NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.G.Stokstad Found 94 matches. 1998MU16 Phys.Rev. C58, 1569 (1998) J.T.Murgatroyd, J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, W.N.Catford, S.P.Fox, G.J.Gyapong, C.D.Jones, D.L.Watson, W.D.M.Rae, Y.Chan, R.G.Stokstad, S.J.Bennett 16O + 8Be Breakup of 24Mg Via the 12C(20Ne, 16O8Be)8Be and 12C(24Mg, 16O8Be)12C Reactions NUCLEAR REACTIONS 12C(20Ne, 8Be16O), E=160 MeV; 12C(24Mg, 8Be16O), E=170 MeV; measured (Be)(O)-coin, angular correlations, excitation energy spectra. 24Mg deduced levels E, J. Comparison with 12C + 12C breakup channel.
doi: 10.1103/PhysRevC.58.1569
1996IS07 Nucl.Phys.(Proc.Suppl.) S48, 244 (1996) M.C.P.Isaac, Y.D.Chan, D.Hurley, K.T.Lesko, R.J.McDonald, M.E.Moorhead, E.B.Norman, A.R.Smith, R.G.Stokstad Preliminary Results from a Study of the Double Beta Decay of 150Nd RADIOACTIVITY 150Nd(2β); measured Eγ, Iγ followed 2ν-accompanied 2β-decay; deduced T1/2 lower limit for decay to 0+ state in 150Sm.
doi: 10.1016/0920-5632(96)00251-4
1995MU03 Phys.Rev. C51, 2230 (1995) J.T.Murgatroyd, S.J.Bennett, B.R.Fulton, J.S.Pople, N.S.Jarvis, D.L.Watson, W.D.M.Rae, Y.Chan, D.DiGregorio, J.Scarpaci, J.Suro Perez, R.G.Stokstad Evidence for 16O + 12C Cluster Structure in 28Si NUCLEAR REACTIONS 12C(20Ne, 12C16O), E=160 MeV; measured (12C)(16O)-coin total energy spectra. 28Si levels deduced 12C + 16O cluster structure, shape features.
doi: 10.1103/PhysRevC.51.2230
1995SC30 Phys.Rev. C52, 764 (1995) J.A.Scarpaci, Y.Chan, D.DiGregorio, B.A.Harmon, J.Pouliot, R.G.Stokstad, J.Suro Central Collisions in the 16O + 12C Reaction at 32.5 MeV/nucleon NUCLEAR REACTIONS 12C(16O, X), E=32.5 MeV/nucleon; measured fusion, incomplete fusion fragment velocity, total kinetic energy spectra, yields. Incomplete fusion followed by statistical decay.
doi: 10.1103/PhysRevC.52.764
1995WI20 Phys.Rev. C52, 1028 (1995) F.E.Wietfeldt, E.B.Norman, Y.D.Chan, M.T.F.da Cruz, A.Garcia, E.E.Haller, W.L.Hansen, M.M.Hindi, R.-M.Larimer, K.T.Lesko, P.N.Luke, R.G.Stokstad, B.Sur, I.Zlimen Further Studies on the Evidence for a 17-keV Neutrino in a 14C-Doped Germanium Detector RADIOACTIVITY 14C(β-); measured β-endpoint energy; deduced Qβ, no 17 keV neutrino evidence. Source doping of Ge detector.
doi: 10.1103/PhysRevC.52.1028
1994FU01 J.Phys.(London) G20, 151 (1994) B.R.Fulton, S.J.Bennett, J.T.Murgatroyd, N.S.Jarvis, D.L.Watson, W.D.M.Rae, Y.Chan, D.DiGregorio, J.Scarpaci, J.Suro Perez, R.G.Stokstad Resonances in 24Mg Revealed in the 12C(20Ne, 12C12C)8Be Reaction NUCLEAR REACTIONS 12C(20Ne, 212C), E=160 MeV; measured coincident 12C nuclei total energy spectra. 24Mg deduced excited state population, breakup mechanism.
doi: 10.1088/0954-3899/20/1/015
1994PO19 Z.Phys. A349, 349 (1994) J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, J.T.Murgatroyd, Y.Chan, R.G.Stokstad, W.D.M.Rae, W.N.Catford, S.P.Fox, G.J.Gyapong, D.L.Watson, S.J.Bennett, and the Charissa Collaboration The Breakup of 24Mg into 16O and 8Be NUCLEAR REACTIONS 12C(24Mg, 8Be16O), E=170 MeV; 12C(20Ne, 8Be16O), E=160 MeV; measured breakup spectra; deduced reaction mechanism. 24Mg deduced breakup level configuration, shape features.
1993CH24 Phys.Rev. C48, 699 (1993) E.Chavez-Lomeli, A.Dacal, M.E.Oritz, S.B.Gazes, Y.Chan, R.G.Stokstad, E.Plagnol, K.Siwek-Wilczynska, J.Wilczynski 16O Breakup in Quasielastic Reactions Near the Fermi Energy NUCLEAR REACTIONS 197Au(16O, X), E=32.5 MeV/nucleon; measured (fragment)(fragment)-coin; deduced projectile breakup mechanism, σ for breakup into α+12C and other channels. Monte Carlo simulations.
doi: 10.1103/PhysRevC.48.699
1993DA19 Phys.Rev. C48, 3106 (1993) M.T.F.da Cruz, D.W.Bardayan, Y.Chan, A.Garcia, M.M.Hindi, R.-M.Larimer, K.T.Lesko, E.B.Norman, D.F.Rossi, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Thick-Target Yields of Iodine Isotopes from Proton Interactions in Te, and the Double-β Decays of 128,130Te NUCLEAR REACTIONS, ICPND 126,128,130Te(p, xn)126I/128I/130I, E=15-50 MeV; measured thick target residuals yields. 126,128,130Te(p, xn)126I/128I/130I, E=1.85, 5 GeV; measured residuals production σ; deduced revised correction for cosmic ray production of 126,128,130Xe ores, 120,128Te 2β-decay T1/2 implications. Activation technique, Ge detector.
doi: 10.1103/PhysRevC.48.3106
1993DA20 Phys.Rev. C48, 3110 (1993) M.T.F.da Cruz, Y.Chan, A.Garcia, M.M.Hindi, G.Kenchian, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Search for the β+ Decay of 54Mn RADIOACTIVITY 54Mn(β+); measured γγ-coin; deduced log ft. 54Cr levels deduced Iβ+ limit. Source as cosmic ray chronometer discussed. Hyperpure Ge detectors.
