NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Ogaza Found 32 matches. 1993OG01 Nucl.Phys. A559, 100 (1993) S.Ogaza, J.Kownacki, M.P.Carpenter, J.Gascon, G.B.Hagemann, Y.Iwata, H.J.Jensen, T.Komatsubara, J.Nyberg, G.Sletten, P.O.Tjom, W.Walus, I.Hamamoto Shapes, Electromagnetic Properties and Enhanced E1 Strength in 169Lu NUCLEAR REACTIONS 154Sm(19F, 4n), E=85 MeV; measured Eγ, γγ-coin, Iγ, DSA. 169Lu deduced levels, Iγ, rotational band-structure, configuration-dependent shape, pairing, T1/2, transition quadrupole moments, B(M1)/B(E2), B(E1). Comparison to particle-rotor calculations including octupole softness. Enriched target, array of Compton suppressed Ge-detectors.
doi: 10.1016/0375-9474(93)90182-W
1990AT01 Phys.Lett. 252B, 545 (1990) A.Atac, J.J.Gaardhoje, B.Herskind, Y.Iwata, S.Ogaza, A.Bracco, A.M.Bruce, A.James, R.Chapman, F.Khazaie, J.C.Lisle, J.N.Mo, K.A.Connell, J.Simpson GDR Decay in Hot Hg Isotopes. An Approach to Improve the Sensitivity to GDR Decay following Fusion Reactions NUCLEAR REACTIONS 142Nd(48Ca, X), E=205 MeV; measured Eγ, Iγ, γ(recoil)-coin. 190Hg deduced GDR decay, parameters.
doi: 10.1016/0370-2693(90)90480-T
1990GA15 Nucl.Phys. A513, 344 (1990) J.Gascon, C.-H.Yu, G.B.Hagemann, M.C.Carpenter, J.M.Espino, Y.Iwata, T.Komatsubara, J.Nyberg, S.Ogaza, G.Sletten, P.O.Tjom, D.C.Radford, J.Simpson, A.Alderson, M.A.Bentley, P.Fallon, P.D.Forsyth, J.W.Roberts, J.F.Sharpey-Schafer Configuration-Dependent Transition Rates in 157Ho NUCLEAR REACTIONS 124Sn(37Cl, 4n), E=150 MeV; 142Ce(19F, 4n), E=85.5 MeV; measured Iγ, γγ-coin, DSA. 157Ho deduced levels, J, π, T1/2, transition quadrupole moments, nuclear deformation, B(M1). Enriched targets, array of Compton-suppressed Ge-detectors.
doi: 10.1016/0375-9474(90)90102-R
1988NE03 Nucl.Phys. A483, 126 (1988) J.O.Newton, D.J.Hinde, R.J.Charity, J.R.Leigh, J.J.M.Bokhorst, A.Chatterjee, G.S.Foote, S.Ogaza Measurement and Statistical Model Analysis of Pre-Fission Neutron Multiplicities NUCLEAR REACTIONS 150Sm(18O, F), E=108-122 MeV; 159Tb(19F, F), E=110-124 MeV; 169Tm(19F, F), E=105-135 MeV; 164Er(28Si, F), E=170 MeV; 170Er(28Si, F), E=135-165 MeV; 181Ta(19F, F), E=95-135 MeV; 170Er(30Si, F), E=160 MeV; 192Os(18O, F), 197Au(16O, F), E=95-124 MeV; 232Th(19F, F), E=105-138 MeV; measured fission (fragment)n-coin, σ(fragment θ, E(n)); deduced pre-, post-fission neutron multiplicities. 168Yb, 178W, 188Pt, 192,198,200Pb, 210Po, 213Fr, 251Es deduced statistical model parameters, dynamical, temperature effects.
doi: 10.1016/0375-9474(88)90068-1
1987SI07 J.Phys.(London) G13, 847 (1987) J.Simpson, M.A.Riley, J.R.Cresswell, D.V.Elenkov, P.D.Forsyth, G.B.Hagemann, D.Howe, B.M.Nyako, S.Ogaza, J.C.Lisle, J.F.Sharpey-Schafer Near-Yrast Discrete Line γ-Ray Spectroscopy of 159Er and 160Er to I ≥ 40(h-bar) NUCLEAR REACTIONS 148Nd(16O, 4n), E=80 MeV; 116Cd(48Ca, 4n), (48Ca, 5n), E=210 MeV; measured γγ-coin, γγ(θ). 159,160Er deduced levels, J, π, ICC. Enriched targets. Cranked shell model calculations.
