NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = R.E.Brown Found 98 matches. 1992KO18 Phys.Rev. C46, 2554 (1992) D.D.Koetke, R.Fisk, D.S.Koetke, R.Manweiler, T.J.Bowles, A.Brown, R.E.Brown, R.L.Burman, D.A.Clark, S.Clearwater, T.Dombeck, H.Kruse, D.Lee, B.Aas, G.Igo, C.Newsom, D.Beavis, S.Y.Fung, W.Gorn, R.T.Poe, G.J.VanDalen, B.Bassalleck, B.Dieterle, C.Gregory, R.E.Hill, J.H.Kang, C.Leavitt, L.Auerbach, S.Datta, Y.Huang Muon-Neutrino Carbon Charged-Current Interaction Near the Muon Threshold NUCLEAR REACTIONS 12C(ν, μ-X), 12C(ν, μ-), E ≈ 202 MeV; measured average σ(E).
doi: 10.1103/PhysRevC.46.2554
1990BR04 Phys.Rev. C41, 1391 (1990) Differential Cross Sections at Low Energies for 2H(d, p)3H and 2H(d, n)3He NUCLEAR REACTIONS, ICPND 2H(d, n), (d, p), E=20-117 keV; measured σ(E, θ); deduced σ(E), astrophysical S-factor vs E. Analytical, R-matrix fits.
doi: 10.1103/PhysRevC.41.1391
1987BR02 Phys.Rev. C35, 383 (1987) R.E.Brown, F.D.Correll, P.M.Hegland, J.A.Koepke, C.H.Poppe 3He + 3He Reaction Cross Sections at 17.9, 21.7, and 24.0 MeV NUCLEAR REACTIONS, ICPND 3He(3He, 2p), (3He, pd), (3He, 3p), (3He, n2p), (3He, 2pd), (3He, X), E=17.9, 21.7, 24 MeV; measured σ. Enriched gas target, three-detector telescope.
doi: 10.1103/PhysRevC.35.383
1987BR10 Phys.Rev. C35, 1999 (1987); Erratum Phys.Rev. C36, 1220 (1987) Fusion-Energy Reaction 3H(d, α)n at Low Energies NUCLEAR REACTIONS, ICPND 3H(d, α), E=80-116 keV; measured σ(E); deduced astrophysical S-factor vs E. 5He deduced resonances, Γα, Γd. Flowing gas target, Si surface barrier detectors.
doi: 10.1103/PhysRevC.35.1999
1987CI06 Phys.Rev. C36, 822 (1987) J.A.Cizewski, D.G.Burke, R.E.Brown, J.W.Sunier Ir(t(pol), α)Os Reaction and Implications for Tests of Supersymmetries NUCLEAR REACTIONS 191,193Ir(polarized t, α), E=17 MeV; measured σ(θ), analyzing powers. 190,192Os levels deduced population mechanism, possible supersymmetry model inadequancies. Enriched targets. DWBA calculations.
doi: 10.1103/PhysRevC.36.822
1987CO34 Nucl.Phys. A475, 407 (1987) F.D.Correll, R.E.Brown, G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, P.Doleschall Study of the Reaction H(d(pol), 2p)n at 16 MeV Around Collinear Configurations NUCLEAR REACTIONS, MECPD 1H(polarized d, 2p), E=16 MeV; measured σ(E(p3), θ(p3), E(p4), θ(p4)), analyzing powers vs arc length. Three-body Faddeev analysis.
doi: 10.1016/0375-9474(87)90071-6
1987HA20 Phys.Rev.Lett. 59, 763 (1987) Pole Structure of the J(π) = (3/2)+ Resonance in 5He NUCLEAR REACTIONS 3H(d, d), E(cm) ≤ 100 keV; calculated S-matrix amplitudes; deduced S-matrix poles. 5He deduced resonance, parameters Γ, Γn, Γd. R-matrix.
doi: 10.1103/PhysRevLett.59.763
1987HA44 Phys.Rev.Lett. 59, 2819 (1987) Hale, Brown, and Jarmie Reply:
doi: 10.1103/PhysRevLett.59.2819
1986BR20 Radiat.Eff. 92, 45 (1986) Hydrogen Fusion-Energy Reactions NUCLEAR REACTIONS, ICPND 2H(t, α), E=12.5-117 keV; measured σ; deduced astrophysical S-factor vs E. 2H(d, n), (d, p), E ≤ 125 keV; measured S-factor, anisotropy vs E. 3H(t, α), E ≤ 120 keV; measured σ(Eα); deduced astrophysical S-factor vs E.
doi: 10.1080/00337578608208295
1986DA15 Phys.Rev. C34, 815 (1986) W.W.Daehnick, R.E.Brown, E.R.Flynn, R.A.Hardekopf, J.C.Peng Analyzing Powers for 207Pb(t(pol), p)209Pb at 17 MeV as Evidence for Multistep Contributions NUCLEAR REACTIONS 207Pb(polarized t, p), E=17 MeV; measured σ(Ep), σ(θ), A(θ); deduced reaction mechanism, model parameters. 209Pb levels deduced L, transfer j, spectroscopic amplitudes, σ. DWBA analysis.
doi: 10.1103/PhysRevC.34.815
1986HA24 Nucl.Phys. A455, 494 (1986) J.S.Hanspal, K.I.Pearce, N.M.Clarke, R.J.Griffiths, R.E.Brown, R.A.Hardekopf, W.Gruebler The Interaction of 17 MeV Polarised Tritons with 30Si NUCLEAR REACTIONS 30Si(polarized t, t), (polarized t, t'), (polarized t, d), (polarized t, α), E=17 MeV; measured σ(θ), A(θ). 30Si deduced deformation parameters. 31Si, 29Al levels deduced spectroscopic factors. Optical model, CCBA, DWBA analyses.
