NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Woodward Found 16 matches. 1998BA24 Phys.Lett. 420, 211 (1998) J.T.Balewski, A.Budzanowski, H.Dombrowski, W.Eyrich, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, J.Hauffe, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, A.Metzger, P.Moskal, W.Oelert, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, F.Stinzing, A.Strzalkowski, C.Thomas, S.Wirth, M.Wolke, R.Woodward, P.Wustner, D.Wyrwa Total Cross Section of the Reaction pp → pK+ Λ Close to Threshold NUCLEAR REACTIONS 1H(p, pX), E at 2.3 GeV/c; measured total σ vs excess energy for pK+Λ final state; deduced reaction mechanism features.
doi: 10.1016/S0370-2693(97)01527-X
1983GA16 Phys.Scr. T5, 178 (1983) J.J.Gaardhoje, J.D.Garrett, G.B.Hagemann, B.Herskind, A.Holm, P.Nolan, G.Sletten, J.R.Beene, M.L.Halbert, D.C.Hensley, I.Y.Lee, F.Plasil, F.A.Dilmanian, M.Jaaskelainen, H.Puchta, D.G.Sarantites, R.Woodward, Th.Lindblad High Spin Phenomena in the Mass 100-200 Region Seen through the Crystal Ball NUCLEAR REACTIONS 112,114Cd, 96Zr, 135Ba, 124Sn(50Ti, X), E=230 MeV; measured entry region γ-spectra average properties; deduced γ-ray fold distribution mass dependence. 166,164,162,160,156Yb deduced γ-ray fold distribution neutron dependence. Spin spectrometer.
doi: 10.1088/0031-8949/1983/T5/034
1983HA28 Phys.Scr. T5, 91 (1983) M.L.Halbert, J.H.Barker, J.R.Beene, R.L.Ferguson, D.C.Hensley, G.R.Young, F.A.Dilmanian, M.Jaaskelainen, H.Puchta, D.G.Sarantites, R.Woodward Heavy-Ion Reaction Mechanisms Studied with the Spin Spectrometer NUCLEAR REACTIONS 146Nd(20Ne, 5n), (20Ne, 6n), (20Ne, 7n), (20Ne, 8n), E=136 MeV; measured γ-multiplicity, σ vs multiplicity, excitation. 159Tb(19F, X), E=180 MeV; measured γ-multiplicity vs fragment mass, Z, σ(fragment θ) for X=C, B, Be, N, O, Ne. Comparison with sum rule predictions.
doi: 10.1088/0031-8949/1983/T5/014
1983JA04 Nucl.Phys. A396, 319c (1983) M.Jaaskelainen, D.G.Sarantites, F.A.Dilmanian, R.Woodward, H.Puchta, J.R.Beene, J.Hattula, M.L.Halbert, D.C.Hensley, J.H.Barker Evolution of Nuclear Shapes in 157-161Yb as a Function of Spin and Neutron Number NUCLEAR REACTIONS 146Nd(20Ne, 6n), (20Ne, 7n), E=136, 149 MeV; 146Nd(20Ne, 8n), 144Nd(20Ne, 6n), (20Ne, 7n), E=149 MeV; 146Nd(20Ne, 5n), E=136 MeV; measured continuum Eγ, Iγ, γ(θ) vs multiplicity. 157,158,159,160,161Yb deduced nuclear shapes.
doi: 10.1016/0375-9474(83)90028-3
1983JA12 Phys.Scr. T5, 175 (1983) M.Jaaskelainen, D.G.Sarantites, F.A.Dilmanian, R.Woodward, H.Puchta, J.R.Beene, J.Hattula, M.L.Halbert, D.C.Hensley Transition from Prolate to Oblate to Triaxial Shapes in 158Yb NUCLEAR REACTIONS 144Nd(20Ne, 6n), 146Nd(20Ne, 8n), E=149 MeV; measured γ-multiplicity, γ(θ) vs multiplicity. 158Yb deduced average excitation energy, continuum decay characteristics, prolate to oblate shape change.
1983SA10 Nucl.Phys. A400, 435c (1983) R.C.Sarantites, M.Jaaskelainen, F.A.Dilmanian, H.Puchta, R.Woodward, J.R.Beene, D.C.Hensley, M.L.Halbert, J.Hattula, J.H.Barker, R.Novotny, L.Adler, R.K.Choudhury, M.N.Namboodiri, R.P.Schmitt, J.B.Natowitz Research Highlights with the Spin Spectrometer NUCLEAR REACTIONS 146Nd(20Ne, 8n), E=136 MeV; 146Nd(20Ne, 6n), (20Ne, 7n), E=136, 149 MeV; 144Nd(20Ne, 6n), (20Ne, 7n), 146Nd(20Ne, 8n), E=149 MeV; measured continuum γ-spectra, γ-multiplicities; deduced fusion reaction, entry state energy, angular momentum dependences. 160,158,159Yb deduced effective moment of inertia vs spin, entry line energy vs γ-multiplicity, localized stretched dipole transition. 157,161Yb deduced localized stretched dipole transition.
