, 283 (1983) F.T.Baker, A.Scott, M.A.Grimm, W.G.Love, V.Penumetcha, C.Glashausser, G.S.Adams, G.Igo, G.W.Hoffmann, J.M.Moss, W.Swenson, B.E.Wood The 90,92Zr(p(pol), p') Reactions at E(p) = 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(Ep', θ), σ(θ), Aθ, A(Ep', θ). Distorted wave analyses, collective, semimicroscopic-models, free nucleon-nucleon t-matrix. Enriched targets.
doi: 10.1016/0375-9474(83)90143-4
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
1982CA08 Phys.Rev.Lett. 49, 266 (1982) T.A.Carey, J.M.Moss, S.J.Seestrom-Morris, A.D.Bacher, D.W.Miller, H.Nann, C.Olmer, P.Schwandt, E.J.Stephenson, W.G.Love Polarization and Analyzing-Power Differences in the Excitation of 1+ States in 12C at 150 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=150 MeV; measured polarization, analyzing power difference vs θ. 12C level deduced transition density matrix elements. Q2DM magnetic spectrometer.
doi: 10.1103/PhysRevLett.49.266
1982CO21 Phys.Rev. C26, 1800 (1982) J.R.Comfort, G.L.Moake, C.C.Foster, P.Schwandt, W.G.Love Analysis of the 12C(p(pol), p')12C Reaction at 200 MeV in the Distorted-Wave Impulse Approximation NUCLEAR REACTIONS 12C(polarized p, p'), E=200 MeV; measured σ(Ep, θ), A(Ep, θ); deduced effective interaction role. 12C deduced transition characteristics, levels J, π, T. DWIA analysis.
doi: 10.1103/PhysRevC.26.1800
1982HA26 Phys.Rev. C25, 3035 (1982) M.Haji-Saeid, G.Igo, F.Irom, J.B.McClelland, G.Pauletta, C.A.Whitten, Jr., C.Glashausser, W.D.Cornelius, J.M.Moss, H.A.Thiessen, M.A.Franey, M.Gazzaly, W.G.Love Excitation of Low Spin States in the 12C(p, p') Reaction at 800 MeV NUCLEAR REACTIONS 12C(p, p'), E=0.8 GeV; measured σ(θ). DWIA, nucleon-nucleon t-matrix, shell model, electron scattering transition densities.
doi: 10.1103/PhysRevC.25.3035
1981BA54 Phys.Rev.Lett. 47, 1823 (1981) F.T.Baker, C.Glashausser, A.Scott, M.A.Grimm, G.S.Adams, G.Hoffmann, G.Igo, W.G.Love, J.M.Moss, S.Nanda, V.Penumetcha, W.Swenson, B.E.Wood Test of Data-to-Data Relations for the Reactions 90,92Zr(p(pol), p') at 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced data-to-data relation inadequacies.
doi: 10.1103/PhysRevLett.47.1823
1981CO10 Phys.Rev. C23, 1858 (1981) J.R.Comfort, R.E.Segel, G.L.Moake, D.W.Miller, W.G.Love 12C(p, p')12C Reaction at 155 and 200 MeV and Precritical Phenomena NUCLEAR REACTIONS 12C(p, p'), E=155 MeV; measured σ(Ep, θ); 12C(polarized p, p'), E=200 MeV; measured σ(Ep, θ), A(θ); deduced precritical phenomena implications. DWIA.
doi: 10.1103/PhysRevC.23.1858
1981CO20 Phys.Rev. C24, 1834 (1981) J.R.Comfort, G.L.Moake, C.C.Foster, P.Schwandt, C.D.Goodman, J.Rapaport, W.G.Love Analyzing Powers for the 12C(p(pol), p')12C Reaction at 120 MeV and a Test of the Distorted-Wave Impulse Approximation NUCLEAR REACTIONS 12C(polarized p, p'), E=120 MeV; measured σ(E, θ), A(θ). DWIA analysis.
