NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.O.Sayer Found 54 matches. 2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2006SA17 Phys.Rev. C 73, 044603 (2006) R.O.Sayer, K.H.Guber, L.C.Leal, N.M.Larson, T.Rauscher R-matrix analysis of Cl neutron cross sections up to 1.2 MeV NUCLEAR REACTIONS Cl, 35,37Cl(n, X), E=0.02-1250 keV; analyzed σ. 35,37Cl deduced resonance energies, widths, neutron strength functions. Multilevel Reich-Moore R-matrix formalism, comparison with previous results.
doi: 10.1103/PhysRevC.73.044603
2005GU34 Nucl.Instrum.Methods Phys.Res. B241, 218 (2005) K.H.Guber, L.C.Leal, R.O.Sayer, P.E.Koehler, T.E.Valentine, H.Derrien, J.A.Harvey New neutron cross-section measurements at ORELA and their application in nuclear criticality calculations NUCLEAR REACTIONS 35Cl(n, X), E ≈ 10-1000 keV; measured total σ. Comparison with previous results, other targets discussed.
doi: 10.1016/j.nimb.2005.07.083
2003GU05 Phys.Rev. C 67, 062802 (2003) K.H.Guber, P.E.Koehler, H.Derrien, T.E.Valentine, L.C.Leal, R.O.Sayer, T.Rauscher Neutron capture reaction rates for silicon and their impact on the origin of presolar mainstream SiC grains NUCLEAR REACTIONS 28,29,30Si(n, γ), E=0.1-700 keV; measured capture σ; deduced resonance parameters, astrophysical reaction rates.
doi: 10.1103/PhysRevC.67.062802
2002GU17 Phys.Rev. C65, 058801 (2002) K.H.Guber, R.O.Sayer, T.E.Valentine, L.C.Leal, R.R.Spencer, J.A.Harvey, P.E.Koehler, T.Rauscher New Maxwellian Averaged Neutron Capture Cross Sections for 35, 37Cl NUCLEAR REACTIONS 35,37Cl(n, γ), (n, X), E=0.1-600 keV; measured capture and total σ; deduced parameters, Maxwellian averaged σ, astrophysical reaction rates.
doi: 10.1103/PhysRevC.65.058801
2001GU26 Nucl.Sci.Eng. 139, 111 (2001) K.H.Guber, R.R.Spencer, L.C.Leal, P.E.Koehler, J.A.Harvey, R.O.Sayer, H.Derrien, T.E.Valentine, D.E.Pierce, V.M.Cauley, T.A.Lewis High-Resolution Transmission Measurements of 233U using a Cooled Sample at the Temperature T = 11 K NUCLEAR REACTIONS 233U(n, X), E < 300 keV; measured total σ. High-resolution transmission spectra, comparisons with previous results.
doi: 10.13182/NSE01-A2226
2000GU18 Nucl.Sci.Eng. 135, 141 (2000) K.H.Guber, R.R.Spencer, L.C.Leal, J.A.Harvey, N.W.Hill, G.Dos Santos, R.O.Sayer, D.C.Larson New High-Resolution Fission Cross-Section Measurements of 233U in the 0.4-eV to 700-keV Energy Range NUCLEAR REACTIONS 233U(n, F), E < 700 keV; measured fission σ. High-resolution measurement, comparisons with previous data.
doi: 10.13182/NSE00-A2130
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
1989BE06 Phys.Rev. C39, 1307 (1989) J.R.Beene, F.E.Bertrand, M.L.Halbert, R.L.Auble, D.C.Hensley, D.J.Horen, R.L.Robinson, R.O.Sayer, T.P.Sjoreen Heavy-Ion Excitation and Photon Decay of Giant Resonances in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), E=381 MeV; measured σ(E(17O'), θ(17O')), γ-spectra, γγ(θ). 208Pb deduced giant resonances, decay, γ-branching, B(λ).
doi: 10.1103/PhysRevC.39.1307
1989BR03 Phys.Rev. C39, 725 (1989) A.Bracco, J.R.Beene, F.E.Bertrand, M.L.Halbert, D.C.Hensley, R.L.Auble, D.J.Horen, R.L.Robinson, R.O.Sayer Neutron Decay from the Giant Respnance Region in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O'), E=378 MeV; measured γ-spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1103/PhysRevC.39.725
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
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.