doi: 10.1103/PhysRevC.48.3110
1993GA09 Phys.Rev. C47, 2910 (1993) A.Garcia, Y.-D.Chan, M.T.F.da Cruz, R.M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen, D.M.Moltz, J.Batchelder, T.J.Ognibene, M.M.Hindi Electron-Capture Decay of 100Tc and the Double-β Decay of 100Mo RADIOACTIVITY 100Tc(EC) [from 100Mo(p, n), E=9 MeV]; measured Eγ, Iγ, E X-ray, I X-ray; deduced log ft, T1/2. 100Mo deduced two-step process role in 2ν-accompanied 2β-decay, T1/2.
doi: 10.1103/PhysRevC.47.2910
1993WI05 Phys.Rev.Lett. 70, 1759 (1993) F.E.Wietfeldt, Y.D.Chan, M.T.F.da Cruz, A.Garcia, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, I.Zlimen Search for a 17 keV Neutrino in the Electron-Capture Decay of 55Fe RADIOACTIVITY 55Fe(EC); measured internal bremsstrahlung γ spectra; deduced no evidence for 5-25 keV mass neutrino. Chemically purified 55Fe sample, coaxial Ge detector.
doi: 10.1103/PhysRevLett.70.1759
1992BE01 Phys.Rev. C45, 677 (1992) M.Begemann-Blaich, Th.Blaich, M.M.Fowler, J.B.Wilhelmy, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, D.J.Massoletti, M.N.Namboodiri, B.A.Remington, T.C.Sangster, G.L.Struble, M.L.Webb, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel Fission from Fe and Nb Reactions with Heavy Targets at 50-100 MeV/Nucleon NUCLEAR REACTIONS Ta, 197Au, Th(Fe, F), (93Nb, F), E=50-100 MeV/nucleon; measured fission σ, charge loss distribution, fragment velocity systematics, momentum transfers. Peripheral collisions, model analysis.
doi: 10.1103/PhysRevC.45.677
1992DA15 Phys.Rev. C46, 1132 (1992) M.T.F.da Cruz, Y.Chan, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Half-Life of 56Ni RADIOACTIVITY 56Ni(EC) [from 56Fe(3He, 3n), E=50 MeV]; measured Eγ, Iγ, time dependent γ yields; deduced T1/2.
doi: 10.1103/PhysRevC.46.1132
1992PA15 Phys.Rev. C45, 2861 (1992) A.J.Pacheco, J.O.Fernandez Niello, D.E.DiGregorio, M.diTada, J.E.Testoni, Y.Chan, E.Chavez, S.Gazes, E.Plagnol, R.G.Stokstad Capture Reactions in the 40,48Ca + 197Au and 40,48Ca + 208Pb Systems NUCLEAR REACTIONS 208Pb, 197Au(40Ca, F), (48Ca, F), E=195-416 MeV; measured capture fission fragment σ(θ), σ vs E; deduced isotopic dependence. Extra push model, coupled-channels analyses.
doi: 10.1103/PhysRevC.45.2861
1992SA15 Phys.Rev. C46, 1404 (1992) T.C.Sangster, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, M.N.Namboodiri, B.A.Remington, M.L.Webb, M.Begemann-Blaich, T.Blaich, M.M.Fowler, J.B.Wilhelmy, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel, G.Peilert, H.Stocker, W.Greiner, A.Botvina, I.N.Mishustin Intermediate Mass Fragment Emission in Fe + Au Collisions NUCLEAR REACTIONS 197Au(Fe, X), E=50-100 MeV/nucleon; measured σ(fragment θ), charge, velocity distributions; deduced intermediate mass fragment production mechanism. Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.46.1404
1992SU13 Nucl.Phys. A548, 353 (1992) J.Suro, Y.D.Chan, J.A.Scarpaci, R.G.Stokstad, K.Mohring, T.C.Schmidt Projectile Breakup of 16O at 32.5 MeV/A Comparison of a Classical Dynamical Model with Experiment NUCLEAR REACTIONS 197Au(16O, 4α), E=32.5 MeV/nucleon; measured multiple breakup of projectile. Comparison with classical dynamical reaction model.
doi: 10.1016/0375-9474(92)90015-C
1992ZL01 Phys.Rev. C46, 1136 (1992) I.Zlimen, E.Browne, Y.Chan, M.T.F.da Cruz, A.Garcia, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt Second-Forbidden Electron-Capture Decay of 55Fe RADIOACTIVITY 55Fe(EC); measured I gamma; deduced log ft, decay characteristics. 55Mn level deduced branching.
doi: 10.1103/PhysRevC.46.1136
1991DI01 Phys.Rev. C43, 265 (1991) Systematic Analysis of Average Angular Momenta and Cross Sections in Sub-Barrier Fusion NUCLEAR REACTIONS, ICPND 144Nd, 154Sm(16O, X), 154Sm(28Si, X), 128Te(12C, X), 80Se(80Se, X), 96Zr, 100Mo(64Ni, X), 232Th(19F, X), 136,137Ba(3He, X), 136Ba(α, X), E not given; analyzed fusion σ, γ-multiplicity, isomer σ ratio data. 208Pb, 232Th(16O, F), 238U(12C, F), 232Th(19F, F), E not given; analyzed fission data. Barrier penetration model.
doi: 10.1103/PhysRevC.43.265
1991DI02 Phys.Rev. C43, 687 (1991) D.E.DiGregorio, Y.Chan, E.Chavez, A.Dacal, M.E.Ortiz, J.Suro, R.G.Stokstad Fusion Cross Sections for 12C + 128Te and the Deduction of Absolute Average Angular Momenta NUCLEAR REACTIONS, ICPND 128Te(12C, X), E(cm)=40.4-56.6 MeV; measured fusion σ(E); deduced absolute average angular momenta. TOF technique, multiwire proportional gaseous counters. Coupled-channels model, sharp cutoff approximation.
doi: 10.1103/PhysRevC.43.687
1991PO01 Phys.Rev. C43, 735 (1991) J.Pouliot, Y.Chan, D.E.DiGregorio, B.A.Harmon, R.Knop, C.Moisan, R.Roy, R.G.Stokstad Excitation and Multiple Dissociation of 12C, 14N, and 16O Projectiles in Peripheral Collisions at 32.5 MeV/Nucleon NUCLEAR REACTIONS 197Au(16O, X), (12C, X), (14N, X), E=32.5 MeV/nucleon; measured fragment yields; deduced projectile dissociation mechanism.