doi: 10.1088/0305-4616/13/6/013
1986CH30 Nucl.Phys. A457, 441 (1986) R.J.Charity, J.R.Leigh, J.J.M.Bokhorst, A.Chatterjee, G.S.Foote, D.J.Hinde, J.O.Newton, S.Ogaza, D.Ward Heavy-Ion Induced Fusion-Fission Systematics and the Effect of the Compound-Nucleus Spin Distribution on Fission-Barrier Determination NUCLEAR REACTIONS, ICPND 139La, 159Tb, 169Tm(19F, X), (19F, F), E=70-129 MeV; 150Sm, 192Os(18O, X), (18O, F), E=65-124 MeV; measured fission, evaporation σ(fragment θ), σ(E). Statistical model.
doi: 10.1016/0375-9474(86)90388-X
1986HI01 Nucl.Phys. A452, 550 (1986) D.J.Hinde, R.J.Charity, G.S.Foote, J.R.Leigh, J.O.Newton, S.Ogaza, A.Chatterjee Neutron Multiplicities in Heavy-Ion-Induced Fission: Timescale of fusion-fission NUCLEAR REACTIONS 150Sm(18O, F), E=108-122 MeV; 164Er(28Si, F), E=170 MeV; 170Er(28Si, F), E=135-165 MeV; 170Er(30Si, F), E=160 MeV; 181Ta(19F, F), E=95-135 MeV; 192Os(18O, F), 197Au(16O, F), E=95-124 MeV; 232Th(19F, F), E=105-138 MeV; measured (fragment)n-coin, σ(fragment θ, En); deduced pre-, post-fission neutron multiplicities. 168Yb, 192,198,200Pb, 210Po, 213Fr, 251Es deduced fission dynamics. Statistical model.
doi: 10.1016/0375-9474(86)90214-9
1986HU02 Nucl.Phys. A453, 316 (1986) H.Hubel, A.P.Byrne, S.Ogaza, A.E.Stuchbery, G.D.Dracoulis, M.Guttormsen High-Spin Structure of 190-194Hg and the Cranked Shell Model NUCLEAR REACTIONS 170Er(24Mg, xn), (26Mg, xn), E=120-130 MeV. 184,186W(13C, xn), E=84-87 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 190,191,192,193,194Hg deduced levels, J, π, γ-branching. Enriched targets. Compton-suppressed Ge(high purity) detectors. Cranked shell model calculations.
doi: 10.1016/0375-9474(86)90014-X
1984HI04 Phys.Rev.Lett. 52, 986 (1984) D.J.Hinde, R.J.Charity, G.S.Foote, J.R.Leigh, J.O.Newton, S.Ogaza, A.Chatterjee Neutron Emission from Fission Fragments during Acceleration NUCLEAR REACTIONS 232Th(19F, F), E=124 MeV; measured fission fragment(n)-coin vs neutron velocity, neutron multiplicity vs excitation, fragment(n)(θ); deduced neutron emission mechanism.
doi: 10.1103/PhysRevLett.52.986
1984HU10 Phys.Lett. 145B, 29 (1984) H.Hubel, A.P.Byrne, S.Ogaza, A.E.Stuchbery, M.Guttormsen The Second and Third Backbendings in 194Hg NUCLEAR REACTIONS 186W(13C, 5n), E=85 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 194Hg deduced levels, J, π, yrast sequence, γ-branching, backbending. Cranking shell model.
doi: 10.1016/0370-2693(84)90941-9
1981FO03 Nucl.Phys. A361, 242 (1981) F.Folkmann, J.D.Garrett, G.B.Hagemann, M.N.Harakeh, B.Herskind, D.L.Hillis, S.Ogaza, H.Emling, E.Grosse, D.Schwalm, R.S.Simon, P.O.Tjom High Angular Momentum Decay Properties of the Compound Systems 100Ru* and 160Er* formed in 50Ti-Induced Reactions NUCLEAR REACTIONS 50Ti, 110Pd(50Ti, X), E=163-229 MeV; measured γγ-coin, Eγ, < Eγ >, anisotropy vs summed cascade Eγ. 100Ru, 160Er deduced entry lines, effective moments of inertia, continuum γ-multipolarity vs spin.