1987LE01 Phys.Rev. C35, 605 (1987) I.Y.Lee, C.Baktash, J.R.Beene, M.P.Fewell, M.L.Halbert, N.R.Johnson, F.K.McGowan, W.T.Milner, H.J.Kim, R.O.Sayer, D.G.Sarantites Distributions of the Total Energy and Multiplicity of Gamma Rays feeding the Discrete Yrast States in Heavy-Ion-Induced Fusion Reactions NUCLEAR REACTIONS 150Sm(12C, 4n), (12C, 3n), E=65 MeV; 100Mo(34S, 4n), E=144 MeV; 70Zn(50Ti, 4n), (50Ti, 3n), E=170 MeV; measured γ-multiplicities, total energy distributions. 158,159Er, 130Ce, 116,117Te deduced entry state distribution width vs yrast transition spin. Ge, NaI detectors, spin spectrometer.
doi: 10.1103/PhysRevC.35.605
1986BE14 Phys.Rev. C34, 45 (1986) F.E.Bertrand, E.E.Gross, D.J.Horen, R.O.Sayer, T.P.Sjoreen, D.K.McDaniels, J.Lisantti, J.R.Tinsley, L.W.Swenson, J.B.McClelland, T.A.Carey, K.Jones, S.J.Seestrom-Morris Giant Resonance Structure in 208Pb Measured using the (p, p') Reaction at 334 MeV NUCLEAR REACTIONS 208Pb(polarized p, p'), E=334 MeV; measured σ(Ep), σ(θ); deduced model parameters. 208Pb deduced giant resonances, Γ, L, EWSR, B(λ). DWBA analysis.
doi: 10.1103/PhysRevC.34.45
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
1982HA25 Phys.Lett. 112B, 327 (1982) J.H.Hamilton, A.V.Ramayya, R.M.Ronningen, R.O.Sayer, H.Yamada, C.F.Maguire, P.Colombani, D.Ward, R.M.Diamond, F.S.Stephens, I.Y.Lee, P.A.Butler, D.Habs Isomeric Trapping following Coulomb Excitation of High Spin States in 178Hf NUCLEAR REACTIONS 178,180Hf(86Kr, 86Kr'), (136Xe, 136Xe'), E=384-594 MeV; 178Hf(136Xe, 136Xe'), E=628, 652, 682 MeV; measured Eγ, Iγ, Coulomb excitation, recoil, Doppler broadening. 178,180Hf levels deduced T1/2, moment of inertia. 178Hf deduced isomer excitation. Cranked shell model calculations.
doi: 10.1016/0370-2693(82)91061-9
1981WE07 Phys.Rev. C24, 171 (1981) J.C.Wells, R.L.Robinson, H.J.Kim, R.O.Sayer, R.B.Piercey, A.V.Ramayya, J.H.Hamilton, C.F.Maguire, K.Kumar, R.W.Eastes, M.E.Barclay, A.J.Caffrey High-Spin States and Band Structure in 76Br NUCLEAR REACTIONS 66Zn(12C, pn), E=38 MeV; measured Eγ, Iγ, γ(θ), linear polarization, γγ-coin. 76Br deduced levels, J, π, δ, γ-branching, rotational band structure. Enriched target, large-volume Ge(Li) detector.
doi: 10.1103/PhysRevC.24.171
1980JO08 Phys.Rev. C22, 2416 (1980) N.R.Johnson, M.W.Guidry, R.J.Sturm, E.Eichler, R.O.Sayer, D.C.Hensley, N.C.Singhal Lifetimes of Rotational States in 154Sm NUCLEAR REACTIONS 154Sm(40Ar, 40Ar'), E=146, 153 MeV; measured Doppler shift, recoil, Coulomb excitation, Eγ, Iγ. 154Sm levels deduced T1/2, B(E2). Ridid rotor model.
doi: 10.1103/PhysRevC.22.2416
1980RO02 Phys.Rev. C21, 603 (1980) R.L.Robinson, H.J.Kim, R.O.Sayer, W.T.Milner, R.B.Piercey, J.H.Hamilton, A.V.Ramayya, J.C.Wells, Jr., A.J.Caffrey High-Spin Levels and Band Structure in 78Kr NUCLEAR REACTIONS 68Zn(12C, 2n), E=33-38 MeV; measured Eγ, Iγ, γ(θ), Doppler broadening, linear polarization. 78Kr levels deduced J, π, δ, γ-branching, T1/2.
doi: 10.1103/PhysRevC.21.603
1980WE07 Phys.Rev. C22, 1126 (1980) J.C.Wells, Jr., R.L.Robinson, H.J.Kim, R.O.Sayer, R.B.Piercey, A.V.Ramayya, J.H.Hamilton, C.F.Maguire High-Spin States and Band Structure in 76Se NUCLEAR REACTIONS 71Ga(7Li, 2n), E=15-22 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), γγ-coin, σ(Eγ). 76Se deduced levels, J, π, δ, T1/2, γ-branching.