doi: 10.1103/PhysRevC.24.1834
1981LO11 Phys.Rev. C24, 1073 (1981); Erratum Phys.Rev. C27, 438 (1983) Effective Nucleon-Nucleon Interaction for Scattering at Intermediate Energies NUCLEAR REACTIONS 12C(p, p'), E=120, 402, 800 MeV; 90Zr(p, n), E=120 MeV; 58Ni(p, p'), E=800 MeV; calculated σ(θ). On-shell nucleon-nucleon t-matrix, energy-dependent Yukawa representation.
doi: 10.1103/PhysRevC.24.1073
1981SC04 Nucl.Phys. A357, 9 (1981) A.Scott, F.T.Baker, W.G.Love, J.D.Wiggins, Jr., M.L.Whiten Comparison of the 92Mo(p, p') and 90Zr(p, p') Reactions at 61.2 MeV NUCLEAR REACTIONS 92Mo(p, p'), E=61.2 MeV; measured σ(Ep', θ). 90Zr(p, p'), E=61.2 MeV; analyzed σ(θ). 92Mo deduced levels, deformation parameter β(L). Isotopically enriched target.
doi: 10.1016/0375-9474(81)90623-0
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
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
1980CO05 Phys.Rev. C21, 2147 (1980) J.R.Comfort, S.M.Austin, P.T.Debevec, G.L.Moake, R.W.Finlay, W.G.Love Inelastic Excitation of 12C and 14N by 122 MeV Protons and Implications for the Effective Nucleon-Nucleon Interaction NUCLEAR REACTIONS 12C, 14N(p, p), (p, p'), E=122 MeV; measured σ(Ep, θ). 12C level deduced β2. DWIA analysis, spin-orbit tensor effective interaction. Exchange terms.
doi: 10.1103/PhysRevC.21.2147
1980CO07 Phys.Rev.Lett. 44, 1656 (1980) Evidence Regarding Precritical Phenomena in 12C NUCLEAR REACTIONS 12C(p, p'), E=122 MeV; calculated σ(θ). 12C level deduced no precritical behavior near pion condensation threshold. DWIA, exact knockon exchange term.
doi: 10.1103/PhysRevLett.44.1656
1980GO07 Phys.Rev.Lett. 44, 1755 (1980) C.D.Goodman, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, C.C.Foster, W.G.Love, F.Petrovich Gamow-Teller Matrix Elements from 0°(p, n) Cross Sections NUCLEAR REACTIONS 7Li, 12,13C, 25,26Mg, 27Al, 28Si, 90Zr(p, n), E=120 MeV; measured σ(θ=0°). 7Be, 12,13N, 25,26Al, 27Si, 28P, 90Nb deduced Gamow-Teller matrix elements.
doi: 10.1103/PhysRevLett.44.1755
1980HO21 Phys.Lett. B95, 27 (1980) D.J.Horen, C.D.Goodman, C.C.Foster, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, E.Sugarbaker, T.G.Masterson, F.Petrovich, W.G.Love Search for Isobaric Analogues of M1 States and Giant Spinflip Resonance NUCLEAR REACTIONS 208Pb(p, n), E=120, 160 MeV; measured σ(θ, En). 209Bi deduced resonances, Γ, J, π, analog M1 states, giant spinflip resonance. Tof, enriched target.
doi: 10.1016/0370-2693(80)90391-3
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
1980MO06 Phys.Rev.Lett. 44, 1189 (1980) J.M.Moss, C.Glashausser, F.T.Baker, R.Boudrie, W.D.Cornelius, N.Hintz, G.Hoffmann, G.Kyle, W.G.Love, A.Scott, H.A.Thiessen Excitation of Unnatural-Parity States in 12C by 800-MeV Polarized Protons NUCLEAR REACTIONS 12C(polarized p, p'), E=800 MeV; measured σ(θ), A(θ). 12C levels deduced T, J, π. DWIA analysis.