doi: 10.1016/0375-9474(81)90478-4
1981LI15 Nucl.Phys. A366, 281 (1981) J.C.Lisle, J.D.Garrett, G.B.Hagemann, B.Herskind, S.Ogaza Strongly Interacting Bands in 170Hf NUCLEAR REACTIONS 158Gd(16O, 4n), E=80 MeV; measured γγ-coin, γ(θ), I(ce). 170Hf deduced levels, J, π, ICC, rotational band moments of inertia, Eγ correlations. Cranked shell-model analysis. Enriched target.
doi: 10.1016/0375-9474(81)90289-X
1977AR19 Hyperfine Interactions 5, 81 (1977) A.Arnesen, K.Johansson, E.Karlsson, T.Noreland, L.-O.Norlin, S.Ogaza Gyromagnetic Ratios of First 2+ States in 126,128,130,132Xe NUCLEAR MOMENTS 126,128,130,132Xe; measured γγ(θ, H) from Coulomb excitation; deduced g of first 2+ state. IMPAC technique.
doi: 10.1007/BF01021680
1975BR19 Nucl.Phys. A248, 356 (1975) R.Broda, M.Ishihara, B.Herskind, H.Oeschler, S.Ogaza, H.Ryde Heavy-Ion Fusion Cross Sections NUCLEAR REACTIONS 148Nd(18O, xnypzα), E(lab)=50-81 MeV; 148,150Nd(16O, xnypzα), E(lab)=50-85 MeV; 152Sm(12C, xnypzα), E(lab)=40-63 MeV; 159Tb(7Li, xnypzα), E(lab)=17-36 MeV; 162Dy(α, xn), E(lab)=12-27 MeV; measured absolute σ; deduced fusion σ; calculated total reaction σ. Enriched targets.
doi: 10.1016/0375-9474(75)90170-0
1975HA17 Nucl.Phys. A245, 166 (1975) G.B.Hagemann, R.Broda, B.Herskind, M.Ishihara, S.Ogaza, H.Ryde Gamma Decay after Heavy Ion Reactions Studied by First and Higher Order Multiplicity Measurements NUCLEAR REACTIONS 148,150Nd(16O, xnγ), E(lab)=65-84 MeV; measured γ-ray multiplicities. Enriched targets.
doi: 10.1016/0375-9474(75)90087-1
1972SK06 Phys.Lett. 40B, 446 (1972) B.Skaali, S.Ogaza, D.G.Fleming, B.Herskind Transient Magnetic Field at Gd in Ferromagnetic Gadolinium NUCLEAR REACTIONS 154,156,158,160Gd(16O, 16O'γ), E=56 MeV; measured (16O')(γ)(θ) in ferromagnetic Gd; deduced transient magnetic field.
doi: 10.1016/0370-2693(72)90547-3
1970HA55 Acta Phys. 28, 185 (1970) On the Magnetic Hyperfine Field at 182W Recoil Implanted into Iron NUCLEAR REACTIONS 182W(16O, 16O'γ), E=36 MeV; measured σ(E(16O'), Eγ), γγ(θ, H) in Fe; deduced internal magnetic field.
doi: 10.1007/BF03055161
1968BO50 Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.158 (1968) E.Bozek, R.Broda, J.Golczewski, A.Z.Hrynkiewicz, R.Kulessa, S.Ogaza, M.Rybicka, W.Walus g-Factors of the Excited States in 124Te and 147Sm RADIOACTIVITY 124Sb, 147Eu; measured γγ(θ, H). 124Te, 147Sm levels deduced g.
1968DE28 Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.731 (1968) B.I.Deutch, G.B.Hagemann, K.A.Hagemann, S.Ogaza Larmor Precession for the 4+ States in Some Erbium Isotopes NUCLEAR REACTIONS 166,168,170Er(16O, 16O'γ), E not given; measured σ(Eγ, E(16O')), γγ(θ, H). 166,168,170Er levels deduced g, Larmor precession.
1968HR01 Fizika 1, 47 (1968) A.Z.Hrynkiewicz, S.Ogaza, J.Styczen, B.Hrastnik, I.Basar Perturbed 208.00-59.54 keV Gamma-Gamma Angular Correlation in 237Np RADIOACTIVITY 237U; measured γγ(θ, t). 237Np levels deduced J, γ-mixing.