doi: 10.1103/PhysRevC.22.1126
1978SA03 Phys.Rev. C17, 1026 (1978) R.O.Sayer, E.Eichler, N.C.Singhal, R.Sturm, N.R.Johnson, M.W.Guidry Recoil-Distance Measurement of Lifetimes of Rotational States in 164Dy NUCLEAR REACTIONS 164Dy(40Ar, 40Ar'), E=152.6 MeV; measured Eγ, recoil distance DSA. 164Dy levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.17.1026
1978SI12 ATOMKI Kozlem. 20, 207 (1978) N.C.Singhal, R.O.Sayer, J.H.Hamilton, A.V.Ramayya, W.T.Milner, R.L.Robinson, N.R.Johnson, G.J.Smith Recoil Distance Lifetime Measurements in 72Se NUCLEAR REACTIONS 58Ni(16O, 2p), E=44-46 MeV; measured DSA. 72Se yrast levels deduced T1/2, B(E2), rms deformation β2.
1978WE15 Phys.Rev. C18, 2162 (1978) J.C.Wells, Jr., R.L.Robinson, H.J.Kim, R.O.Sayer, A.J.Caffrey, R.B.Piercey Linear Polarization Measurements of γ Rays from 64Zn NUCLEAR REACTIONS 59Co(7Li, 2nγ), E=18 MeV; measured γ-polarization. 64Zn levels deduced J, π, δ.
doi: 10.1103/PhysRevC.18.2162
1977MC11 Nucl.Phys. A289, 253 (1977) F.K.McGowan, W.T.Milner, R.O.Sayer, R.L.Robinson, P.H.Stelson Coulomb Excitation of 182,184,186W and 166Er with 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(α, α'γ), E=15 MeV; 186W(16O, 16O'γ), E=42 MeV; 166Er(α, α'γ), E=13.5 MeV; 166Er(16O, 16O'γ), E=42 MeV; measured Iγ, Eγ, γ(θ), αγ-coin, 16Oγ-coin. 182W levels deduced J. 184W levels deduced B(EL), J. 186W levels deduced B(EL), J, quadrupole moment. 166Er deduced quadrupole moment. Enriched, natural targets.
doi: 10.1016/0375-9474(77)90532-2
1977RO28 Phys.Rev. C16, 2268 (1977) R.L.Robinson, H.J.Kim, R.O.Sayer, J.C.Wells, Jr., R.M.Ronningen, J.H.Hamilton High-Spin States in 70Ge NUCLEAR REACTIONS 60Ni(12C, 2p), E=30-39 MeV; 65Cu(7Li, 2n), E=16-19 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), DSA. 70Ge deduced levels, J, π, T1/2, δ, γ-branching.
doi: 10.1103/PhysRevC.16.2268
1977WE10 Phys.Rev. C16, 2259 (1977) J.C.Wells, Jr., L.G.Fugate, R.O.Sayer, R.L.Robinson, H.J.Kim, W.T.Milner, G.J.Smith, R.M.Ronningen High-Spin States in 64Zn NUCLEAR REACTIONS 51V(16O, 2np), E=36-46 MeV; 59Co(7Li, 2n), E=18 MeV; measured Eγ, Iγ, γ(θ), DSA recoil distance. 64Zn deduced levels, J, π, T1/2, δ, γ-branching, B(E2).
doi: 10.1103/PhysRevC.16.2259
1976GU06 Phys.Rev. C13, 1164 (1976) M.W.Guidry, R.J.Sturm, N.R.Johnson, E.Eichler, G.D.O'Kelley, N.C.Singhal, R.O.Sayer Recoil Distance Lifetimes of Rotational States in 236U NUCLEAR REACTIONS 236U(40Ar, 40Ar'γ), E=153, 155 MeV; measured Coulomb excitation. 236U levels deduced T1/2, B(E2), quadrupole moment.
doi: 10.1103/PhysRevC.13.1164
1976HA01 Phys.Rev.Lett. 36, 340 (1976) J.H.Hamilton, H.L.Crowell, R.L.Robinson, A.V.Ramayya, W.E.Collins, R.M.Ronningen, V.Maruhn-Rezwani, J.A.Maruhn, N.C.Singhal, H.J.Kim, R.O.Sayer, T.Magee, L.C.Whitlock Lifetime Measurements to Test the Coexistence of Spherical and Deformed Shapes in 72Se NUCLEAR REACTIONS 58Ni(16O, 2pγ), E=46 MeV; measured γγ-coin, DSA. 72Se levels deduced T1/2, B(E2) ratios.
