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NSR database version of May 21, 2024.

Search: Author = R.Stokstad

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0150.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2414.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2416.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1991DI01      Phys.Rev. C43, 265 (1991)

D.E.DiGregorio, R.G.Stokstad

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0082.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1606.

1989FI07      Nucl.Phys. A495, 209c (1989)

D.J.Fields, T.C.Sangster, M.L.Webb, B.A.Remington, H.C.Britt, L.F.Hansen, R.G.Lanier, D.Massoletti, M.N.Namboodiri, G.L.Struble, M.L.Begemann-Blaich, T.Blaich, M.M.Fowler, J.Wilhelmy, S.Kaufman, F.Videbaek, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.Stokstad, Z.Fraenkel

Heavy Ion Reaction Studies of Nb + Au at E/A = 50, 75 and 100 MeV

NUCLEAR REACTIONS 197Au(93Nb, F), E=50-100 MeV/nucleon; measured fission (fragment)(fragment)-coin, (fragment)(fragment)(θ); deduced fission mechanism.

doi: 10.1016/0375-9474(89)90320-5
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0462.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1720.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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1983MU08      Phys.Rev. C28, 428 (1983)

M.J.Murphy, R.G.Stokstad

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
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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
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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
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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
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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
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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
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1981ST01      Phys.Rev. C23, 281 (1981)

R.G.Stokstad, E.E.Gross

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1608.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0170.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1974WI05      Phys.Rev. C9, 1474 (1974)

R.Wieland, R.Stokstad, A.Gobbi, D.Shapira, L.Chua, M.W.Sachs, D.A.Bromley

Three-Body Final States in 16O + 12C-Induced Reactions: The Structure Of 24Mg at High Excitation

NUCLEAR REACTIONS 12C(16O, 2α), (16O, α12C), E=58.3 MeV; measured αα-coin, α12C-coin, deduced reaction mechanism. 20Ne deduced levels; 16O, 24Mg deduced resonances.

doi: 10.1103/PhysRevC.9.1474
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1973CH13      Nucl.Phys. A207, 433 (1973)

P.R.Christensen, I.Chernov, E.E.Gross, R.Stokstad, F.Videbaek

The Interference of Coulomb and Nuclear Excitation in the Scattering of 16O from 58Ni, 88Sr and 142Nd

NUCLEAR REACTIONS 58Ni(16O, 16O), E=35-60 MeV; 88Sr(16O, 16O), E=45-60 MeV; 142Nd(16O, 16O), E=54-72 MeV; measured dσ(θ, E) for g.S., first 2+ state. 58Ni, 88Sr, 142Nd deduced optical model potentials, (βr), B(E2). Enriched targets.

doi: 10.1016/0375-9474(73)90854-3
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1973WI09      Phys.Rev. C8, 37 (1973)

R.Wieland, A.Gobbi, L.Chua, M.W.Sachs, D.Shapira, R.Stokstad, D.A.Bromley

Inelastic Scattering of 12C on 12C

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=40-60 MeV; measured σ(E(12C), θ). Deduced single, mutual excitation of first excited state.

doi: 10.1103/PhysRevC.8.37
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1972RE04      Nucl.Phys. A179, 51 (1972)

I.Rezanka, F.M.Bernthal, J.O.Rasmussen, R.Stokstad, I.Fraser, J.Greenberg, D.A.Bromley

High-Spin States in 153Gd and 154Gd from (α, xnγ) Studies

NUCLEAR REACTIONS 152Sm(α, 3nγ), (α, 2nγ), E=27-32 MeV; measured Eγ, Iγ(θ), γγcoin. 153Gd, 154Gd deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(72)90104-2
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1972ST09      Phys.Rev.Lett. 28, 1523 (1972)

R.Stokstad, D.Shapira, L.Chua, P.Parker, M.W.Sachs, R.Wieland, D.A.Bromley

Possible Nuclear Molecule at 36.5 MeV in Si28

NUCLEAR REACTIONS 12C(16O, X), E approx 19.7 MeV cms; analyzed σ(E). 28Si resonance deduced molecular-type structure.

doi: 10.1103/PhysRevLett.28.1523
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1971GO03      Phys.Rev.Lett. 26, 396 (1971)

A.Gobbi, P.R.Maurenzig, L.Chua, R.Hadsell, P.D.Parker, M.W.Sachs, D.Shapira, R.Stokstad, R.Wieland, D.A.Bromley

Spins and Parities of Highly Excited States in Mg24

NUCLEAR REACTIONS 12C(16O, α1); E=48, 48.8, 58.3 MeV; measured σ(Eα1, Eα2, θ((α1)(α2))). 24Mg levels deduced J, π, branching ratios.

doi: 10.1103/PhysRevLett.26.396
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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
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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
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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
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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
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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
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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
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1968ST13      Phys.Rev. 170, 1072 (1968)

R.G.Stokstad, B.Persson

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
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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
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1967ST16      Nucl.Phys. A99, 507 (1967)

R.G.Stokstad, I.Hall

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
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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
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