NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = J.Osborne Found 21 matches. 2017TA26 Astrophys.J. 848, L27 (2017) N.R.Tanvir, A.J.Levan, C.Gonzalez-Fernandez, O.Korobkin, I.Mandel, S.Rosswog, J.Hjorth, P.D'Avanzo, A.S.Fruchter, C.L.Fryer, T.Kangas, B.Milvang-Jensen, S.Rosetti, D.Steeghs, R.T.Wollaeger, Z.Cano, C.M.Copperwheat, S.Covino, V.D'Elia, A.de Ugarte Postigo, P.A.Evans, W.P.Even, S.Fairhurst, R.Figuera Jaimes, C.J.Fontes, Y.I.Fujii, J.P.U.Fynbo, B.P.Gompertz, J.Greiner, G.Hodosan, M.J.Irwin, P.Jakobsson, U.G.Jorgensen, D.A.Kann, J.D.Lyman, D.Malesani, R.G.McMahon, A.Melandri, P.T.O'Brien, J.P.Osborne, E.Palazzi, D.A.Perley, E.Pian, S.Piranomonte, M.Rabus, E.Rol, A.Rowlinson, S.Schulze, P.Sutton, C.C.Thone, K.Ulaczyk, D.Watson, K.Wiersema, R.A.M.J.Wijers The Emergence of a Lanthanide-rich Kilonova Following the Merger of Two Neutron Stars
doi: 10.3847/2041-8213/aa90b6
2004OS02 Phys.Rev. C 70, 054613 (2004) J.H.Osborne, F.P.Brady, J.L.Romero, J.L.Ullmann, D.S.Sorenson, A.Ling, N.S.P.King, R.C.Haight, J.Rapaport, R.W.Finlay, E.Bauge, J.P.Delaroche, A.J.Koning Measurement of neutron elastic scattering cross sections for 12C, 40Ca, and 208Pb at energies from 65 to 225 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(n, n), E=65-225 MeV; measured σ(θ). Comparison with model predictions, previous results.
doi: 10.1103/PhysRevC.70.054613
2002OS08 Nucl.Phys. A710, 281 (2002) Multiple parton scattering in nuclei: twist-four nuclear matrix elements and off-forward parton distributions NUCLEAR STRUCTURE 32S, 58Ni, 208Pb; calculated twist-four nuclear parton matrix elements, mass dependence.
doi: 10.1016/S0375-9474(02)01085-0
2001JI01 J.Phys.(London) G27, 127 (2001) Generalized Sum Rules for Spin-Dependent Structure Functions of the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated generalized sum rules for spin-dependent structure functions.
doi: 10.1088/0954-3899/27/1/308
2001JI02 Nucl.Phys. A684, 363c (2001) Generalized Drell-Hearn-Gerasimov Sum Rule
doi: 10.1016/S0375-9474(01)00383-9
2000JI01 Phys.Lett. 472B, 1 (2000) Generalized Drell-Hearn-Gerasimov Sum Rule at Order O(p4) in Chiral Perturbation Theory
doi: 10.1016/S0370-2693(99)01365-9
2000JI02 Phys.Rev. D61, 074003 (2000) Nucleon Spin Polarizability at Order O(p4) in Chiral Perturbation Theory
doi: 10.1103/PhysRevD.61.074003
2000JI06 Phys.Rev. D62, 094016 (2000) One-Loop Factorization of the Nucleon g2-Structure Function in the Nonsinglet Case NUCLEAR REACTIONS 1n, 1H(polarized e, e'X), E not given; calculated structure function. Polarized target.
doi: 10.1103/PhysRevD.62.094016
1996HJ01 Phys.Rev. C53, 237 (1996) E.L.Hjort, F.P.Brady, J.R.Drummond, B.McEachern, J.H.Osborne, J.L.Romero, D.S.Sorenson, H.H.K.Tang Measurements of 65 MeV Fe, Sn, and Pb(n, n'x) Continuum Cross Sections NUCLEAR REACTIONS Pb, Fe, Sn(n, n'X), E=65 MeV; measured σ(θn'En'). 120Sn, Fe(p, p'X), E=62 MeV; analyzed σ(θp, Ep'). Cascade-statistical, preequilibrium continuum models.
doi: 10.1103/PhysRevC.53.237
1994HJ01 Phys.Rev. C50, 275 (1994) E.L.Hjort, F.P.Brady, J.L.Romero, J.R.Drummond, D.S.Sorenson, J.H.Osborne, B.McEachern, L.F.Hansen Measurements and Analysis of Neutron Elastic Scattering at 65 MeV NUCLEAR REACTIONS C, Si, Cd, Fe, Sn, Pb(n, n), E=65 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevC.50.275
1994OS07 Nucl.Instrum.Methods Phys.Res. A345, 308 (1994) J.H.Osborne, J.L.Romero, F.P.Brady, E.L.Hjort, W.P.Caskey, J.C.Kintner, D.R.Mayo, D.S.Sorenson, J.L.Ullmann A Compact System with Live Converter for Neutron Spectrum Measurements NUCLEAR REACTIONS 12C(n, n), E=65 MeV; measured σ(θ). Si(n, n), (n, n'), E=65 MeV; measured neutron spectra. Compact detector system with live plastic scintillator converter.
doi: 10.1016/0168-9002(94)91007-3
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
Back to query form Note: The following list of authors and aliases matches the search parameter J.Osborne: , J.H.OSBORNE, J.L.OSBORNE, J.P.OSBORNE |