doi: 10.1016/0375-9474(83)90448-7
1982DI16 Phys.Rev.Lett. 49, 1909 (1982) F.A.Dilmanian, D.G.Sarantites, M.Jaaskelainen, H.Puchta, R.Woodward, J.R.Beene, D.C.Hensley, M.L.Halbert, R.Novotny, L.Adler, R.K.Choudhury, M.N.Namboodiri, R.P.Schmitt, J.B.Natowitz Alpha-Particle Angular Distributions with Respect to Spin Direction NUCLEAR REACTIONS 150Nd(20Ne, xα), E=176 MeV; measured σ(θ, Eα) vs γ-multiplicity, evaporation residue spin direction; deduced α-emitting nucleus deformation characteristics.
doi: 10.1103/PhysRevLett.49.1909
1982JA08 Phys.Rev.Lett. 49, 1387 (1982) M.Jaaskelainen, D.G.Sarantites, R.Woodward, F.A.Dilmanian, H.Puchta, J.R.Beene, J.Hattula, M.L.Halbert, D.C.Hensley, J.H.Barker Evidence for a Prolate to Oblate Shape Change at High Spin in 160Yb NUCLEAR REACTIONS 146Nd(20Ne, 6n), E=136, 149 MeV; measured γ-multiplicity. 160Yb deduced entry state population, decay properties, shape change. Spin spectrometer.
doi: 10.1103/PhysRevLett.49.1387
1982JA10 Phys.Lett. 119B, 65 (1982) M.Jaaskelainen, D.G.Sarantites, F.A.Dilmanian, R.Woodward, H.Puchta, J.R.Beene, J.Hattula, M.L.Halbert, D.C.Hensley Evolution of the Decay Modes of 158Yb with Spin NUCLEAR REACTIONS 144Nd(20Ne, 6n), 146Nd(20Ne, 8n), E=149 MeV; measured continuum Eγ, Iγ, γ-anisotropies. 158Yb deduced entry state decay, collectivity spin dependence, stretched dipole component.
doi: 10.1016/0370-2693(82)90244-1
1982SA21 Phys.Lett. 115B, 441 (1982) D.G.Sarantites, M.Jaaskelainen, R.Woodward, F.A.Dilmanian, D.C.Hensley, J.H.Barker, J.R.Beene, M.L.Halbert, W.T.Milner Population of the Entry States in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 146Nd(20Ne, 5n), (20Ne, 6n), (20Ne, 7n), E=136 MeV; measured σ vs γ-multiplicity, entry state distributions; deduced entrance channel fusion (L). Statistical model.
doi: 10.1016/0370-2693(82)90388-4
1981YA10 Phys.Rev. C24, 2565 (1981) H.Yamada, C.F.Maguire, J.H.Hamilton, A.V.Ramayya, D.C.Hensley, M.L.Halbert, R.L.Robinson, F.E.Bertrand, R.Woodward Localized l Window from Partial Fusion Reactions Accompanied by Proton, Deuteron, and Triton Emission NUCLEAR REACTIONS 154Sm(14N, xnp), (14N, xnd), (14N, xnt), E=167 MeV; measured γ(particle)-coin, γ-multiplicity, σ(evaporation residue); deduced entrance channel localized fusion L window. 158Er deduced yrast transition γ-multiplicity. Massive transfer model.
doi: 10.1103/PhysRevC.24.2565
1980BA20 Phys.Rev.Lett. 45, 424 (1980) J.H.Barker, J.R.Beene, M.L.Halbert, D.C.Hensley, M.Jaaskelainen, D.G.Sarantites, R.Woodward Direct Evidence for a Narrow Window at High Angular Momentum in Incomplete-Fusion Reactions NUCLEAR REACTIONS 146Nd(16O, xnα), E=142 MeV; measured αγ-coin, side feeding; deduced narrow window at high angular momentum, no central collisions. Generalized incomplete fusion model.
doi: 10.1103/PhysRevLett.45.424
1958CL49 J.S.African Chem.Inst. 11, 82 (1958) F.L.Clark, H.J.Spencer-Palmer, R.N.Woodward The Determination of the Half-Lives and Alpha-Particle Energies of Some Radioactive Isotopes. Part III. The Alpha-Particle Energy of U233
1957CL16 J.S.African Chem.Inst. 10, 62 (1957) F.L.Clark, H.J.Spencer-Palmer, R.N.Woodward The Determination of the Half-Lives and α-Particle Energies of Some Radioactive Isotopes. Part I. The Determination of the Half-Lives of Uranium 235 and Uranium 238
1957CL17 J.S.African Chem.Inst. 10, 74 (1957) F.L.Clark, H.J.Spencer-Palmer, R.N.Woodward The Determination of the Half-Lives and α-Particle Energies of Some Radioactive Isotopes. Part II. The Determination of Some α-Particle Energies
1952FU19 Phys.Rev. 88, 170A (1952) S.C.Fultz, R.J.Nash, R.L.Woodward, M.L.Pool Radiations of Rh99 and Ga67
doi: 10.1103/PhysRev.88.170A
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