doi: 10.1016/0375-9474(86)90319-2
1986MO05 Phys.Rev. C33, 1224 (1986) G.L.Morgan, P.W.Lisowski, S.A.Wender, R.E.Brown, N.Jarmie, J.F.Wilkerson, D.M.Drake Measurement of the Branching Ratio 3H(d, γ)/3H(d, n) using Thick Tritium Gas Targets NUCLEAR REACTIONS, ICPND 3H(d, γ), (d, n), E=0.0-0.72 MeV; measured Eγ, Iγ, En, relative γ yield. 5He resonance deduced branching ratio.
doi: 10.1103/PhysRevC.33.1224
1985AJ02 Phys.Rev. C31, 777 (1985) F.Ajzenberg-Selove, R.E.Brown, E.R.Flynn, J.W.Sunier (t, 3He) Reactions on 56Fe, 58Fe, and 58Ni NUCLEAR REACTIONS 56,58Fe, 58Ni(t, 3He), E=25 MeV; measured σ(Et), σ(θ). 56,58Mn, 58Co deduced levels, J, π. Coupled-channels calculations.
doi: 10.1103/PhysRevC.31.777
1985AJ03 Phys.Rev. C32, 756 (1985) F.Ajzenberg-Selove, R.E.Brown, E.R.Flynn, J.W.Sunier (t, 3He) Reactions on 40,42,44Ca, 46,48,50Ti, 54Cr, and 54Fe NUCLEAR REACTIONS 40,42,44Ca, 46,48,50Ti, 54Cr, 54Fe(t, 3He), E=25 MeV; measured σ(θ), σ(E(3He)). 40,42,44K, 46,48,50Sc, 54V, 54Mn deduced levels, J, π. CCBA analysis.
doi: 10.1103/PhysRevC.32.756
1985BR33 Nucl.Instrum.Methods Phys.Res. B10/11, 356 (1985) R.E.Brown, R.A.Hardekopf, N.Jarmie, F.D.Correll, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, W.W.Jacobs, H.O.Meyer, E.J.Stephenson, J.Q.Yang, W.T.H.van Oers, P.Doleschall, J.A.Tjon Polarization in Three-Nucleon Breakup: Experiment and theory NUCLEAR REACTIONS 1H(polarized d, d), E=16, 79 MeV; measured vector analyzing power vs rotation angle. Faddeev formalism.
doi: 10.1016/0168-583X(85)90268-X
1985BU18 Nucl.Phys. A445, 70 (1985) D.G.Burke, W.F.Davidson, J.A.Cizewski, R.E.Brown, J.W.Sunier Two-Quasiproton States in 168Er Studied by the 169Tm(t(pol), α)168Er Reaction NUCLEAR REACTIONS 169Tm(polarized t, α), E=17 MeV; measured σ(θ), σ(E(α), θ). 168Er deduced levels, J, π, K, two-quasiparticle Nilsson assignments.
doi: 10.1016/0375-9474(85)90361-6
1985BU19 Can.J.Phys. 63, 1309 (1985) D.G.Burke, W.F.Davidson, J.A.Cizewski, R.E.Brown, E.R.Flynn, J.W.Sunier The Nuclear Structure of 168Er Studied with the 170Er(p, t)168Er and 166Er(t, p)168Er Reactions NUCLEAR REACTIONS 170Er(p, t), E=18 MeV; 166Er(t, p), E=17 MeV; measured σ(Et), σ(Ep), σ(θ). 168Er deduced levels, J, π, configurations.
doi: 10.1139/p85-216
1985CE13 Phys.Rev. C32, 690 (1985) F.E.Cecil, D.M.Cole, R.Philbin, N.Jarmie, R.E.Brown Reaction 2H(3He, γ)5Li at Center-of-Mass Energies between 25 and 60 keV NUCLEAR REACTIONS, ICPND 2H(3He, γ), E(cm)=25-60 keV; measured Eγ, Iγ; deduced relative σ. 2H(3He, p), E=140 keV; measured σ(Ep), σ(Eα); deduced Γγ/Γp, relative σ. 5Li deduced level energy, relative γ-branching ratio. 4He level deduced γ-branching ratios.
doi: 10.1103/PhysRevC.32.690
1985CO22 Z.Phys. A322, 491 (1985) M.D.Cohler, R.Wadsworth, S.M.Lane, D.L.Watson, M.J.Smithson, R.E.Brown, D.M.Drake, N.Stein, J.-C.Peng, J.W.Sunier Investigation of a Possible Abrupt Change in Structure at N = 58-60 using Two-Proton Transfer NUCLEAR REACTIONS 106,110,112,116Cd(14C, 14C), (14C, 16O), E=60 MeV; measured σ(θ); deduced optical model parameters. 104,108,110,114Pd levels deduced relative S.
doi: 10.1007/BF01412085
1985JA16 Nucl.Instrum.Methods Phys.Res. B10/11, 405 (1985) Low-Energy Nuclear Reactions with Hydrogen Isotopes NUCLEAR REACTIONS, ICPND 2H(d, p), (d, 3He), E=20-117 keV; measured σ; deduced σ(E) for 2H(d, 3He), astrophysical S-function vs E.
doi: 10.1016/0168-583X(85)90279-4
1985MC04 Phys.Rev. C31, 1651 (1985) R.H.McCamis, P.J.T.Verheijen, W.T.H.van Oers, P.Drakopoulos, C.Lapointe, G.R.Maughan, N.T.Okumusoglu, R.E.Brown 3He(pol)(p, p)3He Analyzing Powers between 25 and 35 MeV NUCLEAR REACTIONS 3He(p, p), E=25-35 MeV; measured recoil analyzing power vs θ. Conventional optical pumping, 4He discharge lamp, polarized target.
