NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = B.L.Burks Found 26 matches. 1990BE03 Phys.Rev. C41, 920 (1990) J.R.Beene, F.E.Bertrand, D.J.Horen, R.L.Auble, B.L.Burks, J.Gomez del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien Heavy-Ion Coulomb Excitation and Photon Decay of the Giant Dipole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured σ(E(17O)), γ(particle)(θ, φ) following Coulomb excitation, σ(θ). 208Pb deduced giant resonance decay features, B(λ), M(n)/M(p).
doi: 10.1103/PhysRevC.41.920
1989HO11 Z.Phys. A333, 39 (1989) D.J.Horen, J.Lisantti, R.L.Auble, F.E.Bertrand, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson T = 1, Spin-Dipole Strength in 40Ca NUCLEAR REACTIONS 40Ca(p, p'), E=500 MeV; measured σ(θ), σ(Ep). 40Ca deduced T=1 spin-dipole transition strength distribution.
1989LI03 Phys.Rev. C39, 568 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Collective Model Distored-Wave Born Approximation Analysis of 500-MeV Proton Scattering form 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; analyzed σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca levels deduced deformation lengths, multipole matrix elements. Relativistic, non-relativistic DWBA analysis.
doi: 10.1103/PhysRevC.39.568
1989LI15 Phys.Rev. C40, 211 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Giant Resonance Strength Distribution in 40Ca from Inelastic Scattering of 500 MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; measured σ(θp, Ep), σ(θ). 40Ca deduced giant resonance strength distribution.
doi: 10.1103/PhysRevC.40.211
1989SW01 Phys.Rev. C40, 246 (1989) L.W.Swenson, X.Y.Chen, J.Lisantti, D.K.McDaniels, I.Bergqvist, F.E.Bertrand, D.J.Horen, E.E.Gross, C.Glover, R.O.Sayer, B.L.Burks, O.Hausser, K.Hicks, M.J.Iqbal Different Continuum Approaches to Giant Resonances in 208Pb with 400-MeV Protons NUCLEAR REACTIONS 208Pb(p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200 MeV; measured σ(θ). 208Pb deduced giant resonance L, Γ, EWSR. DWBA analysis, continuum models comparison.
doi: 10.1103/PhysRevC.40.246
1988BA39 Phys.Lett. 209B, 182 (1988) J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, D.J.Horen, J.R.Beene, F.E.Bertrand, R.L.Auble, B.L.Burks, J.Gomez Del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, B.Haas, J.P.Vivien Coulomb Excitation of Giant Resonances in 208Pb by E = 84 MeV/Nucleon 17O Projectiles NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), E=1428 MeV; measured σ(θ). 208Pb deduced giant resonance excitation mechanism, B(λ), EWSR.
doi: 10.1016/0370-2693(88)90929-X
1988BU15 Phys.Rev. C38, 1680 (1988) B.L.Burks, M.A.G.Fernandes, G.R.Satchler, D.J.Horen, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen Optical Model and Coupled-Channels Analyses of the Elastic and Inelastic Scattering of 18O from 28Si at 352 MeV NUCLEAR REACTIONS 28Si(18O, 18O), (18O, 18O'), E=351.7 MeV; measured σ(θ). Optical model, coupled-channels analyses.
doi: 10.1103/PhysRevC.38.1680
1988HA26 Phys.Rev. C38, 572 (1988) B.A.Harmon, D.Shapira, P.H.Stelson, B.L.Burks, K.A.Erb, B.Shivakumar, K.Teh, S.T.Thornton Effect of Entrance Channel Asymmetry of Fusion Reactions Leading to Compound Nuclei with A = 40, 42 NUCLEAR REACTIONS 12C(28Si, X), E=6.4, 7.8, 9.4 MeV/nucleon; 12C(30Si, X), E=5.2, 5.7, 6.4, 7.5, 8.3 MeV/nucleon; measured fusion σ; deduced entrance channel asymmetry role.
doi: 10.1103/PhysRevC.38.572
1988LI18 Phys.Rev. C37, 2408 (1988) J.Lisantti, F.E.Bertrand, D.J.Horen, B.L.Burks, C.W.Glover, D.K.McDaniels, L.W.Swenson, X.Y.Chen, O.Hausser, K.Hicks Excitation of Giant Resonances in 28Si with 250 MeV Protons NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=250 MeV; measured σ(θ). 28Si deduced level deformation lengths, giant resonance EWSR.
doi: 10.1103/PhysRevC.37.2408
1987BE02 Phys.Rev. C35, 111 (1987) F.E.Bertrand, R.O.Sayer, R.L.Auble, M.Beckerman, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, J.Gomez del Campo, D.Shapira, H.P.Morsch Excitation of the High Energy Nuclear Continuum in 208Pb by 22 MeV/Nucleon 17O and 32S NUCLEAR REACTIONS 208Pb(17O, 17O'), (32S, 32S'), E=22 MeV/nucleon; measured σ(E(17O)), σ(E(32S)). Enriched targets, magnetic spectrograph.