doi: 10.1103/PhysRevLett.44.1189
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
1980PE05 Phys.Rev. C21, 1718 (1980) F.Petrovich, W.G.Love, R.J.McCarthy Separation of Current and Spin Contributions to Isovector M1 Excitations by Means of the (e, e') and (p, n) Reactions NUCLEAR REACTIONS 12C, 24Mg, 28Si(p, n), E=62 MeV; calculated σ(θ), B(M1), transition radii. 12C, 24Mg, 28Si(e, e'), E not given; calculated orbital current densities. 12C, 24Mg, 28Si deduced current, spin contributions to T=1, M1 excitations. g-matrix, shell model, distorted, plane wave approximations.
doi: 10.1103/PhysRevC.21.1718
1980PE11 Phys.Lett. B95, 166 (1980) F.Petrovich, W.G.Love, A.Picklesimer, G.E.Walker, E.R.Siciliano Differences in the Structure of Isoscalar and Isovector Stretched Excitations in 24Mg and 28Si NUCLEAR REACTIONS 24Mg, 28Si(p, p'), E=135 MeV; analyzed σ(θ). 24Mg, 28Si levels deduced isospin dependence of S, stretched configurations.
doi: 10.1016/0370-2693(80)90461-X
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
1979AD03 Phys.Rev.Lett. 43, 421 (1979) G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.R.Smith, M.Gazzaly, L.Ray, W.G.Love, F.Petrovich Microscopic Description of 800-MeV Polarized-Proton Scattering from 16O NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), A(θ). Microscopic impulse approximation analysis.
doi: 10.1103/PhysRevLett.43.421
1979LI06 Phys.Rev.Lett. 42, 1524 (1979) R.A.Lindgren, W.J.Gerace, A.D.Bacher, W.G.Love, F.Petrovich Tensor Force and Inelastic Electron and Proton Scattering to Unnatural-Parity States of Stretched Configurations NUCLEAR STRUCTURE 12C, 16O, 24Mg, 28Si, 58Ni, 208Pb; analyzed(e, e'), (p, p') transitions involving unnatural parity states; deduced high-momentum components of tensor term of nucleon-nucleon force.
doi: 10.1103/PhysRevLett.42.1524
1979LO12 Phys.Rev. C20, 1638 (1979) Spin-Unsaturated Subshells and the Nucleon-Nucleus Optical-Model Spin-Orbit Potential NUCLEAR REACTIONS 12C(p, p), E=45.5 MeV; calculated A(θ). 28Si(p, p), E=30 MeV; calculated σ(θ), A(θ). 48Ca(p, p), E=30 MeV; calculated A(θ). Optical model, spin-orbit potential. Spin unsaturated shells.
doi: 10.1103/PhysRevC.20.1638
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
1978LO03 Phys.Rev. C17, 1876 (1978) Double-Folding Model Potential for Anomalous Large-Angle 4He + 40Ca Scattering NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.17.1876
1978LO15 Nucl.Phys. A312, 160 (1978) A Study of the Local Slater-Exchange Approximation for Nucleon and Heavy-Ion Scattering NUCLEAR REACTIONS 40Ca(n, n'), (p, p'), E=10-160 MeV; calculated σ(θ) using Slater-exchange approximation for nucleon-HI scattering.
doi: 10.1016/0375-9474(78)90582-1
1978SA23 Phys.Lett. 76B, 23 (1978) 6Li Scattering: A Failure of the Double-Folded Potential Model NUCLEAR REACTIONS 40,44Ca(6Li, 6Li), E=30 MeV; 40,48Ca(6Li, 6Li), E=28, 34 MeV; 90Zr(6Li, 6Li), E=34 MeV; 40Ca, 58Ni, 124Sn, 208Pb(6Li, 6Li), E=50.6 MeV; 58Ni(6Li, 6Li), E=22.8 MeV; 28Si(6Li, 6Li), E=135.1 MeV; calculated σ, normalization. Double-folded potential model.
doi: 10.1016/0370-2693(78)90089-8
1977BA49 Phys.Rev. C16, 1377 (1977); Erratum Phys.Rev. C17, 856 (1978) D.E.Bainum, R.W.Finlay, J.Rapaport, J.D.Carlson, W.G.Love Excitation of Low-Lying Collective States in 40Ca and 208Pb by Inelastic Neutron Scattering NUCLEAR REACTIONS 208Pb(n, n), (n, n'), E=11, 25.7 MeV; 40Ca(n, n), (n, n'), E=11, 20 MeV; measured σ(θ). 208Pb, 40Ca deduced β. Distorted wave analysis.