doi: 10.1103/PhysRevC.31.1651
1984AJ03 Phys.Rev. C30, 1850 (1984) F.Ajzenberg-Selove, R.E.Brown, E.R.Flynn, J.W.Sunier Experimental Location of Gamow-Teller Strength for Astrophysical Calculations in the Region of A = 54-58 NUCLEAR REACTIONS 54,56,58Fe, 58Ni(t, 3He), E=25 MeV; measured σ(θ). 54,56,58Mn, 58Co levels deduced relative Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.30.1850
1984BI05 Phys.Rev. C29, 2009 (1984) J.Birchall, W.T.H. van Oers, J.W.Watson, H.E.Conzett, R.M.Larimer, B.Leemann, E.J.Stephenson, P.von Rossen, R.E.Brown Analyzing Power Measurements for 3He(p(pol), p)3He Elastic Scattering between 20 and 50 MeV NUCLEAR REACTIONS 3He(polarized p, p), E=21.4-49.6 MeV; measured analyzing power vs θ. Phase shift analysis.
doi: 10.1103/PhysRevC.29.2009
1984BO29 J.Phys.(Paris), Colloq.C3, 27 (1984) T.J.Bowles, J.D.Moses, J.Sunier, R.E.Brown, P.Lisowski, W.Mampe, P.Liaud Time Reversal Invariance in Polarized Neutron Beta Decay RADIOACTIVITY 1n(β-); measured β-decay triple correlation; deduced current limit improvements. Polarized source.
1984CO19 Z.Phys. A319, 107 (1984) M.D.Cohler, D.L.Watson, R.Wadsworth, S.M.Lane, M.J.Smithson, R.E.Brown, J.-C.Peng, N.Stein, J.W.Sunier, D.M.Drake Measurement of the Mass of 110Pd and 114Pd using the (14C, 16O) Reaction NUCLEAR REACTIONS 112,114Cd(14C, 16O), E=60 MeV; measured σ(E(16O)). 110,114Pd deduced mass. Enriched target. Mass model comparison.
doi: 10.1007/BF01429774
1984FI01 Phys.Rev. C29, 324 (1984) D.Fick, R.E.Brown, W.Gruebler, R.A.Hardekopf, J.S.Hanspal Elastic Scattering of Polarized Tritons from 12C, 51V, and 58Ni at 9 and 11 MeV NUCLEAR REACTIONS 12C, 58Ni(polarized t, t), E=9, 11 MeV; 51V(polarized t, t), E=11 MeV; measured σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevC.29.324
1984JA08 Phys.Rev. C29, 2031 (1984); Erratum Phys.Rev. C33, 385 (1986) N.Jarmie, R.E.Brown, R.A.Hardekopf Fusion-Energy Reaction 2H(t, α)n from E(t) = 12.5 to 117 keV NUCLEAR REACTIONS, ICPND 2H(t, α), E=12.5-117 keV; measured fusion σ(E), σ(Eα), astrophysical S-function vs E; deduced Maxwellian reactivities upto plasma temperatures. Single level R-matrix analysis. 2H(p, p), E=10.04 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.29.2031
1984MU13 Phys.Rev. C29, 2001 (1984) B.T.Murdoch, D.K.Hasell, A.M.Sourkes, W.T.H. van Oers, P.J.T.Verheijen, R.E.Brown 3He(p, p)3He Scattering in the Energy Range 19 to 48 MeV NUCLEAR REACTIONS 3He(p, p), E=19.5-47.5 MeV; measured σ(θ); deduced phase shifts, inelasticity parameter.
doi: 10.1103/PhysRevC.29.2001
1984WA05 J.Phys.(London) G10, L79 (1984) R.Wadsworth, M.D.Cohler, S.M.Lane, M.J.Smithson, D.L.Watson, R.E.Brown, D.M.Drake, J.-C.Peng, N.Stein, J.W.Sunier A Study of the (14C, 16O) Reaction in the Mass-100 Region NUCLEAR REACTIONS 96,100,102,104Ru, 106,108,110Pd(14C, 16O), E=60 MeV; measured σ(θ). 94,98,100,102Mo, 104,106,108Ru levels deduced relative spectroscopic factors. 96,102,104Ru, 106,108,110Pd(14C, 14C), E=60 MeV; 100Mo(16O, 16O), E=65 MeV; measured σ(θ); deduced optical model parameters. Exact finite-range DWBA analysis.
doi: 10.1088/0305-4616/10/4/003
1983AL05 Phys.Rev. C27, 1032 (1983) W.P.Alford, R.N.Boyd, E.Sugarbaker, F.W.N.de Boer, R.E.Brown, E.R.Flynn Two-Step Contributions in the 206Pb(t(pol), p)208Pb Two-Neutron Transfer Reaction NUCLEAR REACTIONS 206Pb(polarized t, p), E=17 MeV; measured σ(θ), A(θ). DWBA, sequential transfer calculations.
doi: 10.1103/PhysRevC.27.1032
1983CI01 Phys.Rev. C27, 1040 (1983) J.A.Cizewski, D.G.Burke, E.R.Flynn, R.E.Brown, J.W.Sunier Single Proton Structure of 193,195,197Ir and Perturbed Spin(6) Symmetry NUCLEAR STRUCTURE 194,196,198Pt, 193,195,197Ir; calculated levels, proton pickup S. Interacting boson fermion model, perturbed spin(6) symmetry. NUCLEAR REACTIONS 194,196,198Pt(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 193,195,197Ir deduced levels, J, π, S.
doi: 10.1103/PhysRevC.27.1040
1983CI15 Phys.Rev. C28, 2199 (1983) J.A.Cizewski, R.E.Brown, E.R.Flynn, J.W.Sunier 197Au(t, p)199Au Reaction NUCLEAR REACTIONS 197Au(t, p), E=17 MeV; measured σ(θ), σ(Ep); deduced optical model parameters. 199Au deduced levels, L, J, π, L=4 transfer strength. DWBA analyses.
doi: 10.1103/PhysRevC.28.2199
1983FL04 Phys.Rev. C27, 2587 (1983) E.R.Flynn, F.Ajzenberg-Selove, R.E.Brown, J.A.Cizewski, J.W.Sunier Proton Hole States in Neutron Rich Pd Nuclei NUCLEAR REACTIONS 106,108,110Pd(polarized t, α), E=17 MeV; measured σ(θ), analyzing power vs θ, σ(Eα). 105,107Rh deduced levels, J, π, C2S, configurations. 109Rh levels deduced C2S, configurations.