doi: 10.1103/PhysRevC.43.735
1990DI10 Phys.Rev. C42, 2108 (1990) D.E.DiGregorio, K.T.Lesko, B.A.Harmon, E.B.Norman, J.Pouliot, B.Sur, Y.Chan, R.G.Stokstad Angular Momentum in Sub-Barrier Fusion: Experimental study using the isomer ratio 137mCe/137gCe NUCLEAR REACTIONS, ICPND 128Te(12C, 3n), 133Cs(7Li, 3n), 137,136Ba(3He, 2n), 136Ba(α, 3n), 137Ba(3He, 3n), E=2.7-9.5 MeV/nucleon; measured 137mCe/137gCe isomer ratio, 3n, 2n reaction σ(E); deduced absolute average angular momentum for fusion. Coupled-channels model, statistical decay model calculations. Activation technique.
doi: 10.1103/PhysRevC.42.2108
1990HA05 Phys.Lett. 235B, 234 (1990) B.A.Harmon, J.Pouliot, J.A.Lopez, J.Suro, R.Knop, Y.Chan, D.E.Digregorio, R.G.Stokstad Kinematic Signatures of the Projectile Breakup Process at 32.5 MeV/Nucleon NUCLEAR REACTIONS 197Au(16O, X), E=32.5 MeV/nucleon; measured (particle)(particle)-correlation; deduced projectile breakup mechanism. Lopez-Randrup model.
doi: 10.1016/0370-2693(90)91956-C
1989DI01 Phys.Rev. C39, 516 (1989) D.E.DiGregorio, M.diTada, D.Abriola, M.Elgue, A.Etchegoyen, M.C.Etchegoyen, J.O.Fernandez Niello, A.M.J.Ferrero, S.Gil, A.O.Macchiavelli, A.J.Pacheco, J.E.Testoni, P.R.Silveira Gomes, V.R.Vanin, R.Liguori Neto, E.Crema, R.G.Stokstad Subbarrier Fusion of 16O + 147,149Sm NUCLEAR REACTIONS, ICPND 147,149Sm(16O, X), (16O, n), (16O, 3n), (16O, 4n), (16O, xnα), E=61-75 MeV; measured fusion σ(E), residual relative yield vs E.
doi: 10.1103/PhysRevC.39.516
1989PL02 Phys.Lett. 221B, 11 (1989) E.Plagnol, L.Vinet, D.R.Bowman, Y.D.Chan, R.J.Charity, E.Chavez, S.B.Gazes, H.Han, W.L.Kehoe, M.A.McMahan, L.G.Moretto, R.G.Stokstad, G.J.Wozniak, G.Auger Where has all the Fusion Gone...( Question ) NUCLEAR REACTIONS 12C, 27Al(40Ar, X), E=19.7 MeV/nucleon; measured σ(fragment θ), yields, charge distributions, kinetic energy spectra; deduced reaction mechanisms.
doi: 10.1016/0370-2693(89)90182-2
1989PO07 Phys.Lett. 223B, 16 (1989) J.Pouliot, Y.Chan, A.Dacal, D.E.DiGregorio, B.A.Harmon, R.Knop, M.E.Oritz, E.Plagnol, R.G.Stokstad, C.Moisan, L.Potvin, C.Rioux, R.Roy Excitation and Multiple Dissociation of 16O, 14N and 12C Projectiles at 32.5 MeV per Nucleon NUCLEAR REACTIONS 197Au(16O, X), (14N, X), (12C, X), E=32.5 MeV/nucleon; measured fragment angle-integrated spectra.
doi: 10.1016/0370-2693(89)90911-8
1989PO08 Nucl.Phys. A495, 223c (1989) J.Pouliot, Y.D.Chan, A.Dacal, D.E.DiGregorio, B.A.Harmon, R.Knop, M.E.Oritz, E.Plagnol, R.G.Stokstad, R.Roy, C.Moisan, L.Potvin, C.Rioux Multiple Dissociation of 16O, 14N and 12C at 32.5 MeV/Nucleon NUCLEAR REACTIONS 197Au(12C, X), (14N, X), (16O, X), E=32.5 MeV/nucleon; measured multiple dissociation channel yields; deduced projectile breakup mechanism.
doi: 10.1016/0375-9474(89)90321-7
1989ST02 Phys.Rev.Lett. 62, 399 (1989) R.G.Stokstad, D.E.DiGregorio, K.T.Lesko, B.A.Harmon, E.B.Norman, J.Pouliot, Y.D.Chan Observation of a Constant Average Angular Momentum for Fusion at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 128Te(12C, 3n), E(cm)=34.5-50 MeV; measured σ(E); deduced isomer ratio.
doi: 10.1103/PhysRevLett.62.399
1988GA11 Phys.Lett. 208B, 194 (1988) S.B.Gazes, Y.D.Chan, E.Chavez, A.Dacal, M.E.Ortiz, K.Siwek-Wilczynska, J.Wilczynski, R.G.Stokstad Neutron Pickup and Four-Body Processes in Reactions of 16O - 197Au at 26.5 and 32.5 MeV/Nucleon NUCLEAR REACTIONS 197Au(16O, X), E=424, 520 MeV; measured (particle)(particle)-coin; deduced reaction mechanism.
doi: 10.1016/0370-2693(88)90416-9
1988GA12 Phys.Rev. C38, 712 (1988) S.B.Gazes, H.R.Schmidt, Y.Chan, E.Chavez, R.Kamermans, R.G.Stokstad Stripping- and Pickup-Induced Breakup in 11- and 17-MeV/Nucleon 20Ne + 197Au Reactions NUCLEAR REACTIONS 197Au(20Ne, X), E=220, 341 MeV; measured (fragment)p-, (fragment)α-coin; deduced reaction mechanism, projectile breakup.
doi: 10.1103/PhysRevC.38.712
1987SI06 Phys.Rev. C35, 1316 (1987) K.Siwek-Wilczynska, J.Wilczynski, C.R.Albiston, Y.Chan, E.Chavez, S.B.Gazes, H.R.Schmidt, R.G.Stokstad Projectile-Breakup and Transfer-Reemission Reactions in the 12C + 20Ne System NUCLEAR REACTIONS 12C(20Ne, α16O), 12C(20Ne, α20Ne), 12C(20Ne, α12C), E=157 MeV; measured (particle)(particle)-coin; deduced reaction mechanism. 20Ne, 16O, 24Mg deduced excitation energy.
doi: 10.1103/PhysRevC.35.1316
1986DI08 Phys.Lett. 176B, 322 (1986) D.E.Di Gregorio, J.O.Fernandez Niello, A.J.Pacheco, D.Abriola, S.Gil, A.O.Macchiavelli, J.E.Testoni, P.R.Pascholati, V.R.Vanin, R.Liguori Neto, N.Carlin Filho, M.M.Coimbra, P.R.Silveira Gomes, R.G.Stokstad Fusion of 16O + 144Sm at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E=63-72 MeV; measured (X-ray)(t); deduced fusion σ(E).