1967HR02 Acta Phys.Polon. 32, 77 (1967) A.Z.Hrynkiewicz, S.Ogaza, M.Rybicka, R.Kulessa, W.Walus Lifetimes of Excited Nuclear States in 115In RADIOACTIVITY 115Cd; measured βγ-, γγ-delay. 115In levels deduced J, π, T1/2.
1966HR02 Nucl.Phys. 80, 608 (1966) A.Z.Hrynkiewicz, S.Ogaza, J.Styczen, B.Hrastnik, B.Pudlowska, R.Kulessa The g-Factor of the 87 keV Excited State in 155Gd RADIOACTIVITY 155Tb [from 181Ta(p, X)]; measured γγ(θ, H), γγ(θ, t), γγ(θ, H, t). 155Gd level deduced T1/2, g. Natural target.
doi: 10.1016/0029-5582(66)90068-X
1965KA02 Nucl.Phys. 61, 582(1965) E.Karlsson, E.Matthias, S.Gustafsson, K.Johansson, A.G.Svensson, S.Ogaza, P.da Rocha Andrade The Magnetic Moment of the 3/2+ State in Tl203 and the Question of Core Excitations RADIOACTIVITY 203Pb[from 203Tl(d, 2n)] measured γγ(θ), γγ(θ, H). 203Tl deduced μ 0.279 level. Natural target.
doi: 10.1016/0029-5582(65)90608-5
1964BO16 Phys. Letters 11, 63 (1964) E.Bozek, A.Z.Hrynkiewicz, S.Ogaza, J.Styczen HFS-Interaction of the Gd155 Nucleus in the 87 keV Excited State NUCLEAR STRUCTURE 155Gd, 155Tb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90260-4
1963BO22 Phys.Letters 6, 89 (1963) E.Bozek, A.Z.Hrynkiewicz, S.Ogaza, M.Rybicka, J.Styczen The Half-Life of the 57 keV First Excited State in Pr143 NUCLEAR STRUCTURE 143Ce; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90233-6
1963BO24 PAN-231 (1963); Nucl.Sci.Abstr. 17, 3463, Abstr. 26460 (1963) E.Bozek, H.Niewodniczanski, S.Ogaza, M.Rybicka, J.Styczen Gamma-Gamma Directional Correlations in Eu146 NUCLEAR STRUCTURE 146Gd; measured not abstracted; deduced nuclear properties.
1963BO44 Acta Phys.Pol. 24, 131 (1963) E.Bozek, N.A.Lebedev, H.Niewodniczanski, S.Ogaza, M.Rybicka, J.Styczen Gamma-gamma Directional Correlations in 146Eu
1962BO19 Physica 28, 705 (1962) E.Bozek, A.Z.Hrynkiewicz, Z.Konieczny, S.Ogaza, M.Rybicka, S.Szymczyk The Attenuation of the Angular Correlation of 181Ta 133-482 keV Cascade in Liquids NUCLEAR STRUCTURE 181Hf; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(62)90127-1
1962KA14 Arkiv Fysik 22, 257 (1962) E.Karlsson, E.Matthias, S.Ogaza The Gyromagnetic Ratio of the First Rotational State in Hf178 NUCLEAR STRUCTURE 178Hf; measured not abstracted; deduced nuclear properties.
1961BO15 Acta Phys.Polon. 20, 257 (1961) E.Bozek, H.Niewodniczanski, S.Ogaza, S.Szymczyk, Yu.V.Norseev Energy Levels in 166Er Nucleus NUCLEAR STRUCTURE 166Tm; measured not abstracted; deduced nuclear properties.
1961BO20 Acta.Phys.Polon. 20, 351 (1961) E.Bozek, H.Niewodniczanski, S.Ogaza, S.Szymczyk, T.Walczak, I.A.Yutlandov Gamma-Vibrational Levels in 166Er NUCLEAR STRUCTURE 166Er; measured not abstracted; deduced nuclear properties.
1960BO32 Repts.Third Conf.Neutron-Deficient Isotopes, Dubna (June 1960); NP-13165, Vol.1, p.65 (1964) E.Bozek, K.Nevodnichanskii, S.Ogaza, S.Shimchak, Y.Norseev Energy Levels of Er166 NUCLEAR STRUCTURE 166Yb; measured not abstracted; deduced nuclear properties.
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