doi: 10.1103/PhysRevC.35.111
1987BE03 Phys.Rev.Lett. 58, 455 (1987) M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, C.W.Glover, R.O.Sayer, G.R.Satchler, D.Shapira, R.L.Varner Quasielastic Transfer of a Neutron between 58Ni and 208Pb at Bombarding Energies of 598 and 1011 MeV NUCLEAR REACTIONS 208Pb(58Ni, 59Ni), (58Ni, 57Ni), E=598, 1011 MeV; measured σ(E(59Ni)), σ(E(57Ni)), σ(θ). Enriched targets, tof. DWBA analyses.
doi: 10.1103/PhysRevLett.58.455
1987BE23 Phys.Rev. C36, 657 (1987) M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, R.O.Sayer, G.R.Satchler, D.Shapira, Y.Sugiyama, R.L.Varner Elastic and Inelastic Scattering of 58Ni + 208Pb at Bombarding Energies from 598 to 1011 MeV NUCLEAR REACTIONS 208Pb(58Ni, 58Ni), (58Ni, 58Ni'), E=598-1011 MeV; measured σ(E), σ(θ). 208Pb, 58Ni levels deduced B(E2), Coulomb deformation constants. Optical model, DWBA, coupled-channels calculations.
doi: 10.1103/PhysRevC.36.657
1987FE04 Phys.Rev. C36, 108 (1987) M.A.G.Fernandes, F.E.Bertrand, R.L.Auble, R.O.Sayer, B.L.Burks, D.J.Horen, E.E.Gross, J.L.Blankenship, D.Shapira, M.Beckerman Single-Nucleon Transfer Reactions Induced by 376-MeV 17O on 208Pb NUCLEAR REACTIONS 208Pb(17O, 16O), (17O, 18F), E=376 MeV; measured σ(θ); deduced model parameters. 209Pb, 207Tl levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.36.108
1987HO18 Z.Phys. A328, 189 (1987) D.J.Horen, M.A.G.Fernandes, G.R.Satchler, B.L.Burks, R.L.Auble, F.E.Bertrand, E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira Transfer Reactions at High Energy and Ambiguities in Heavy-Ion Potentials NUCLEAR REACTIONS 28Si(16O, 16O), E=56, 351.7 MeV; calculated σ(θ); deduced optical potential parameters. 28Si(18O, 17O), E=352 MeV; 28Si(18O, 19F), E=352 MeV; analyzed data; deduced model parameters. 29Si, 29Al levels deduced spectroscopic factors.
1987MC03 Nucl.Phys. A467, 557 (1987) D.K.McDaniels, J.Lisantti, I.Bergqvist, L.W.Sewnson, X.Y.Chen, D.J.Horen, F.E.Bertrand, E.E.Gross, C.Glover, R.Sayer, B.L.Burks, O.Hausser, K.Hicks Validity of Collective Model DWBA Analysis for Intermediate Energy Proton Scattering to Low-Lying States of 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=200, 400 MeV; measured σ(θ). 208Pb levels deduced deformation lengths, multipole moments, neutron, proton matrix element ratio. DWBA analysis.
doi: 10.1016/0375-9474(87)90386-1
1986BU14 Nucl.Phys. A457, 337 (1986) B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, B.C.Karp, Y.Aoki A DWBA Analysis of the 86Sr(d(pol), p)87Sr Reaction and Implications for a 87Rb Solar Neutrino Detector NUCLEAR REACTIONS 86Sr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), vector analyzing power versus θ. 87Sr deduced levels, J, π, S. DWBA, optical model analyses.
doi: 10.1016/0375-9474(86)90382-9
1986BU18 Phys.Rev. C34, 2316 (1986) B.L.Burks, R.L.Varner, E.J.Ludwig Q-Value Determination for the 80Kr(d, p)81Kr Reaction NUCLEAR REACTIONS 80Kr(d, p), E=11 MeV; measured σ(Ep); deduced Q. 80Kr deduced mass excess. Ion implanted foil target.