doi: 10.1016/0370-2693(86)90172-3
1986SC29 Phys.Lett. 180B, 9 (1986) H.R.Schmidt, S.B.Gazes, Y.Chan, R.Kamermans, R.G.Stokstad Partition of Excitation Energy in Peripheral Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(20Ne, αX), E=220 MeV; measured α(projectile-like fragment)-coin; deduced excitation energy partition, mass transfer direction correlation.
doi: 10.1016/0370-2693(86)90124-3
1986WI14 Phys.Lett. 181B, 229 (1986) J.Wilczynski, K.Siwek-Wilczynska, Y.Chan, E.Chavez, S.B.Gazes, R.G.Stokstad 12C Decay of 24Mg following Nuclear Inelastic Scattering NUCLEAR REACTIONS 12C(24Mg, 212C), E=15 MeV/nucleon; measured total energy spectrum, σ(θ), (12C)(12C)(θ). 24Mg level deduced J, π, 12C-decay characteristics. ΔE, position sensitive detectors.
doi: 10.1016/0370-2693(86)90037-7
1985BU16 Phys.Rev. C32, 1534 (1985) A.Budzanowski, H.Dabrowski, Y.Chan, R.G.Stokstad, I.Tserruya, S.Wald Momentum Balance for the Incomplete Fusion 16O + 40Ca NUCLEAR REACTIONS 40Ca(16O, X), E=313 MeV; measured σ(fusion residue θ, θα) vs fragment velocity; deduced projectile breakup mechanism.
doi: 10.1103/PhysRevC.32.1534
1985SC28 Nucl.Instrum.Methods 242, 111 (1985) H.R.Schmidt, M.Bantel, Y.Chan, S.B.Gazes, S.Wald, R.G.Stokstad A Segmented Position-Sensitive Plastic Phoswich Detector NUCLEAR REACTIONS 197Au(20Ne, α16O), (20Ne, 2α12C), E=11 MeV/nucleon; measured α(16O)-coin, energy correlations, αα12C-coin. Segmented position sensitive plastic phoswich detector.
doi: 10.1016/0168-9002(85)90894-0
1985WA22 Phys.Rev. C32, 894 (1985) S.Wald, S.B.Gazes, C.R.Albiston, Y.Chan, B.G.Harvey, M.J.Murphy, I.Tserruya, R.G.Stokstad, P.J.Countryman, K.Van Bibber, H.Homeyer Transfer and Breakup Processes in Reactions of 11- and 17-MeV/nucleon 20Ne + 197Au NUCLEAR REACTIONS 197Au(20Ne, X), E=220, 341 MeV; measured σ(fragment E, θ, Z) for X=Li, Be, B, C, N, O, F; deduced transfer, breakup, primary ejectile yields. Coincidence techniques.
doi: 10.1103/PhysRevC.32.894
1984GO05 Phys.Rev. C29, 1722 (1984) J.Gomez del Campo, J.A.Biggerstaff, R.A.Dayras, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad Comparison of Fusion Cross Sections for the 10B + 16O and 12C + 14N Systems NUCLEAR REACTIONS, ICPND 12C(14N, X), E=158, 248 MeV; 10B(16O, X), E=203.6 MeV; measured σ(fragment θ, E) for fragment Z=3, 10, fusion, reaction, direct σ(E), fragment velocity spectra. 16O(10B, X), E=42-169.7 MeV; measured fusion, reaction σ(E). 10B(16O, X), E=203.6 MeV; measured evaporation residue σ(θ). 12C(14N, X), E=182 MeV; measured evaporation residue relative yield. Monte Carlo Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.29.1722
1984GR20 Phys.Rev. C30, 1214 (1984) K.Grotowski, Z.Majka, R.Planeta, M.Szczodrak, Y.Chan, G.Guarino, L.G.Moretto, D.J.Morrissey, L.G.Sobotka, R.G.Stokstad, I.Tserruya, S.Wald, G.J.Wozniak Symmetric Splitting of very Light Systems NUCLEAR REACTIONS, ICPND 40Ca(6Li, X), E=153 MeV; 40Ca(9Be, X), E=141 MeV; 40Ca(12C, X), E=74-185 MeV; measured (fragment)(fragment)-coin, σ(fragment θ, E), σ(fragment θ, E, Z), angular, energy, charge correlations, σ(θ1, θ2); deduced symmetric mass split σ(E). 52Fe, 49Cr, 46V deduced near symmetric breakup.
doi: 10.1103/PhysRevC.30.1214
1984RA10 Phys.Rev. C30, 158 (1984) W.D.M.Rae, A.J.Cole, B.G.Harvey, R.G.Stokstad Breakup of 16O and 20Ne at 9 MeV/Nucleon NUCLEAR REACTIONS 12,13C, 28Si(16O, 16O'), (16O, 20Ne), E=140 MeV; 12C(20Ne, 20Ne), E=175 MeV; measured relative E spectra, α(12C)-, α(16O)-coin; deduced ejectile sequential breakup role.
doi: 10.1103/PhysRevC.30.158
1983CH04 Phys.Rev. C27, 447 (1983) Y.Chan, M.Murphy, R.G.Stokstad, I.Tserruya, S.Wald, A.Budzanowski Onset of Nonequilibrium Phenomena in Fusionlike Processes for 16O-Induced Reactions NUCLEAR REACTIONS 27Al, 40Ca, 60Ni(16O, X), E=8.8, 13.6, 19.6 MeV/nucleon; measured evaporation residue velocity distribution; deduced linear momentum transfer, reaction mechanism. Statistical model.
doi: 10.1103/PhysRevC.27.447
1983MU08 Phys.Rev. C28, 428 (1983) Momentum Widths of Heavy-Ion Reaction Products at 27.4 MeV/Nucleon NUCLEAR REACTIONS Au(9Be, 6LiX), (9Be, 7LiX), E=27 MeV/nucleon; measured inclusive σ(E(Li)); deduced ejectile momentum widths.