doi: 10.1103/PhysRevC.27.2587
1983FL06 Phys.Rev. C28, 575 (1983) E.R.Flynn, R.E.Brown, F.Ajzenberg-Selove, J.A.Cizewski Proton Hole States in 95Y and 95,97,99Nb NUCLEAR REACTIONS 96Zr, 96,98,100Mo(polarized t, α), E=17 MeV; measured σ(θ), analyzing power vs θ, σ(Eα); deduced Q. 95Y, 95,97,99Nb levels deduced J, π, C2S. DWBA analysis.
doi: 10.1103/PhysRevC.28.575
1983NA17 Phys.Rev. C28, 2230 (1983) S.Nath, R.G.Graves, J.C.Hiebert, L.C.Northcliffe, H.L.Woolverton, R.L.York, R.E.Brown, P.Doleschall Measurement of the 1H(d(pol), n(pol))pp Transverse Polarization Transfer Coefficient at 42.8 MeV NUCLEAR REACTIONS 1H(polarized d, n), E=42.8 MeV; measured transverse polarization transfer coefficient at θ=0°. Spectator stripping model, Faddeev calculation comparison.
doi: 10.1103/PhysRevC.28.2230
1983RO01 Phys.Rev. C27, 11 (1983) R.G.H.Roberston, P.Dyer, T.J.Bowles, R.E.Brown, N.Jarmie, C.J.Maggiore, S.M.Austin Cross Section of the Capture Reaction 3He(α, γ)7Be NUCLEAR REACTIONS, ICPND 3He(α, γ), 4He(3He, γ), E(cm)=897 keV; measured σ; deduced astrophysical capture σ. Activation technique.
doi: 10.1103/PhysRevC.27.11
1983SL01 Nucl.Phys. A397, 205 (1983) I.Slaus, J.M.Lambert, P.A.Treado, F.D.Correll, R.E.Brown, R.A.Hardekopf, N.Jarmie, Y.Koike, W.Gruebler The 4He(d(pol), αp)n Reaction at 12 and 17 MeV NUCLEAR REACTIONS 4He(polarized d, pα), E=12, 17 MeV; measured σ(E(α), θ(α), E(p), θ(p)), analyzing powers vs arc length. Three-body Fadeev analysis, energy and angle dependence.
doi: 10.1016/0375-9474(83)90102-1
1983VO04 Z.Phys. A310, 275 (1983) W.von Oertzen, E.R.Flynn, J.C.Peng, J.W.Sunier, R.E.Brown Study of Spin-Orbit Interaction of 13C and 15N Nuclei in 14C Induced Transfer Reactions on 138Ba NUCLEAR REACTIONS 138Ba(14C, 15N), (14C, 13C), E=64 MeV; measured σ(E(15N)), σ(E(13C)), σ(θ), reaction asymmetry; deduced optical potential parameters, spin-orbit interaction role. DWBA analysis.
1983VO12 Z.Phys. A313, 371 (1983) W.von Oertzen, R.E.Brown, E.R.Flynn, J.C.Peng, J.W.Sunier Pairing Enhancement of Two-Neutron Transfer in (14C, 12C) Reactions NUCLEAR REACTIONS 138Ba(14C, 12C), E=64 MeV; 124Sn(14C, 12C), E=59.7 MeV; measured σ(E(12C)), σ(θ); deduced two-neutron transfer mechanism.
1982BA45 Nucl.Phys. A388, 542 (1982) J.M.Barnwell, R.J.Griffiths, R.E.Brown, R.A.Hardekopf, N.Jarmie, F.D.Correll The Interactions of Polarised Tritons with 32S NUCLEAR REACTIONS 32S(polarized t, t), (polarized t, t'), (polarized t, α), E=17 MeV; measured σ(θ), A(θ). 31P levels deduced spectroscopic factors. Optical model, DWBA, CCBA analyses.
doi: 10.1016/0375-9474(82)90476-6
1982CI02 Phys.Rev. C26, 1960 (1982) J.A.Cizewski, E.R.Flynn, R.E.Brown, J.W.Sunier Fragmentation of L = 0 Transfer Strength in the 195Pt(t, p)197Pt Reaction NUCLEAR REACTIONS 195Pt(t, p), E=17 MeV; measured σ(Ep), σ(θ). 197Pt deduced levels, L, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.26.1960
1982FU01 Phys.Rev. C25, 23 (1982) R.D.Furber, R.E.Brown, G.L.Peterson, D.R.Thompson, Y.C.Tang Resonating-Group Study of the 3He(3H) + α Systems: Bound states to 113 MeV NUCLEAR REACTIONS 3He(α, α), E(cm)=4.98, 10.14, 24.36, 44.5, 60.2, 131.1 MeV; calculated σ(θ); 3H(α, α), E=9.69 MeV; 3He(α, α), E=17.09 MeV; calculated A(θ). Resonating group method, effective nucleon-nucleon spin-orbit force.
doi: 10.1103/PhysRevC.25.23
1982SC21 Phys.Rev. C26, 369 (1982) P.Schwandt, R.E.Brown, F.D.Correll, R.A.Hardekopf, G.G.Ohlsen Elastic Scattering of Polarized Tritons from A = 26-28 Nuclei at 17 MeV NUCLEAR REACTIONS 26Mg, 27Al, 28Si(polarized t, t), E=17 MeV; measured σ(θ), A(θ). Optical model analysis.
doi: 10.1103/PhysRevC.26.369
1981AJ02 Phys.Rev. C24, 1762 (1981) F.Ajzenberg-Selove, R.E.Brown, E.R.Flynn, J.W.Sunier States of 69Cu NUCLEAR REACTIONS 70Zn(polarized t, α), E=17 MeV; measured σ(θ), A(θ), Q. 69Cu deduced mass excess, levels, J, π. Q3D spectrometer. DWBA analysis.
