NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.L.Osborne Found 10 matches. 1988TR01 Nucl.Phys. A483, 406 (1988) S.Trentalange, S.-C.Wu, J.L.Osborne, C.A.Barnes Elastic Scattering and Fusion Cross Sections of 13C + 13C NUCLEAR REACTIONS, ICPND 13C(13C, X), E(cm)=3.26-8 MeV; measured σ, γ-ray yields from 18O, 21,22Ne, 24Na, 24,25Mg; deduced total fusion σ, elastic σ(E), σ(θ). Optical, incoming wave boundary condition models.
doi: 10.1016/0375-9474(88)90543-X
1986HA30 Phys.Lett. 176B, 297 (1986) M.N.Harakeh, D.H.Dowell, G.Feldman, E.F.Garman, R.Loveman, J.L.Osborne, K.A.Snover Role of Isospin in the Statistical Decay of the Giant Dipole Resonance Built on Excited States NUCLEAR REACTIONS 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40.2 MeV; 12C(12C, γ), 12,13C(13C, γ), E=40 MeV; measured σ vs Eγ, γ yields. 28Si, 24,25,26Mg deduced GDR, Γ, EWSR, T-mixing parameters.
doi: 10.1016/0370-2693(86)90167-X
1985AD10 Phys.Rev.Lett. 55, 2129 (1985) E.G.Adelberger, P.B.Fernandez, C.A.Gossett, J.L.Osborne, V.J.Zeps Does the Cabibbo Angle Vanish in Fermi Matrix Elements of High-J States ( Question ) RADIOACTIVITY 24Al(β+) [from 24Mg(p, n), E=18 MeV]; measured Eγ, Iγ, T1/2; deduced ft, vector coupling constant, no evidence for Cabibbo angle vanishing in high spin states. 24Mg levels deduced absolute β+-branching ratios.
doi: 10.1103/PhysRevLett.55.2129
1985GO04 Phys.Rev.Lett. 54, 1486 (1985) C.A.Gossett, K.A.Snover, J.A.Behr, G.Feldman, J.L.Osborne Deformation of Heated Nuclei Observed in the Statistical Decay of the Giant Dipole Resonance NUCLEAR REACTIONS 154,148Sm(12C, X), E=63 MeV; measured Eγ, Iγ, continuum spectra, σ(Eγ). 160,166Er deduced excited state based GDR parameters, splitting, deformation at high temperature.
doi: 10.1103/PhysRevLett.54.1486
1984AD01 Nucl.Phys. A417, 269 (1984) E.G.Adelberger, J.L.Osborne, H.E.Swanson, B.A.Brown The l-Forbidden Gamow-Teller Decay of 39Ca RADIOACTIVITY 35Ar, 39Ca(β+); measured Iγ, Eγ; deduced ft, empirical single-particle operator normalizations. 35Cl levels deduced Iβ, γ-branching ratios, Gamow-Teller transition strengths. 39K levels deduced Iβ, Gamow-Teller transition strengths. Shell model.
doi: 10.1016/0375-9474(84)90508-6
1984OS03 Nucl.Phys. A419, 115 (1984) J.L.Osborne, C.A.Barnes, R.W.Kavanagh, R.M.Kremer, G.J.Mathews, J.L.Zyskind, P.D.Parker, A.J.Howard Low-energy behavior of the 3He(α, γ)7Be cross section NUCLEAR REACTIONS, ICPND 3He(α, γ), E=165-1169 keV; measured σ(E), Eγ, γ-branching ratio. 3He(α, γ), E(cm)=947, 1255 keV; measured σ(E). Enriched target.
doi: 10.1016/0375-9474(84)90288-4
1983NO03 Phys.Rev. C27, 1728 (1983); Erratum Phys.Rev. C28, 1409 (1983) E.B.Norman, T.E.Chupp, K.T.Lesko, J.L.Osborne, P.J.Grant, G.L.Woodruff 7Be Decay Scheme and the Solar Neutrino Problem RADIOACTIVITY 7Be(EC) [from 7Li(p, n), E=1.9, 2.1, 3.5 MeV]; measured Iγ. 7Li level deduced EC-branching ratio.
doi: 10.1103/PhysRevC.27.1728
1982OS02 Phys.Rev.Lett. 48, 1664 (1982) J.L.Osborne, C.A.Barnes, R.W.Kavanagh, R.M.Kremer, G.J.Mathews, J.L.Zyskind, P.D.Parker, A.J.Howard Low-Energy 3He(α, γ)7Be Cross-Section Measurements NUCLEAR REACTIONS, ICPND 3He(α, γ), E(cm)=165-1170 keV; measured absolute σ vs E, γ-branching ratio; deduced zero-energy intercept. Activation technique, 3He gas target.
doi: 10.1103/PhysRevLett.48.1664
1979IK02 Nucl.Phys. A319, 109 (1979) P.G.Ikossi, K.A.Snover, J.L.Osborne, E.G.Adelberger, A.B.McDonald The α-Width of the Lowest T = 2 State in 28Si NUCLEAR REACTIONS 24Mg(α, α), E=5.9-6.25 MeV; measured σ(Eα, θ). 28Si deduced resonances, L, J, π, Γ, Γα, T. Enriched target.
doi: 10.1016/0375-9474(79)90174-X
1978OS04 Nucl.Phys. A305, 144 (1978) J.L.Osborne, E.G.Adelberger, K.A.Snover Total Width of the Lowest T = 2 State in 24Mg NUCLEAR REACTIONS 23Na(p, γ), E=3906 keV; 27Al(p, γ), E=3671 keV; measured σγ(Ep, θ=90°). 24Mg T=2 resonance, 28Si resonance deduced Γ(cm). Natural targets.
doi: 10.1016/0375-9474(78)90168-9
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