doi: 10.1103/PhysRevC.28.428
1983SH25 Phys.Rev. C28, 1148 (1983) D.Shapira, D.DiGregorio, J.Gomez del Campo, R.A.Dayras, J.L.C.Ford, Jr., A.H.Snell, P.H.Stelson, R.G.Stokstad, F.Pougheon Fusion and Peripheral Processes in the Collisions of 20Ne + 20Ne and 20Ne + 16O NUCLEAR REACTIONS, ICPND 20Ne, 16O(20Ne, 20Ne), (20Ne, X), E=80-160 MeV; measured elastic σ, σ(fragment θ, E), σ(θ) for Z=6, 7, 8, 9, fusion σ(E), reaction σ, deep inelastic σ; deduced fusion potential parameters, entrance channel effects. Monte Carlo simulation.
doi: 10.1103/PhysRevC.28.1148
1983SO08 Phys.Rev.Lett. 51, 2187 (1983) L.G.Sobotka, M.L.Padgett, G.J.Wozniak, G.Guarino, A.J.Pacheco, L.G.Moretto, Y.Chan, R.G.Stokstad, I.Tserruya, S.Wald Compound-Nucleus Decay via the Emission of Heavy Nuclei NUCLEAR REACTIONS Ag(3He, α), (3He, 7Be), (3He, 9Be), E=90 MeV; measured σ(θ), σ(θ, Eα), σ(θ, E(Be)). Ag(3He, X), E=90 MeV; measured σ(fragment E), σ(fragment θ), σ(fragment Z) for X=B, C, N, O; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.51.2187
1982OR02 Phys.Rev. C25, 1436 (1982) M.E.Ortiz, J.Gomez del Campo, Y.D.Chan, D.E.DiGregorio, J.L.C.Ford, D.Shapira, R.G.Stokstad, J.P.F.Sellschop, R.L.Parks, D.Weiser Fusion, Direct, and Total Reaction Cross Sections of the 10B + 14N System up to E(14N) = 180 MeV NUCLEAR REACTIONS, ICPND 10B(14N, X), E=86-180 MeV; measured σ(fragment θ, E) for Z=3-11; deduced fusion σ, total σ, direct σ, grazing (L), critical (J) vs E. Optical, entrance channel model analyses.
doi: 10.1103/PhysRevC.25.1436
1981CO22 Phys.Rev.Lett. 47, 1705 (1981) A.J.Cole, W.D.M.Rae, M.E.Brandan, A.Dacal, B.G.Harvey, R.Legrain, M.J.Murphy, R.G.Stokstad 12C + 12C Reaction Cross Section between 70 and 290 MeV Obtained from Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=120-290 MeV; measured σ(θ) vs momentum transfer; deduced σ(total), σ(reaction).
doi: 10.1103/PhysRevLett.47.1705
1981RA20 Phys.Lett. 105B, 417 (1981) W.D.Rae, A.J.Cole, A.Dacal, R.Legrain, B.G.Harvey, J.Mahoney, M.J.Murphy, R.G.Stokstad, I.Tserruya Coherent and Incoherent Processes in Projectile Breakup NUCLEAR REACTIONS 12,13C, 28Si(16O, α12C), E=140 MeV; measured 12Cα-coin, total, relative energies of fragments; deduced coherent, incoherent projectile breakup.
doi: 10.1016/0370-2693(81)91195-3
1981ST01 Phys.Rev. C23, 281 (1981) Analysis of the Sub-Barrier Fusion of 16O + 148,150,152,154Sm NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; analyzed σ(fusion) data. Coupled-channel analysis, static deformation, dynamic effects, sub-barrier fusion.
doi: 10.1103/PhysRevC.23.281
1980DA14 Phys.Rev. C22, 1485 (1980) R.A.Dayras, R.G.Stokstad, D.C.Hensley, M.L.Halbert, D.G.Sarantites, L.Westerberg, J.H.Barker Angular Momentum Transfer in the Reactions Induced by 166 MeV 20Ne on 63Cu NUCLEAR REACTIONS 63Cu(20Ne, X), E=166 MeV; measured σ(fragment E, θ, Z), γ-ray multiplicity, Xγ(θ); deduced relaxation times, diffusion coefficients, random angular momentum. 63Cu(12C, X), E=133 MeV; measured γ-ray multiplicity. Enriched target.
doi: 10.1103/PhysRevC.22.1485
1980RA12 Phys.Rev.Lett. 45, 884 (1980) W.D.Rae, R.G.Stokstad, B.G.Harvey, A.Dacal, R.Legrain, J.Mahoney, M.J.Murphy, T.J.M.Symons Molecular Resonances and the Production of Fast α Particles in the Reaction of 16O with 12,13C Nuclei NUCLEAR REACTIONS 12,13C(16O, α), E=140 MeV; measured α12C-coin; deduced no molecular resonance or final-state interaction between carbon ions. 16O levels deduced excitation, decay probabilities.
doi: 10.1103/PhysRevLett.45.884
1980SA25 Nucl.Phys. A346, 179 (1980) G.R.Satchler, M.L.Halbert, R.G.Stokstad, R.M.Devries, D.A.Goldberg, J.G.Cramer Energy Dependence in 12C + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(12C, 12C), E=131.5 MeV; measured σ(θ); deduced optical model potentials. Enriched targets. Optical model analyses.
doi: 10.1016/0375-9474(80)90496-0
1980SI15 Phys.Rev. C22, 1971 (1980) R.Singh, K.A.Eberhard, R.G.Stokstad Fluctuations in 12C(16O, α)24Mg and 12C(16O, 8Be(g.s.))20Ne Reactions NUCLEAR REACTIONS 12C(16O, α), E=13.17-23.09 MeV; 12C(16O, 8Be), E(cm)=14.07-23.09 MeV; measured σ(E, θ); deduced fluctuation component of σ. Statistical model analysis.
doi: 10.1103/PhysRevC.22.1971
1980ST09 Phys.Rev. C21, 2427 (1980) R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya Fusion of 16O + 148,150,152,154Sm at Sub-Barrier Energies NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured evaporation residue Eγ, E(K X-ray), I(K X-ray); deduced fusion σ(E).
doi: 10.1103/PhysRevC.21.2427
1980ST11 Z.Phys. A295, 269 (1980) R.G.Stokstad, W.Reisdorf, K.D.Hildenbrand, J.V.Kratz, G.Wirth, R.Lucas, J.Poitou The Sub-Barrier Fusion of 40Ar with 144,148,154Sm NUCLEAR REACTIONS 144,148,154Sm(40Ar, X), E=3.6-4.5 MeV/nucleon; measured I(K X-ray)(t, fragment E); deduced evaporation-residue production σ, fusion-fission σ. ΔE-E ionization chamber.