doi: 10.1103/PhysRevC.24.1762
1981AR19 Phys.Rev. C24, 2326 (1981) L.G.Arnold, R.N.Boyd, F.Ajzenberg-Selove, R.E.Brown, E.R.Flynn, J.W.Sunier 6.53 MeV State of 6Li NUCLEAR REACTIONS 9Be(polarized t, α), E=17 MeV; measured σ(θ), analyzing power vs θ. 8Li level deduced J, π. CCBA analysis.
doi: 10.1103/PhysRevC.24.2326
1981CI01 Phys.Rev. C23, 1453 (1981) J.A.Cizewski, E.R.Flynn, R.E.Brown, D.L.Hanson, S.D.Orbesen, J.W.Sunier Two-Neutron Transfer in Pt Nuclei and the Structure of 200Pt NUCLEAR STRUCTURE 186,188,190,192,194,196,198,200Pt; calculated L=4 transition systematics. Interacting boson, schematic, pairing vibration, boson expansion models. NUCLEAR REACTIONS 194,196,198Pt(t, p), E=17 MeV; measured σ(Ep, θ). 196,198,200Pt deduced levels, J, π, L, two-nucleon transfer strengths. DWBA analysis.
doi: 10.1103/PhysRevC.23.1453
1981CI02 Phys.Rev.Lett. 46, 1264 (1981) J.A.Cizewski, D.G.Burke, E.R.Flynn, R.E.Brown, J.W.Sunier Dynamical Supersymmetries and Single-Particle Strengths in Iridium Nuclei NUCLEAR REACTIONS 194,196,198Pt(polarized t, α), 191,193Ir(t, p), E=17 MeV; measured σ(θ). 193,195,197Ir deduced levels, J, π, S. 195,197Ir deduced no evidence for dynamical supersymmetry. Spin(6) supersymmetry scheme.
doi: 10.1103/PhysRevLett.46.1264
1981CO07 Phys.Rev. C23, 960 (1981) F.D.Correll, G.G.Ohlsen, R.E.Brown, R.A.Hardekopf, N.Jarmie, P.Doleschall Kinematically Incomplete Three-Nucleon Breakup Reaction 1H(pol(d), p)pn at 16 MeV NUCLEAR REACTIONS 1H(polarized d, p), E=16 MeV; measured analyzing power vs Ep, θ. Kinematically incomplete breakup reaction, Faddeev calculation.
doi: 10.1103/PhysRevC.23.960
1981FL01 Phys.Lett. B98, 166 (1981); Erratum Phys.Lett. 99B, 507 (1981) E.R.Flynn, J.A.Cizewski, R.E.Brown, J.W.Sunier 136,138Ba(t, p) and the Systematics of Neutron Pairing Vibrations at N=82 NUCLEAR REACTIONS 136,138Ba(t, p), E=17 MeV; measured σ(Ep). 138Ba deduced levels, vibrational character. 138,140Ba deduced two-neutron binding energy.
doi: 10.1016/0370-2693(81)90979-5
1981FL02 Phys.Rev. C24, 902 (1981); Erratum Phys.Rev. C25, 2851 (1982) E.R.Flynn, F.Ajzenberg-Selove, R.E.Brown, J.A.Cizewski, J.W.Sunier Proton Hole States in Neutron Rich Nuclei near A = 100 NUCLEAR REACTIONS 104Ru, 110Pd(polarized t, α), E=17 MeV; measured σ(Eα), σ(θ), analyzing power vs θ. 109Rh, 103Tc deduced levels, L, J, π, C2S, mass excess. DWBA analysis.
doi: 10.1103/PhysRevC.24.902
1981FL05 Phys.Lett. 105B, 125 (1981) E.R.Flynn, R.E.Brown, J.W.Sunier, J.M.Gursky, J.A.Cizewski, D.G.Burke Proton-Hole Excitations in 201,203Au from 202,204Hg(t(pol), α) Reactions NUCLEAR REACTIONS 202,204Hg(polarized t, α), E=17 MeV; measured σ(θ), analyzing power vs θ. 203,201Au deduced levels, J, π, C2S, Q.
doi: 10.1016/0370-2693(81)91004-2
1981FL06 Phys.Rev. C24, 2475 (1981); Erratum Phys.Rev. C25, 2850 (1982) E.R.Flynn, F.Ajzenberg-Selove, R.E.Brown, J.A.Cizewski, J.W.Sunier 92,94,97,98Mo(t, p) Reactions at Et = 17 MeV NUCLEAR REACTIONS 92,94,97,98Mo(t, p), E=17 MeV; measured σ(θ). 94,96,99,100Mo deduced levels, J, π, two-nucleon transfer strengths. DWBA analysis.
doi: 10.1103/PhysRevC.24.2475
1981VO06 Z.Phys. A301, 365 (1981) W.von Oertzen, E.R.Flynn, J.C.Peng, J.W.Sunier, R.E.Brown Optical Model Spin-Orbit Potential of 15N NUCLEAR REACTIONS 138Ba(14C, 15N), E=64 MeV; measured σ(θ); deduced spin-orbit potential paramters for 15N projectiles. Q3D spectrometer, ΔE-E detectors. Finite-range DWBA analysis.
