NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.Winkler Found 29 matches. 2011DE03 Phys.Rev. C 83, 015801 (2011) F.Dellinger, W.Kutschera, O.Forstner, R.Golser, A.Priller, P.Steier, A.Wallner, G.Winkler Upper limits for the existence of long-lived isotopes of roentgenium in natural gold ATOMIC MASSES 261,265,289,290,291,292,293,294,295,296Rg; measured abundance in natural gold using accelerator mass spectrometry (AMS). No events observed for 261Rg and 265Rg, not confirming a positive identification in another recent study. No events observed for 289,290,292,293,295,296Rg. Two and nine events recorded apparently for 291Rg and 294Rg, respectively could be explained otherwise, thus making positive identification for Rg unlikely. Upper limits established in the range of 1016.
doi: 10.1103/PhysRevC.83.015801
2011DE21 Phys.Rev. C 83, 065806 (2011) F.Dellinger, O.Forstner, R.Golser, A.Priller, P.Steier, A.Wallner, G.Winkler, W.Kutschera Ultrasensitive search for long-lived superheavy nuclides in the mass range A=288 to A=300 in natural Pt, Pb, and Bi ATOMIC MASSES 288,289,290,291,292,293,294,295Ds, 292,293,294,295,296,297,298,299Fl, 293,294,295,296,297,298,299,300Mc; measured abundance in natural platinum, lead, and bismuth samples using accelerator mass spectrometry (AMS) technique. Comparison with previous data. Ultrasensitive search for SHE in natural Pt, Pb and Bi samples proved negative with upper limits established.
doi: 10.1103/PhysRevC.83.065806
2004SC03 Appl.Radiat.Isot. 60, 263 (2004) R.Schon, G.Winkler, W.Kutschera A critical review of experimental data for the half-lives of the uranium isotopes 238U and 235U RADIOACTIVITY 235,238U(α), (SF); compiled, analyzed T1/2 data.
doi: 10.1016/j.apradiso.2003.11.027
1999OB04 Int.J. Mass Spectrom. 184, 145 (1999) F.Oberli, P.Gartenmann, M.Meier, W.Kutschera, M.Suter, G.Winkler The half-life of 126Sn refined by thermal ionization mass spectrometry measurements RADIOACTIVITY 126Sn(β-); measured decay products; deduced T1/2 and its uncertainty. Mass spectrometry, comparison with available data.
doi: 10.1016/S1387-3806(98)14281-1
1997PR09 Phys.Rev. C56, 1424 (1997) A.Priller, P.Steier, A.Pavlik, B.Strohmaier, H.Vonach, A.Wallner, G.Winkler, M.B.Chadwick Double-Differential Neutron Emission Cross Sections of 14-MeV Neutron Induced Reactions on Na and Pb NUCLEAR REACTIONS 23Na, Pb(n, n), (n, n'X), E=14 MeV; measured neutron tof spectra, σ(E, θ). Statistical model calculations.
doi: 10.1103/PhysRevC.56.1424
1996HA45 Nucl.Instrum.Methods Phys.Res. B114, 131 (1996); Erratum Nucl.Instrum.Methods Phys.Res. B117, 474 (1996) P.Haas, P.Gartenmann, R.Golser, W.Kutschera, M.Suter, H.-A.Synal, M.J.M.Wagner, E.Wild, G.Winkler A New Half-Life Measurement of the Long-Lived Fission Product 126Sn RADIOACTIVITY 126Sn(β-); measured Specific activity; deduced T1/2. Source material extracted from spent fuel rods.
doi: 10.1016/0168-583X(95)01571-X
1989LI23 Ann.Nucl.Energy 16, 563 (1989) H.Liskien, M.Uhl, M.Wagner, G.Winkler The Excitation Function for the Reaction 52Cr(n, 2n)51Cr NUCLEAR REACTIONS 52Cr(n, 2n), E ≈ threshold-20 MeV; measured σ(E). Activation technique.