doi: 10.1103/PhysRevC.16.1377
1977BE26 Nucl.Phys. A284, 399 (1977) G.Bertsch, J.Borysowicz, H.McManus, W.G.Love Interactions for Inelastic Scattering Derived from Realistic Potentials NUCLEAR REACTIONS 208Pb, 40Ca(p, p'), E=35 MeV; calculated σ(θ). 14N(p, p'), E=23.7 MeV; 120Sn(polarized p, n), E=24.5 MeV; calculated asymmetry.
doi: 10.1016/0375-9474(77)90392-X
1977LO02 Phys.Rev. C15, 1261 (1977) Microscopic Description of Sn(p, n) Reactions NUCLEAR REACTIONS 112,116,124Sn(p, n), E=22.8 MeV; calculated σ(θ). 120Sn(polarized p, n), E=24.5 MeV; calculated A(θ).
doi: 10.1103/PhysRevC.15.1261
1977LO07 Phys.Rev.Lett. 39, 6 (1977) W.G.Love, T.Terasawa, G.R.Satchler Dynamic Polarization Potential for Coulomb Excitation Effects on Heavy-Ion Scattering NUCLEAR REACTIONS 184W(18O, 18O), E=90 MeV; 238U(40Ar, 40Ar), E=340 MeV; 209Bi(84Kr, 84Kr), E=600 MeV; 209Bi(136Xe, 136Xe), E=1130 MeV; calculated σ(θ). polarization potential.
doi: 10.1103/PhysRevLett.39.6
1977LO15 Nucl.Phys. A291, 183 (1977) W.G.Love, T.Terasawa, G.R.Satchler A Dynamic Polarization Potential for Heavy-Ion Scattering NUCLEAR REACTIONS 209Bi(136Xe, 136Xe), E=1130 MeV; 238U(40Ar, 40Ar), E=340 MeV; 209Bi(84Kr, 84Kr), E=600 MeV; 238U(α, α), E=24.7 MeV; 184W(18O, 18O), E=90 MeV; 152Sm(16O, 16O), E=72 MeV; 208Pb(20Ne, 20Ne), E=131 MeV; calculated plarization potential, effects due to Coulomb excitation, σ(θ).
doi: 10.1016/0375-9474(77)90205-6
1977SC26 Nucl.Phys. A289, 123 (1977) Excitation of Neutron-Hole States in 207Pb by Inelastic Scattering of 61 MeV Protons NUCLEAR REACTIONS 207Pb(p, p'), E=61.2 MeV; measured σ(Ep', θ). 207Pb deduced levels, β(L). Isotopically enriched target, 92.4%.
doi: 10.1016/0375-9474(77)90525-5
1976SA27 Phys.Lett. 65B, 415 (1976) A New Interaction for Heavy-Ion Scattering NUCLEAR REACTIONS 60Ni(16O, X); calculated potential.
doi: 10.1016/0370-2693(76)90432-9
1975LO01 Nucl.Phys. A239, 74 (1975) Exchange Effects from Realistic Interactions in the Reformulated Optical Model NUCLEAR REACTIONS 40Ca(p, p), E=20, 40, 60 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(75)91133-1
1975LO07 Phys.Rev.Lett. 35, 1219 (1975) Final-State Spin Dependence for Inelastic Scattering from Odd-A Nuclei NUCLEAR REACTIONS 63Cu(polarized p, p), (polarized d, d); calculated σ(θ), A(θ).
doi: 10.1103/PhysRevLett.35.1219
1974LO09 Nucl.Phys. A226, 319 (1974) On the Nuclear I . L Potential NUCLEAR REACTIONS 9Be, 59Co(α, α); calculated spin orbit potential.