1980BR10 Phys.Rev. C21, 2663 (1980) R.E.Brown, J.A.Cizewski, J.W.Sunier, E.R.Flynn, P.Alford, E.Sugarbaker, D.Ardouin Search for Nuclear Structure Dependence of Analyzing Powers for the (t, p) Reaction in Medium Mass Nuclei NUCLEAR REACTIONS 96Mo, 106Pd, 126Te(polarized t, p); measured σ(θ), analyzing power vs θ. DWBA analysis.
doi: 10.1103/PhysRevC.21.2663
1980FL03 Phys.Rev. C22, 43 (1980) E.R.Flynn, R.E.Brown, J.A.Cizewski, J.W.Sunier, W.P.Alford, E.Sugarbaker, D.Ardouin Analyzing Power Measurements for Two-Nucleon Transfer Reactions in a Shape Transitional Nucleus NUCLEAR REACTIONS 96,100Mo(polarized t, p), E=17 MeV; measured σ(Ep, θ), analyzing power vs θ. 98,102Mo deduced shape. DWBA.
doi: 10.1103/PhysRevC.22.43
1979BR18 Phys.Rev. C20, 892 (1979) R.E.Brown, F.D.Correll, R.F.Haglund, Jr., R.A.Hardekopf, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach Direct-Reaction and Isospin Symmetries in d + d Reactions NUCLEAR REACTIONS 2H(polarized d, p), E=13.39, 15.50, 17.00 MeV; 2H(polarized d, n), E=15.50, 17.00 MeV; measured analyzing power(θ).
doi: 10.1103/PhysRevC.20.892
1979BR19 Phys.Rev. C20, 1301 (1979) R.E.Brown, J.A.Cizewski, E.R.Flynn, J.W.Sunier N = 152 Shell Gap and the 244Pu(t, p)246Pu Reaction NUCLEAR REACTIONS 244Pu(t, p), E=17 MeV; measured σ(θ). 246Pu deduced mass excess, shell gap. DWBA analysis.
doi: 10.1103/PhysRevC.20.1301
1979CI05 Phys.Lett. 88B, 207 (1979) J.A.Cizewski, E.R.Flynn, R.E.Brown, J.W.Sunier Two-Particle Transfer in O(6) Nuclei NUCLEAR REACTIONS 192,194,196,198Pt, 186,188,190,192Os(t, p), E=17 MeV; measured σ(θ). 194,196,198,200Pt, 188,190,192,194Os deduced 2n transfer strengths. Natural, enriched target. DWBA analysis, O(6) limit interacting boson approximation model.
doi: 10.1016/0370-2693(79)90449-0
1979FL01 Phys.Rev.Lett. 42, 626 (1979) E.R.Flynn, R.E.Brown, F.D.Correll, D.L.Hanson, R.A.Hardekopf Total Angular Momentum Determinations from the (t(pol), d) Reaction On 58,64Ni NUCLEAR REACTIONS 58,64Ni(polarized t, d), E=16 MeV; measured σ(θ), Ay(θ). 59Ni deduced(2J+1)s. 59,65Ni levels deduced J, π, (2J+1)S. DWBA analysis.
doi: 10.1103/PhysRevLett.42.626
1979FL03 Nucl.Phys. A319, 61 (1979) E.R.Flynn, R.E.Brown, R.F.Haglund, Jr., R.A.Hardekopf, P.A.Schmelzbach, J.W.Sunier, W.von Oertzen Analyzing Power in the Mass-Six Supermultiplet System NUCLEAR REACTIONS 9Be(polarized t, 6Li), E=17 MeV; measured σ(θ), Ay(θ); deduced reaction mechanism.
doi: 10.1016/0375-9474(79)90171-4
1979GR13 Nucl.Phys. A331, 61 (1979) W.Gruebler, R.E.Brown, F.D.Correll, R.A.Hardekopf, N.Jarmie, G.G.Ohlsen d + α Scattering from 12 to 17 MeV NUCLEAR REACTIONS 4He(polarized d, d), E=12, 14, 15, 17 MeV; measured σ(θ), vector, tensor analyzing power, A(θ). Phase-shift analysis.
doi: 10.1016/0375-9474(79)90301-4
1978HA38 Phys.Lett. 79B, 35 (1978) R.F.Haglund, Jr., R.E.Brown, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach, D.Fick Triton-Proton Elastic Scattering and Spin-Dependent Nucleon-Nucleon Forces NUCLEAR REACTIONS 1H(polarized t, t), E(cm)=1.26-3.71 MeV; measured σ(θ), analyzing power A(Et, θ).
doi: 10.1016/0370-2693(78)90429-X
1978HA48 Helv.Phys.Acta 51, 506 (1978) R.F.Haglund, Jr., R.E.Brown, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach, D.Fick Elastic Triton-Proton Scattering and Spin Dependent Nucleon-Nucleon Forces NUCLEAR REACTIONS 1H(polarized t, t), E(cm)=1.26, 1.68, 2.19, 2.70, 3.21, 3.71 MeV; measured σ(θ), A(θ); deduced phase shifts. Cluster model calculations.
1977BR21 Phys.Rev. C16, 513 (1977) R.E.Brown, G.G.Ohlsen, R.F.Haglund, Jr., N.Jarmie 3H(α, 6Li)n Reaction at 0° NUCLEAR REACTIONS 3He(α, α), (α, 6Li), (α, t), E=11.3-12.0 MeV; measured σ(E).
doi: 10.1103/PhysRevC.16.513
1977CO19 J.Inorg.Nucl.Chem. 39, 1706 (1977) K.E.Collins, C.H.Collins, R.E.Brown, H.Djojosubroto The Half-Life of 55Cr RADIOACTIVITY 55Cr; measured T1/2.
doi: 10.1016/0022-1902(77)80132-2
1977HA17 Phys.Rev. C15, 1613 (1977) R.F.Haglund, Jr., G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.E.Brown, P.A.Schmelzbach 3He(t, t)3He Elastic Scattering Measurements from 9 to 17 MeV NUCLEAR REACTIONS 3He(polarized t, t), E=9-17 MeV; measured σ(E, θ), A(E, θ).
doi: 10.1103/PhysRevC.15.1613
1977HA42 Phys.Rev. C16, 2151 (1977) R.F.Haglund, Jr., G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.E.Brown Analyzing-Power Measurements for the 3He(t, d)4He Reaction NUCLEAR REACTIONS 3He(polarized t, d), E=9.02-17.27 MeV; measured A(E, θ).