doi: 10.1103/PhysRevC.34.2316
1986FE03 Phys.Rev. C33, 1971 (1986) M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen One-Nucleon-Transfer Reactions Induced by 352-MeV 18O on 28Si NUCLEAR REACTIONS 28Si(18O, 17O), (18O, 19F), E=352 MeV; measured σ(θ); deduced model parameters. 29Si, 27Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.33.1971
1986HO27 Phys.Lett. 181B, 38 (1986) D.J.Horen, B.L.Burks, M.A.G.Fernandes, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, G.R.Satchler, D.Shapira, T.P.Sjoreen, F.Petrovich Investigation of the One-Step Direct Contribution to the 28Si(18O, 18F)28Al Reaction at 19.6 MeV/Nucleon NUCLEAR REACTIONS, MECPD 28Si(18O, 18F), E=352 MeV; measured σ(E(18F)), σ(θ); deduced reaction mechanism. Magnetic spectrometer system, particle identification ionization chamber. Microscopic DWIA calculations.
doi: 10.1016/0370-2693(86)91250-5
1986KA27 Nucl.Phys. A457, 15 (1986) B.C.Karp, E.J.Ludwig, J.E.Bowsher, B.L.Burks, T.B.Clegg, F.D.Santos, A.M.Eiro Alpha-Particle D-State and Configuration-Mixing Effects in the 89Y(d, α)87Sr Reaction NUCLEAR REACTIONS 89Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 89Y(polarized d, d), E=12 MeV; measured σ(θ), vector analyzing power vs θ. 87Sr(α, α), E=19.5 MeV; measured σ(θ). 87Sr levels deduced L, J, configuration mixing, α-particle D-state parameter. Finite range DWBA.
doi: 10.1016/0375-9474(86)90517-8
1985BU14 Nucl.Phys. A442, 300 (1985) B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, R.L.Varner Spins and Parities of Low-Lying States in 81Kr from the 80Kr(d(pol), p)81Kr Reaction and Implications for a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 80Kr(polarized d, p), (polarized d, d), E=11 MeV; 80Kr(polarized p, p), E=16 MeV; measured σ(θ), A(θ). 81Kr levels deduced J, π, S. Enriched gas, ion-implanted foil target. Optical model, DWBA analyses.
doi: 10.1016/0375-9474(85)90147-2
1984BU23 Phys.Rev. C30, 742 (1984) B.L.Burks, R.E.Anderson, Y.Aoki, B.C.Karp, E.J.Ludwig, W.J.Thompson, R.L.Varner 81Kr-81Br Ground-State Mass Difference and Implications for Calibration of a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 82Kr(d, t), (d, 3He), E=17 MeV; measured σ(Et), σ(E(3He)); deduced Q-value difference. 81Kr, 81Br deduced mass difference.
doi: 10.1103/PhysRevC.30.742
1984DE01 Nucl.Phys. A414, 113 (1984) J.P.Delaroche, R.L.Varner, T.B.Clegg, R.E.Anderson, B.L.Burks, E.J.Ludwig, J.F.Wilkerson Structure of Low-Lying States of 76,78,80,82Se Deduced from (p(pol), p') Scattering at 16 MeV NUCLEAR REACTIONS 76,78,80,82Se(polarized p, p), (polarized p, p'), E=16 MeV; measured σ(θ), A(θ). 76,78,80,82Se deduced deformation parameters. Coupled-channels calculations.
doi: 10.1016/0375-9474(84)90500-1
1984HA22 Nucl.Phys. A419, 45 (1984) M.Haller, W.Kretschmer, R.E.Anderson, B.L.Burks, T.B.Clegg, E.J.Ludwig, R.L.Varner, J.F.Wilkerson Investigation of the Reactions 58Ni(d, α)56Co and 50Ti(d, α)48Sc with Vector and Tensor Polarized Deuterons NUCLEAR REACTIONS 58Ni, 50Ti(d, α), E=16 MeV; measured σ(θ), relative vector, tensor analyzing power vs θ. 56Co, 48Sc levels deduced L-transfer, J, π. DWBA analysis.
doi: 10.1016/0375-9474(84)90284-7
1982BU01 Nucl.Phys. A377, 105 (1982) B.L.Burks, R.R.Cadmus, Jr., T.B.Clegg, E.J.Ludwig Spins and Parities of Low-Lying States in 79Kr from the 78Kr(d(pol), p)79Kr Reaction NUCLEAR REACTIONS 78Kr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), A(θ). 79Kr deduced levels, J, π, S. Enriched target. DWBA, optical model analyses.
doi: 10.1016/0375-9474(82)90323-2
1982BU03 Phys.Rev. C25, 1168 (1982) B.L.Burks, R.E.Anderson, T.B.Clegg, H.Paetz gen.Schieck, E.J.Ludwig, R.L.Varner, J.F.Wilkerson Test of the Polarization-Analyzing Power Equality in Two (p(pol), d) Reactions and Their Inverses NUCLEAR REACTIONS 11B(polarized p, d), E=11.34-11.94 MeV; 13C(polarized p, d), E=13.79-14.39 MeV; measured analyzing power vs E, θ; deduced no definitive time-reversal invariance violation.
doi: 10.1103/PhysRevC.25.1168
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