doi: 10.1016/0375-9474(74)90408-4
1973FA12 Nucl.Phys. A212, 541 (1973) G.J.Faini, R.L.Ezell, E.L.Wills, H.L.Scott, W.G.Love The γ-Ray Decay Properties of Analogue States in 52Cr via the Reaction 51V(p, γ)52Cr NUCLEAR REACTIONS 51V(p, γ), E=745-820 keV; measured σ(E;Eγ), γ(θ). 52Cr deduced resonances, J, π, γ-multipolarities, γ-branching.
doi: 10.1016/0375-9474(73)90822-1
1973HI04 Phys.Rev. C7, 1981 (1973) R.A.Hinrichs, D.Larson, B.M.Preedom, W.G.Love, F.Petrovich 90Zr(p, p')90Zr* Reaction at 40 MeV NUCLEAR REACTIONS 90Zr(p, p'), E=40 MeV; measured σ(Ep', θ). Deduced L. 90Zr deduced levels, β(L).
doi: 10.1103/PhysRevC.7.1981
1972LO16 Nucl.Phys. A192, 49 (1972) The Two-Body Spin-Orbit Interaction in Inelastic Scattering NUCLEAR REACTIONS 90Zr(p, p'), E=61.2 MeV; analyzed σ(θ); deduced role of 2-body spin-orbit interaction.
doi: 10.1016/0375-9474(72)90004-8
1972LO23 Phys.Lett. 42B, 13 (1972) Multiple Excitation of the Second 0+ State in 90Zr
doi: 10.1016/0370-2693(72)90702-2
1971LO11 Phys.Lett. 35B, 371 (1971) Evidence for the Importance of the Nucleon-Nucleon Spin-Orbit Interaction in the Inelastic Excitation of High Spin States in 90Zr NUCLEAR REACTIONS 90Zr(p, p'), E = 61.2 MeV; calculated σ(θ). Microscopic calculation.
doi: 10.1016/0370-2693(71)90396-0
1971LO24 Phys.Lett. 37B, 463 (1971) One-Step Processes in the Inelastic Excitation of Unnatural Parity States by Alpha-Particles NUCLEAR REACTIONS 16O(α, α'), E=40, 65 MeV; 4He(p, p), E=1-20 MeV; calculated phase shifts, σ(θ). One-step process.
doi: 10.1016/0370-2693(71)90345-5
1971SA18 Nucl.Phys. A172, 449 (1971) A Generalized Core-Polarization Model for Inelastic Scattering NUCLEAR REACTIONS 89Y(p, p'), E=61 MeV; calculated σ(θ). Generalized core-polarization model.
doi: 10.1016/0375-9474(71)90037-6
1970LO13 Nucl.Phys. A157, 625 (1970) Tensor Force Formalism for Inelastic Scattering Charge Exchange and Knock-Out Reactions NUCLEAR REACTIONS 54Fe(p, n), E=40 MeV; 12C(p, p'), E=45.5 MeV; measured nothing; analyzed σ(θ). Tensor force formalism.
doi: 10.1016/0375-9474(70)90238-1
1970LO15 Nucl.Phys. A159, 1 (1970) Exchange Effects with a Realistic Interaction for Inelastic Scattering NUCLEAR REACTIONS 12C, 14N, 89Y, Zr, 90Zr, 207Pb(p, p'), 18O, 90Zr(p, n), E=11-61 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(70)90025-4
1969SC25 Nucl.Phys. A137, 445 (1969) Inelastic Scattering of 61 MeV Protons from 89Y and the Associated Reaction Mechanisms NUCLEAR REACTIONS 89Y(p, p'), E = 61.2 MeV; measured σ(Ep', θ). 89Y deduced levels, β(L).
doi: 10.1016/0375-9474(69)90119-5
1968BE54 Phys.Rev. 176, 1268(1968) W.Benenson, S.M.Austin, R.A.Paddock, W.G.Love Scattering of 24.5-MeV Protons from 89Y NUCLEAR REACTIONS 89Y(p, p'), E=24.5 MeV; measured σ(Ep', θ). 89Y deduced levels, J, π, L.
doi: 10.1103/PhysRev.176.1268
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