doi: 10.1103/PhysRevC.16.2151
1977HE09 Phys.Rev.Lett. 39, 9 (1977) P.M.Hegland, R.E.Brown, J.S.Lilley, J.A.Koepke Proton-Proton Central p-Wave Parameter from 6 to 10 MeV (lab) NUCLEAR REACTIONS 1H(p, p), E=6-10 MeV; measured shape σ(E); deduced central p-wave parameter.
doi: 10.1103/PhysRevLett.39.9
1977KO09 Phys.Rev. C16, 18 (1977) Reaction Measurements and Analyses for 3He + 4He at 15.95 MeV (c.m.) NUCLEAR REACTIONS 4He(3He, p), (3He, α), E=28.00 MeV; measured σ(θ); deduced total σ. α-continuum, phase shift analysis. Resonating group comparison.
doi: 10.1103/PhysRevC.16.18
1977LE05 Phys.Rev. C15, 1191 (1977) M.LeMere, R.E.Brown, Y.C.Tang, D.R.Thompson Macroscopic Description of Exchange Effects in Light-Ion Interactions with 16O NUCLEAR REACTIONS 16O(α, α), (3He, 3He), (p, p); calculated phase shifts, σ; deduced exchange effects. Resonating group analysis.
doi: 10.1103/PhysRevC.15.1191
1977TH07 Phys.Rev. C16, 1 (1977) D.R.Thompson, R.E.Brown, M.LeMere, Y.C.Tang Resonating-Group of p + α Scattering from 68 to 125 MeV NUCLEAR REACTIONS 4He(p, p), E(cm)=60, 80, 124.8 MeV; calculated phase shifts, σ(θ). Resonating-group method.
doi: 10.1103/PhysRevC.16.1
1976BR32 Phys.Rev. C14, 1675 (1976) On the Use of α + α Scattering to Study the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 4He(α, α), E(cm)=15 MeV; calculated potential.
doi: 10.1103/PhysRevC.14.1675
1976LI01 Phys.Rev. C13, 55 (1976) T.K.Li, D.Dehnhard, R.E.Brown, P.J.Ellis Investigation of the (d, 5/2)2 and (d5/2s1/2) Two-Particle Configurations in 18O Using the 17O(d, p)18O Reaction at 18 MeV NUCLEAR REACTIONS 17O(d, d), E=18.0 MeV; measured σ(θ); deduced optical model parameters. 17O(d, p), E=18.0 MeV; measured σ(Ep, θ). 18O levels deduced L, S. Enriched target.
doi: 10.1103/PhysRevC.13.55
1976PA20 Nucl.Phys. A273, 341 (1976) R.A.Partridge, Y.C.Tang, D.R.Thompson, R.E.Brown Influence of the Pauli Principle on the Optical Potential for α + 16O Scattering NUCLEAR REACTIONS 16O(α, α), E=20, 25 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90595-9
1976SO01 Phys.Rev. C13, 451 (1976) A.M.Sourkes, A.Houdayer, W.T.H.van Oers, R.F.Carlson, R.E.Brown Total Reaction Cross Section for Protons on 3He and 4He between 18 and 48 MeV NUCLEAR REACTIONS 3,4He(p, X), (p, p), E=18-48 MeV; measured total σ(E). Anti-coin beam-attenuation technique.
doi: 10.1103/PhysRevC.13.451
1975LE20 Phys.Rev. C12, 1140 (1975) M.LeMere, R.E.Brown, Y.C.Tang, D.R.Thompson Resonating-Group Calculation of n + 3H Scattering NUCLEAR REACTIONS 3He(n, n), E=4.5-17.25 MeV; calculated σ(E, θ), phase shifts.
doi: 10.1103/PhysRevC.12.1140
1975OL03 Phys.Rev. C11, 1557 (1975) D.K.Olsen, T.Udagawa, R.E.Brown Study of 20Ne(p, t)18Ne Transitions with the Coupled-Channel Born Approximation NUCLEAR REACTIONS 20Ne(p, t), E=39.8 MeV; measured σ(Et, θ); deduced form factors. 18Ne levels deduced β.
doi: 10.1103/PhysRevC.11.1557
1974BR30 Nucl.Phys. A230, 189 (1974) R.E.Brown, F.S.Chwieroth, Y.C.Tang, D.R.Thompson Odd-Even Features in 3He + 3H Scattering NUCLEAR REACTIONS 3He(t, t), E(cm)=3.91, 9.955, 13.85 MeV; calculated σ(θ). 6Li calculated phase shifts.
doi: 10.1016/0375-9474(74)90301-7
1974CH45 Phys.Rev. C10, 1767 (1974) Study of the α + α System below 15 MeV (c.m.) NUCLEAR REACTIONS 4He(α, α), E=18.00-29.50 MeV; measured σ(E;θ); deduced phase shifts L=0, 2, 4, 6. R-matrix analysis L=4. Comparison with resonating-group calculations. Potential-model analysis.
doi: 10.1103/PhysRevC.10.1767
1974KO03 Phys.Rev. C9, 823 (1974) J.A.Koepke, R.E.Brown, Y.C.Tang, D.R.Thompson Odd-Even Absorption and Coulomb-Exchange Effects in the 3He + 4He and 3H + 4He Systems NUCLEAR REACTIONS 4He(3He, 3He), E(cm)=1.7-44.5 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.9.823
1973CH27 Phys.Rev. C8, 938 (1973) F.S.Chwieroth, R.E.Brown, Y.C.Tang, D.R.Thompson Study of d + 3H and d + 3He Systems with the Resonating-Group Method NUCLEAR REACTIONS 3H, 3He(d, d); calculated σ(θ), phase shifts. Resonating group method.
doi: 10.1103/PhysRevC.8.938
1973HO10 Nucl.Phys. A203, 339 (1973) C.G.Hoot, D.K.Olsen, R.E.Brown, J.R.Maxwell, A.Scott Study of Some Two-Nucleon Pick-up Reactions in the 1p Shell with 39.8 MeV Protons NUCLEAR REACTIONS 12C, 14N, 16O(p, 3He), 14C(p, t), Ep=39.8 MeV; measured σ(E(3He), θ), σ(Et, θ). DWBA analysis.
