Nuclear Science References (NSR)

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
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1994AR17 Phys.Rev. C50, 2480 (1994)

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
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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
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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
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1992AR01 Phys.Rev. C45, 759 (1992)

H.F.Arellano, W.G.Love

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
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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
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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
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1990AR03 Phys.Rev. C41, 2188 (1990); Erratum Phys.Rev. C42, 1782 (1990)

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
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1990AR11 Phys.Rev. C42, 652 (1990)

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
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1990BR22 Phys.Rev. C42, 2573 (1990)

F.A.Brieva, W.G.Love

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
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1989AR05 Phys.Rev.Lett. 63, 605 (1989)

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
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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
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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
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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
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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
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1988NA04 Phys.Rev. C38, 51 (1988)

K.Nakayama, W.G.Love

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
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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
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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
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1986KL01 Phys.Rev.Lett. 56, 700 (1986)

A.Klein, W.G.Love, M.A.Franey

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
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1986KL02 Phys.Rev. C33, 1920 (1986)

A.Klein, W.G.Love

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
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1985KL01 Phys.Rev. C31, 710 (1985)

A.Klein, W.G.Love, N.Auerbach

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
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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
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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
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1984LO04 Phys.Rev. C29, 2135 (1984)

W.G.Love, J.R.Comfort

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
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1984LO10 J.Phys.(Paris), Colloq.C4, 231 (1984); See 1984Lo20

W.G.Love, M.A.Franey

Effective Interactions and the Excitation of Giant Resonances

1984LO20 J.Phys.(Paris), Colloq.C-4, 231 (1984)

W.G.Love, M.A.Franey

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
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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
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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
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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
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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
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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
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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
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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
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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
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1981LO11 Phys.Rev. C24, 1073 (1981); Erratum Phys.Rev. C27, 438 (1983)

W.G.Love, M.A.Franey

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
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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
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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
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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
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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
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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
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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
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1980CO07 Phys.Rev.Lett. 44, 1656 (1980)

J.R.Comfort, W.G.Love

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1977SC26 Nucl.Phys. A289, 123 (1977)

A.Scott, M.Owais, W.G.Love

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
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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
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1975LO01 Nucl.Phys. A239, 74 (1975)

W.G.Love, L.W.Owen

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
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1975LO07 Phys.Rev.Lett. 35, 1219 (1975)

W.G.Love, F.T.Baker

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
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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
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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
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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
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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
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1972LO23 Phys.Lett. 42B, 13 (1972)

Multiple Excitation of the Second 0⁺ State in ⁹⁰Zr

doi: 10.1016/0370-2693(72)90702-2
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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
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1971LO24 Phys.Lett. 37B, 463 (1971)

W.G.Love, L.W.Owen

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
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1971SA18 Nucl.Phys. A172, 449 (1971)