doi: 10.1103/PhysRevLett.36.340
1976RO06 Phys.Rev. C13, 1922 (1976) R.L.Robinson, H.J.Kim, J.B.McGrory, G.J.Smith, W.T.Milner, R.O.Sayer, J.C.Wells, Jr., J.Lin High-Spin States in 42Ca NUCLEAR REACTIONS 28Si(16O, 2p), E=36-42 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), γ(θ). 42Ca deduced levels, J, π, δ, γ-branching, B(E2).
doi: 10.1103/PhysRevC.13.1922
1976RO08 Nucl.Phys. A261, 439 (1976) R.M.Ronningen, A.V.Ramayya, J.H.Hamilton, W.Lourens, J.Lange, H.K.Carter, R.O.Sayer Mean Life of the 854 keV 0+ State in 74Se and the Coexistence Model RADIOACTIVITY 74Br [from 58Ni(16O, 2p), E=46 MeV]; measured γγ(t). 74Se level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(76)90157-3
1975GU21 Phys.Rev. C12, 1937 (1975) M.W.Guidry, E.Eichler, N.R.Johnson, G.D.O'Kelley, R.J.Sturm, R.O.Sayer Sign of the E4 Moment in 236U by Multiple Coulomb Excitation with 40Ar Ions NUCLEAR REACTIONS 236U(40Ar, 40Ar'), E=145.8, 152.4 MeV; measured multiple coulomb excitation. 236U levels deduced M(E4), sign of E4 moment.
doi: 10.1103/PhysRevC.12.1937
1975JO07 Phys.Rev. C12, 1927 (1975) N.R.Johnson, R.J.Sturm, E.Eichler, M.W.Guidry, G.D.O'Kelley, R.O.Sayer, D.C.Hensley, N.C.Singhal, J.H.Hamilton Lifetimes of Rotational States in 232Th NUCLEAR REACTIONS 232Th(40Ar, 40Ar'γ), E=152 MeV; measured recoil-distance DSA, 40Ar'γ-coin. 232Th levels deduced T1/2, B(E2). Coulomb excitation.
doi: 10.1103/PhysRevC.12.1927
1974HA04 Phys.Rev.Lett. 32, 239 (1974) J.H.Hamilton, A.V.Ramayya, W.T.Pinkston, R.M.Ronningen, G.Garcia-Bermudez, H.K.Carter, R.L.Robinson, H.J.Kim, R.O.Sayer Evidence for Coexistence of Spherical and Deformed Shapes in 72Se RADIOACTIVITY 72Br; measured γγ(t). 72Se level deduced T1/2. NUCLEAR REACTIONS 58Ni(16O, 2pγ), E not given; measured Eγ, Iγ, γ(θ), γγ-coin. 72Se deduced levels, J, π.
doi: 10.1103/PhysRevLett.32.239
1974RI12 Phys.Rev.Lett. 33, 1346 (1974) L.L.Riedinger, G.J.Smith, P.H.Stelson, E.Eichler, G.B.Hagemann, D.C.Hensley, N.R.Johnson, R.L.Robinson, R.O.Sayer Dominance of the i13/2 Neutron in Yb Backbending NUCLEAR REACTIONS 148Nd(22Ne, 5nγ), E=109 MeV; measured Eγ, γγ-coin. 156Gd(12C, 3nγ), E=58 MeV; measured Eγ, γ(θ). 165Yb deduced levels, J, π, decoupled rotational bands.
doi: 10.1103/PhysRevLett.33.1346
1974SA03 Phys.Rev. C9, 1103 (1974) R.O.Sayer, E.Eichler, N.R.Johnson, D.C.Hensley, L.L.Riedinger Coulomb Excitation of Ground Bands in 160,162,164Dy with 20Ne and 35Cl Ions NUCLEAR REACTIONS 160,162,164Dy(35Cl, 35Cl'), E=125 MeV; 160,162,164Dy(20Ne, 20Ne'), E=72 MeV; measured Coulomb excitation yields. 160,162,164Dy levels deduced Eγ, B(E2).
doi: 10.1103/PhysRevC.9.1103
1973EI02 Phys.Rev.Lett. 30, 568 (1973); Erratum Phys.Rev.Lett. 30, 1154 (1973) E.Eichler, N.R.Johnson, R.O.Sayer, D.C.Hensley, L.L.Riedinger Sign of the Hexadecapole Moments of 232Th and 238U Nuclei NUCLEAR REACTIONS 232Th, 238U(40Ar, 40Ar'γ), E=145 MeV; measured Coulomb excitation probabilities. 232Th, 238U deduced E4 matrix elements, B(E2), B(E4).