doi: 10.1007/BF01412207
1979DA01 Phys.Rev.Lett. 42, 697 (1979) R.A.Dayras, R.G.Stokstad, C.B.Fulmer, D.C.Hensley, M.L.Halbert, R.L.Robinson, A.H.Snell, D.G.Sarantites, L.Westerberg, J.H.Barker Randomly Oriented Angular Momentum in Strongly Damped Collisions NUCLEAR REACTIONS 63Cu(Ne, Xγ), E=168 MeV; measured γ-ray multiplicity, width, skewness of multiplicity distribution, Iγ(φ); deduced a random component in transferred angular momentum.
doi: 10.1103/PhysRevLett.42.697
1979FU04 Phys.Rev. C20, 670 (1979) C.B.Fulmer, R.M.Wieland, D.C.Hensley, S.Raman, G.R.Satchler, A.H.Snell, P.H.Stelson, R.G.Stokstad 12C + 12C Transfer Reactions at 93.8 MeV NUCLEAR REACTIONS 12C(12C, 11C), (12C, 11B), (12C, 10B), E=93.8 MeV; measured σ(θ). 13C, 13N levels deduced S. DWBA analysis.
doi: 10.1103/PhysRevC.20.670
1979GO09 Phys.Rev.Lett. 43, 26 (1979) J.Gomez del Campo, R.A.Dayras, J.A.Biggerstaff, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad Comparison of Fusion Cross Sections for 10B + 16O → 26Al and 12C + 14N → 26Al NUCLEAR REACTIONS 10B(16O, X), E(cm)=15-80 MeV; measured σ(fusion, E), σ(direct, E).
doi: 10.1103/PhysRevLett.43.26
1979GO11 Phys.Rev. C19, 2170 (1979) J.Gomez del Campo, R.G.Stokstad, J.A.Biggerstaff, R.A.Dayras, A.H.Snell, P.H.Stelson Fusion and Peripheral Reactions of 12C + 14N at Energies up to 13 MeV/A NUCLEAR REACTIONS 12C(14N, X), E=34.1-178.1 MeV; measured σ(θ) of evaporation residues; deduced fusion, direct, total σ. Hauser-Feshbach, optical model calculations.
doi: 10.1103/PhysRevC.19.2170
1979MI01 Phys.Rev. C19, 100 (1979) R.Middleton, R.R.Betts, H.T.Fortune, R.G.Stokstad Energy-Averaged Angular Distributions for 16O + 12C → α + 24Mg NUCLEAR REACTIONS 16O(12C, α), E=22.5-25.5 MeV; 12C(16O, α), E=30-34 MeV; measured σ(Eα, θ); deduced energy-averaged σ. 24Mg levels deduced no evidence for direct reaction mechanism. Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.19.100
1979RU06 Nucl.Phys. A330, 243 (1979) G.Rudolf, A.Gobbi, H.Stelzer, U.Lynen, A.Olmi, H.Sann, R.G.Stokstad, D.Pelte Energy Loss and Nucleon Exchange in the Reaction of 86Kr with 166Er NUCLEAR REACTIONS 166Er(86Kr, X), E=8.18 MeV/nucleon; measured σ(θ, E, fragment) for Z=20-52; deduced number of nucleon exchanges.
doi: 10.1016/0375-9474(79)90548-7
1979SH18 Phys.Rev.Lett. 43, 1781 (1979) D.Shapira, J.L.C.Ford, Jr., J.Gomez del Campo, R.G.Stokstad, R.M.DeVries Orbiting in the 12C + 20Ne System NUCLEAR REACTIONS 12C(20Ne, 11C), (20Ne, 13C), (20Ne, 16O), (20Ne, 20Ne'), E=50-80 MeV; measured σ(E, θ); deduced reaction mechanism.
doi: 10.1103/PhysRevLett.43.1781
1979SH22 Nucl.Instrum.Methods 163, 325 (1979) D.Shapira, R.Dayras, J.L.C.Ford, Jr., J.Gomez del Campo, A.H.Snell, P.H.Stelson, R.G.Stokstad A Gas Cell Target for Studying Fusion and Damped Collisions of Light Nuclei NUCLEAR REACTIONS 20Ne(20Ne, X), E(cm)=83 MeV; measured fusion σ(θ). 16O(20Ne, X), E=131 MeV; measured evaporation residue energy for 12C, 14N, 16O, 19F, 20Ne, 23Na, 24Mg, 27Al, 28Si, 31P, 32S.
doi: 10.1016/0029-554X(79)90115-0
1979ST10 Phys.Rev. C20, 655 (1979) R.G.Stokstad, R.M.Wieland, G.R.Satchler, C.B.Fulmer, D.C.Hensley, S.Raman, L.D.Rickertsen, A.H.Snell, P.H.Stelson Elastic and Inelastic Scattering of 12C by 12C from E = 35-63 MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E(cm)=35-63 MeV; measured σ(E, θ). Optical model, DWBA, coupled-channels analysis.
doi: 10.1103/PhysRevC.20.655
1978GO04 Phys.Rev. C17, 493 (1978) C.D.Goodman, D.L.Hanson, D.C.Hensley, R.G.Stokstad Isospin Conservation in the Reactions 16O(p, t)14O(g.s.) And 16O(p, 3He)14N(2.31 MeV) NUCLEAR REACTIONS 16O(p, t), (p, 3He), E=27-30, 7 MeV; measured σ(E, θ). DWBA, Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.17.493
1978OB01 Phys.Rev. C18, 764 (1978) F.E.Obenshain, R.L.Ferguson, M.L.Halbert, D.C.Hensley, H.Nakahara, F.Plasil, F.Pleasonton, A.H.Snell, R.G.Stokstad Reactions between 20Ne and Nickel NUCLEAR REACTIONS Ni(20Ne, X), E=164 MeV; measured σ(E(A), Z, θ). Gas ionization detector, surface barrier detector.
doi: 10.1103/PhysRevC.18.764
1978ST15 Phys.Rev.Lett. 41, 465 (1978) R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya Effect of Nuclear Deformation on Heavy-Ion Fusion NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured fusion σ(E).
doi: 10.1103/PhysRevLett.41.465
1978ST29 S.Afr.J.Phys. 1, 171 (1978) R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilanski, I.Tserruya The Effect of Nuclear Deformation on Heavy-Ion Fusion NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured σ(fusion); deduced importance of nuclear deformation.