doi: 10.1016/0375-9474(73)90139-5
1973OL03 Phys.Rev. C8, 609 (1973) D.K.Olsen, T.Udagawa, T.Tamura, R.E.Brown Coupled-Channel-Born-Approximation Analysis of 'Allowed' and 'Forbidden' 22Ne(p, t)20Ne Transitions NUCLEAR REACTIONS 22Ne(p, t), E=39.8 MeV; measured σ(Et, θ). 20Ne deduced nothing.
doi: 10.1103/PhysRevC.8.609
1973TH01 Nucl.Phys. A201, 301 (1973) D.R.Thompson, Y.C.Tang, J.A.Koepke, R.E.Brown Odd-Even Absorption in 3He + 3He Scattering NUCLEAR REACTIONS 3He(3He, 3He), E=2.95-37.44 MeV cms; calculated σ(E). 6Be deduced resonance parameters.
doi: 10.1016/0375-9474(73)90067-5
1972OL04 Phys.Rev.Lett. 29, 1178 (1972); Erratum Phys.Rev.Lett. 30, 940 (1973) D.K.Olsen, T.Udagawa, T.Tamura, R.E.Brown Coupled-Channel Born-Approximation Calculation for the Transition Ne22(p, t)Ne20(2-, 4.97 MeV) NUCLEAR REACTIONS 22Ne(p, t), E=39.8 MeV; measured σ(θ); analyzed σ(θ). Coupled-channel Born approximation; rotational wave functions of adiabatic form.
doi: 10.1103/PhysRevLett.29.1178
1972TH06 Phys.Rev. C5, 1939 (1972) D.R.Thompson, Y.C.Tang, R.E.Brown Majorana Component in the Imaginary Potential for p + α Scattering NUCLEAR REACTIONS 4He(p, p), E < 78 MeV; calculated σ(E;θ), P(E;θ), phase shifts. Resonating-group method, Majorana component in imaginary potential.
doi: 10.1103/PhysRevC.5.1939
1971BR30 Nucl.Phys. A170, 225 (1971) Imaginary Potential in Resonating-Group Calculations for the α+α System NUCLEAR REACTIONS 4He(α, α), E=25-60 MeV cms; calculated phase shifts. Resonating-group method.
doi: 10.1016/0375-9474(71)90633-6
1971BR46 Nucl.Phys. A178, 145 (1971) R.E.Brown, I.Reichstein, Y.C.Tang Imaginary Potential in Resonating-Group Calculation of 3He+3He Scattering NUCLEAR REACTIONS 3He(3He, 3He), E=1.5-15 MeV; calculated σ(E;θ). Resonating group method, imaginary potential.
doi: 10.1016/0375-9474(71)90194-1
1971OL04 Nucl.Phys. A170, 544 (1971) The (p, t) and (p, tau) Reactions on 17O at 39.8 MeV NUCLEAR REACTIONS 17O(p, t), (p, 3He), Ep=39.8 MeV; measured σ(Et, θ), σ(E(3He), θ). Enriched target.
doi: 10.1016/0375-9474(71)90234-X
1971TA23 Phys.Rev. C4, 1979 (1971) Exchange Effects in He3 + He4 Scattering NUCLEAR REACTIONS 4He(3He, 3He), E=44.5 cm; calculated σ(θ), phase shifts. Resonating-group formalism.
doi: 10.1103/PhysRevC.4.1979
1970BR42 Phys.Rev.Lett. 25, 1346 (1970) R.E.Brown, E.E.Gross, A.van der Woude Experimental Observation of a Predicted Exchange Resonance in 3He + 4He Elastic Scattering NUCLEAR REACTIONS 4He(3He, 3He), E=19-51 MeV; measured σ(E;θ). 7Be deduced resonance structure.
doi: 10.1103/PhysRevLett.25.1346
1970JA04 Phys.Rev. C1, 1615 (1970) Elastic Scattering of He3 by He4 from 17.8 to 30.0 MeV NUCLEAR REACTIONS 4He(3He, 3He), E=17.8-30 MeV; measured σ(E;θ); deduced phase shifts.
doi: 10.1103/PhysRevC.1.1615
1970JE02 Phys.Rev. C1, 1622 (1970) J.G.Jenkin, W.D.Harrison, R.E.Brown Study of He3 + He3 Elastic Scattering and the Nucleus Be6 NUCLEAR REACTIONS 3He(3He, 3He), E=17.9-32 MeV; measured σ(E;θ). 6Be deduced resonance.
doi: 10.1103/PhysRevC.1.1622
1965BR13 Phys.Rev. 138, B1394 (1965) R.E.Brown, J.S.Blair, D.Bodansky, N.Cue, C.D.Kavaloski O16(α, Be8)C12 Reaction NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B1394
1964SC07 Nucl.Phys. 52, 353 (1964) F.H.Schmidt, R.E.Brown, J.B.Gerhart, W.A.Kolasinski Proton Spin Flip and Substate Excitation in Inelastic Scattering NUCLEAR STRUCTURE 24Mg, 58Ni, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90700-X
1963BR14 Astrophys.J. 137, 338 (1963) Energy Levels in N14 Pertaining to the Ratio C12/C12 Produced in the CNO Cycle NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1086/147509
1962BR08 Phys.Rev. 125, 347 (1962) Experimental Study of the O17(p, α)N14 Reaction and a Calculation of the Rate of this Reaction in the CNO Cycle in Stars NUCLEAR REACTIONS 17O(p, α), E=0.49-1.58 MeV; measured reaction products. 18F; deduced σ, resonance parameters. Comparison with available data.
doi: 10.1103/PhysRev.125.347
1962GE01 Bull.Am.Phys.Soc. 7, No.4, 270, CB12 (1962) J.B.Gerhart, F.H.Schmidt, W.A.Kolasinski, R.E.Brown C12 Spin-Substate Amplitudes in C12(p, p'γ) Scattering at 10.5 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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