doi: 10.1103/PhysRevLett.30.568
1973SA02 Priv.Comm. (March 1973); See Also 72Sa39, 72Sa40
1972SA03 Nucl.Phys. A179, 122 (1972) R.O.Sayer, J.K.Temperley, D.Eccleshall Negative Parity Levels in 103Rh via Coulomb Excitation NUCLEAR REACTIONS 103Rh(α, α'γ), E=7-10 MeV; 103Rh(16O, 16O'γ), E=36-45 MeV; measured Iγ, Eγ, Iγ(θ), 16O-γcoin. 103Rh deduced levels, B(E2), B(M1), J.
doi: 10.1016/0375-9474(72)90110-8
1971MI08 Nucl.Phys. A177, 1 (1971) W.T.Milner, F.K.McGowan, R.L.Robinson, P.H.Stelson, R.O.Sayer Coulomb Excitation of 182,184,186W, 186,188,190,192Os and 192,194,196,198Pt with Protons, 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(p, p'γ), E=5 MeV;182,184,186W(α, α'γ), E=14, 15 MeV; 182,184,186W(16O, 16O'γ), E=45.5 MeV; 188,190,192Os(p, p'γ), E=4.56-5.08 MeV; 186Os(α, α'γ), E=3-5 MeV; 188,190,192Os(α, α'γ), E=15 MeV; 186,188,190,192Os(16O, 16O'γ), E=42, 45.1, 45.5 MeV; 192,194,196,198Pt(p, p'γ), E=4.5 MeV; 192,194,196,198Pt(16O, 16O'γ), E=43.75 MeV; measured Iγ, Eγ, (16O)(γ)-coin, 182,184,186W, 186,188,190,192Os, 192,196,194,198Pt deduced B(E2), B(M1), J. Enriched, natural targets.
doi: 10.1016/0375-9474(71)90161-8
1970SA09 Phys.Rev. C1, 1525 (1970) R.O.Sayer, P.H.Stelson, F.K.McGowan, W.T.Milner, R.L.Robinson Multiple Coulomb Excitation of 152Sm, 166Er, and 172,174,176Yb NUCLEAR REACTIONS 152Sm, 166Er, 172,174,176Yb(α, α'γ), E=7, 8, 9, 10 MeV; 152Sm, 166Er, 172,174,176Yb(16O, 16O'γ), E=25-52 MeV; measured σ(E;Eα', Eγ), σ(E;E(16O'), Eγ). 152Sm, 166Er, 172,174,176Yb levels deduced B(E2).
doi: 10.1103/PhysRevC.1.1525
1969MI07 Nucl.Phys. A129, 687 (1969) W.T.Milner, F.K.McGowan, P.H.Stelson, R.L.Robinson, R.O.Sayer Coulomb Excitation of the Even-A Cadmium Nuclei NUCLEAR REACTIONS 106,108,110,112,114,116Cd(p, p'γ), E=2.7, 3.0 MeV; 106,108,110,112,114,116Cd(α, α'γ), E=9-11 MeV; 106,108Cd(16O, 16O'γ), E=42-49 MeV; measured Iγ, Eγ, γγ-coin, γ(θ). 106,108,110,112,114,116Cd deduced levels, B(E2), B(M1), J. Enriched targets.
doi: 10.1016/0375-9474(69)90710-6
1969RO03 Nucl.Phys. A123, 193 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Gamma-Gamma Angular Correlations Following Coulomb Excitation NUCLEAR REACTIONS 107,109Ag, 110Pd, 117Sn(α, α'γ), E=9.5-10 MeV; 190,192Os(p, p'γ), E=4.5 MeV; measured γγ(θ). 107,109Ag, 110Pd, 117Sn, 190,192Os deduced levels, J, γ-mixing ratio. Enriched target.
doi: 10.1016/0375-9474(69)90899-9
1969RO05 Nucl.Phys. A124, 553 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Coulomb Excitation of 106,108,110Pd NUCLEAR REACTIONS 106,108,110Pd(α, α'γ), E=9-10 MeV; 106,108,110Pd(16O, 16O'γ), E=42-49 MeV, measured Iγ, Eγ, γγ-coin., γ(θ). 106,108,110Pd deduced levels B(E2), B(M1), T1/2, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90650-2
1968ST14 Phys.Rev. 170, 1172 (1968) P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, R.O.Sayer Coulomb Excitation of the Even Tin Nuclei NUCLEAR STRUCTURE 112Sn, 118Sn, 116Sn, 120Sn, 122Sn, 124Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.1172
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