1977ST25 Phys.Lett. 70B, 289 (1977) R.G.Stokstad, R.A.Dayras, J.Gomez del Campo, P.H.Stelson, C.Olmer, M.S.Zisman Measurements of the Fusion of 12C + 14N and the Liquid-Drop Limit for 26Al NUCLEAR REACTIONS 12C(14N, X), E=248 MeV; measured fusion σ.
doi: 10.1016/0370-2693(77)90660-8
1977ST34 Phys.Rev. C16, 2249 (1977) R.G.Stokstad, M.N.Namboodiri, E.T.Chulick, J.B.Natowitz, D.L.Hanson Mechanisms for Li and Be Production in the 14N + 12C Reaction NUCLEAR REACTIONS 12C(14N, 6Li), (14N, 7Li), (14N, 9Be), E=86.9, 157.0 MeV; measured σ(θ). Statistical model calculations.
doi: 10.1103/PhysRevC.16.2249
1977SW02 Nucl.Phys. A279, 502 (1977) Z.E.Switkowski, R.G.Stokstad, R.M.Wieland 14N Fusion with 12C and 16O at Sub-Barrier Energies NUCLEAR REACTIONS 12C(14N, X), E(cm)=3.6-9.2 MeV; measured γ-yields, σ for 21Ne, 22,24Na, 24,25Mg, 25Al products; deduced total fusion σ. 16O(14N, X), E(cm)=5.6-12.6 MeV; measured γ-yields, σ for 25Mg, 26Al, 28Si products; deduced total fusion σ. Ge(Li) detector. IWB analysis.
doi: 10.1016/0375-9474(77)90583-8
1976DA07 Nucl.Phys. A261, 478 (1976) R.A.Dayras, R.G.Stokstad, Z.E.Switkowski, R.M.Wieland Fusion Cross Sections for 10,11B + 12C at Sub-Coulomb Energies NUCLEAR REACTIONS 10,11B(12C, nγ), 10,11B(12C, pγ), 10,11B(12C, αγ), E=5-16 MeV; measured σ(E;Eγ); deduced σ(E;En, p, α), total reaction σ(E) for 10B+12C, 11B+12C. Enriched targets.
doi: 10.1016/0375-9474(76)90161-5
1976DA13 Nucl.Phys. A265, 153 (1976) R.A.Dayras, R.G.Stokstad, Z.E.Switkowski, R.M.Wieland Gamma-Ray Yields from 12C + 13C Reactions Near and below the Coulomb Barrier NUCLEAR REACTIONS 13C(12C, X), E(cm)=3.1-11.9 MeV; measured σ(E, Eγ) for transitions in 17O, 20,21Ne, 23,24Na, 24Mg; deduced total σ. Optical model, statistical analysis. Ge(Li) detector, enriched targets.
doi: 10.1016/0375-9474(76)90121-4
1976LO03 Nucl.Phys. A259, 122 (1976) M.Lowry, J.S.Schweitzer, R.Dayras, R.G.Stokstad Cross Sections for 6Li Production in the Reactions 10B + 16O and 12C + 14N at Low Energies NUCLEAR REACTIONS 10B(16O, 6Li), E(cm)=7.5-16.15 MeV; 12C(14N, 6Li), E(cm)=13.8-16.6 MeV; measured σ(θ). 20Ne deduced levels. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(76)90499-1
1976ST07 Phys.Rev.Lett. 36, 1529 (1976) R.G.Stokstad, J.Gomez del Campo, J.A.Biggerstaff, A.H.Snell, P.H.Stelson Fusion of 14N + 12C at Energies up to 178 MeV NUCLEAR REACTIONS 12C(14N, X), E=43-178 MeV; measured fusion σ(E).
doi: 10.1103/PhysRevLett.36.1529
1976ST12 Phys.Rev.Lett. 37, 888 (1976) R.G.Stokstad, Z.E.Switkowski, R.A.Dayras, R.M.Wieland Measurements of Fusion Cross Sections for Heavy-Ion Systems at Very Low Energies NUCLEAR REACTIONS 10,11B, 12,13C, 14N, 16O(12C, X), 14N, 16O(14N, X), 16O(16O, X), E=sub-Coulomb barrier; measured fusion σ(E).
doi: 10.1103/PhysRevLett.37.888
1976SW02 Nucl.Phys. A274, 202 (1976) Z.E.Switkowski, R.G.Stokstad, R.M.Wieland Measurement of Fusion Cross Sections for 14N + 14N and 12C + 16O at Low Energies NUCLEAR REACTIONS 12C(16O, X), E=10.5-23.3 MeV; measured σ, γ-yields. 14N(14N, X), E=9.4-22 MeV; measured σ, γ-yields; deduced total fusion σ for E(cm)=4.68-11 MeV. Ge(Li), NaI detectors.
doi: 10.1016/0375-9474(76)90237-2
1976WI14 Phys.Rev.Lett. 37, 1458 (1976) R.M.Wieland, R.G.Stokstad, G.R.Satchler, L.D.Rickertsen Analysis of 12C + 12C Scattering and the Depth of the Real Potential NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=35-63 MeV; calculated σ(θ). Folding model.
doi: 10.1103/PhysRevLett.37.1458
1975SH24 Phys.Rev. C12, 1907 (1975) D.Shapira, R.G.Stokstad, M.W.Sachs, A.Gobbi, D.A.Bromley Experimental Studies of the Resonance at E(c.m.) = 19.7 MeV in the 12C + 16O System NUCLEAR REACTIONS 12C(16O, 16O'), (16O, 12C), (16O, α), (16O, p), E=45.96 MeV; measured σ(E). 16O, 24Mg, 27Al, 28Si deduced resonance structure.
doi: 10.1103/PhysRevC.12.1907
1974HA11 Phys.Rev. C9, 929 (1974) D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, D.A.Bromley Compound Nature of the Reaction 12C(14N, 6Li)20Ne NUCLEAR REACTIONS 12C(14N, 6Li), E(cm)=24, 36, 55 MeV; calculated σ(E(6Li), θ). 12C(14N, 2p), (14N, α), (14N, 7Be), E=12-60 MeV; calculated σ.
doi: 10.1103/PhysRevC.9.929
1974HA25 Phys.Rev. C9, 1760 (1974) D.L.Hanson, R.G.Stokstad, K.A.Erb, C.Olmer, M.W.Sachs, D.A.Bromley Systematics of 'Quasimolecular' Resonances: A Search for Sub-Coulomb Resonant Structure in the Reactions 14N + 14N and 9Be + 12C NUCLEAR REACTIONS 9Be(12C, α), (12C, p), E(cm)=2.4-6.34 MeV; measured σ(E, Eα, Ep); 14N(14N, α), (14N, p), (14N, d), E(cm)=7-10 MeV; measured σ(E, Eα, Ep, Ed); deduced no resonances.
doi: 10.1103/PhysRevC.9.1760
1974OL06 Phys.Rev. C10, 1722 (1974) C.Olmer, R.G.Stokstad, D.L.Hanson, K.A.Erb, M.W.Sachs, D.A.Bromley Light Particle and Gamma-Ray Production in 12C + 14N Interactions NUCLEAR REACTIONS 12C(14N, d), (14N, p), (14N, α), E=20, 25 MeV; measured σ(Ed, θ), σ(Ep, θ), σ(Eα, θ); 14N(12C, γ), E=14-33 MeV; measured σ(E, Eγ). 24,25Mg deduced levels, J, π.
doi: 10.1103/PhysRevC.10.1722
1974SH16 Phys.Rev. C10, 1063 (1974) D.Shapira, R.G.Stokstad, D.A.Bromley Statistical Analysis of the Energy Dependence of 12C + 12C Cross Sections NUCLEAR REACTIONS 12C(12C, 12C), E=13.5-37.5 MeV; calculated σ. 12C(12C, α), E=16-21 MeV; measured σ(E, Eα). 24Mg resonances deduced level-width.
doi: 10.1103/PhysRevC.10.1063
1971ST20 Phys.Rev.Lett. 27, 748 (1971) R.G.Stokstad, J.S.Greenberg, I.A.Fraser, S.H.Sie, D.A.Bromley Rotation-Vibration Interaction in Sm152 NUCLEAR STRUCTURE 152Sm; calculated levels, moments of inertia, E2 matrix elements. VMI model;rotation-vibration interaction.
doi: 10.1103/PhysRevLett.27.748
1970DI11 Nucl.Phys. A155, 209 (1970) F.S.Dietrich, B.Herskind, R.A.Naumann, R.G.Stokstad Hole-Vibration Coupling in 115In NUCLEAR REACTIONS 115In(d, d'), E=12 MeV; measured σ(Ed', θ). 115In(16O, 16O'γ), E=41-55 MeV; measured σ(E;E(16O'), Eγ). 115In deduced levels, J, π, B(E2), branching ratios. Natural targets.
doi: 10.1016/0375-9474(70)90087-4
1970ST18 Nucl.Phys. A156, 145 (1970) R.G.Stokstad, I.A.Fraser, J.S.Greenberg, S.H.Sie, D.A.Bromley Doppler Shift Attenuation Studies in Heavy Nuclei NUCLEAR REACTIONS 152Sm(16O, 16O'γ), E=60 MeV; 150Nd, 152Sm(32S, 32S'γ), E=94-110 MeV; measured σ(E;Eγ), Doppler shift attenuation. 150Nd, 152Sm levels deduced T1/2.
doi: 10.1016/0375-9474(70)91122-X
1970WH05 Nucl.Phys. A157, 529 (1970) S.Whineray, F.S.Dietrich, R.G.Stokstad A Study of Isobaric Analogue Resonances in the Yb Isotopes NUCLEAR REACTIONS 168,170,172,174,176Yb(p, p), E=10.0-13.0 MeV; measured σ(Ep;θ). 169,171,173,175,177Lu deduced isobaric analog resonances, p-width, level-width. Lu-Yb deduced Coulomb displacement energies. 174Yb(d, p), E=12.0 MeV; measured σ(90°). 175Yb deduced levels, J, π, S. Enriched targets.
doi: 10.1016/0375-9474(70)90231-9
1969FR10 Phys.Rev.Letters 23, 1047 (1969); Erratum Phys.Rev.Letters 23, 1270 (1969) I.A.Fraser, J.S.Greenberg, S.H.Sie, R.G.Stokstad, G.A.Burginyon, D.A.Bromley Investigation of Band-Mixing Anomalies in Sm152 NUCLEAR REACTIONS 152Sm(16O, 16O'γ), E = 48-60 MeV; measured σ(E;Eγ, θ). 152Sm transitions deduced B(E2), γ-mixing ratios, band mixing parameters.
doi: 10.1103/PhysRevLett.23.1047
1969FR11 Phys.Rev.Letters 23, 1051 (1969) I.S.Fraser, J.S.Greenberg, S.H.Sie, R.G.Stokstad, D.A.Bromley E2 Matrix Elements Between High-Spin States in the Ground-State Bands of Sm152 and Sm154 NUCLEAR REACTIONS 152,154Sm(16O, 16O'γ), E = 48-60 MeV; 152,154Sm(32S, 32S'γ), E = 87-110 MeV; measured σ(E;E(16O'), Eγ), σ(E;E(32S'), Eγ). 152,154Sm transitions deduced E2 matrix elements, band mixing parameters, isomer shifts.
doi: 10.1103/PhysRevLett.23.1051
1968ST13 Phys.Rev. 170, 1072 (1968) Coulomb Excitation of the Lowest States in Tungsten Nuclei NUCLEAR STRUCTURE 183W, 184W, 186W, 182W; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.1072
1968ST25 Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.699 (1968) R.G.Stokstad, R.A.Moline, C.A.Barnes, F.Boehm, A.Winther Hyperfine Fields of Fluorine in Ni and Gd NUCLEAR REACTIONS 19F(α, α'γ), E = 4.1 MeV; Cu, Ni(19F, 19F'γ), E = 30 MeV; measured γγ(θ, H, t); deduced hyperfine fields in Ni, Gd. 19F level deduced g, T1/2.
1967ST03 Nucl.Phys. A92, 319 (1967) R.G.Stokstad, I.Hall, G.D.Symons, J.de Boer The Determination of the Static Quadrupole Moments of the First 2+ States in 114Cd and 116Cd by Higher Order Effects in Coulomb Excitation NUCLEAR REACTIONS 114,116Cd(α, α'), (12C, 12C'), (16O, 16O'), E = 2-3 MeV/nucleon; measured σ(E). 114,116Cd 2+ level deduced quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(67)90221-7
1967ST16 Nucl.Phys. A99, 507 (1967) The Determination of the Static Quadrupole Moments of the First 2+ States in 126Te and 128Te by Coulomb Excitation NUCLEAR REACTIONS 126,128Te(α, α'), (16O, 16O'), E=2-3 MeV/nucleon; measured σ(E). 126,128Te 2+ level deduced quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(67)90949-9
1965DE07 Phys.Rev.Letters 14, 564 (1965) J.de Boer, R.G.Stokstad, G.D.Symons, A.Winther Reorientation Effect in Cd114 NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.14.564
1964DE14 Bull.Am.Phys.Soc. 9, No.7, 718, K6 (1964) J.de Boer, R.G.Stokstad, G.D.Symons, A.Winther Experimental Evidence for the Reorientation Effect in Cd114 NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.
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