doi: 10.1016/0306-4549(89)90010-8
1989WA30 Ann.Nucl.Energy 16, 623 (1989) M.Wagner, G.Winkler, H.Vonach, Cs.M.Buczko, J.Csikai Measurement of the Cross Sections for the Reactions 52Cr(n, 2n)51Cr, 66Zn(n, 2n)65Zn, 89Y(n, 2n)88Y and 96Zr(n, 2n)95Zr from 13.5 to 14.8 MeV NUCLEAR REACTIONS 52Cr, 66Zn, 89Y, 96Zr(n, 2n), E=13.47-14.79 MeV; measured σ(E). Activation technique.
doi: 10.1016/0306-4549(89)90139-4
1988WA15 Ann.Nucl.Energy 15, 363 (1988) M.Wagner, G.Winkler, H.Vonach, G.Peto Measurement of the Cross Section for the Reaction 93Nb(n, n')93mNb at 2.8 MeV NUCLEAR REACTIONS 93Nb(n, n'), E=2.83 MeV; measured isomer production σ. Activation technique, 238U(n, F) standard.
doi: 10.1016/0306-4549(88)90084-9
1986HA32 Radiat.Eff. 92, 155 (1986) S.J.Hasan, A.Pavlik, G.Winkler, M.Kaba Precise Measurement of Cross Sections for the Reactions 59-Co(n, 2n)58-Co and 59-Co(n, p)59-Fe around 14 MeV NUCLEAR REACTIONS 59Co(n, 2n), (n, p), E=13.5, 13.9, 14.5, 14.8 MeV; measured σ(E). 58,58mCo deduced production σ ratio. Activation technique.
doi: 10.1080/00337578608208310
1986HA38 J.Phys.(London) G12, 397 (1986) S.J.Hasan, A.Pavlik, G.Winkler, M.Uhl, M.Kaba Precise Measurement of Cross Sections for the Reactions 59Co(n, 2n)58mgCo and 59Co(n, p)59Fe around 14 MeV NUCLEAR REACTIONS 59Co(n, 2n)58Co/58mCo, 59Co(n, p), E=13.5, 13.9, 14.5, 14.8 MeV; measured σ, isomeric σ ratios. Activation technique, natural target, 4πγ-NaI, Ge(Li) detectors. Nuclear model calculations.
doi: 10.1088/0305-4616/12/5/007
1985PA13 Nucl.Sci.Eng. 90, 186 (1985) A.Pavlik, G.Winkler, M.Uhl, A.Paulsen, H.Liskien Neutron-Induced Reactions on 58Ni NUCLEAR REACTIONS 58Ni(n, 2n), (n, pn), E=12.7-19.6 MeV; measured σ(E). 58Ni(n, xnypzd), E=13.47-14.83 MeV; measured σ for x=0, y=1, z=1. Activation techniques. Optical, compound nucleus, excition models.
doi: 10.13182/NSE85-A17676
1984PR06 Nucl.Phys. A425, 317 (1984) H.Prade, W.Enghardt, W.D.Fromm, H.U.Jager, L.Kaubler, H.-J.Keller, L.K.Kostov, F.Stary, G.Winkler, L.Westerberg New Positive-Parity States and the Shell-Model Description of 111Sn NUCLEAR REACTIONS, ICPND 108Cd(α, n), E=20-27 MeV; measured Eγ, Iγ, γγ-coin, σ(E, Eγ, θγ), αγ(t), I(ce), γ yield vs E. 111Cd(3He, 3n), E=28-32 MeV; measured Eγ, Iγ, γγ-coin, σ(E, Eγ, γγ), 3Heγ(t), γ yield vs E. 109Ag(6Li, 4n), E=40.5 MeV; measured Eγ, Iγ. 111Sn deduced levels, J, π, T1/2, ICC, δ(E2/M1). Enriched targets, Ge(Li), Si-Li detectors. Shell model analysis.
doi: 10.1016/0375-9474(84)90078-2
1983CH47 Nucl.Instrum.Methods 215, 397 (1983) P.Christmas, S.M.Judge, T.B.Ryves, D.Smith, G.Winkler The Decay Scheme of 64Cu RADIOACTIVITY 64Cu(β-), (β+), (EC) [from metallic Cu thermal neutron irradiation]; measured β-spectra, βγ-coin; deduced electron to positron ratio, total β-branching ratio. 64Zn level deduced Iβ-. 64Ni levels deduced EC, β+ branching ratio. 4π β-γ method, liquid scintillation technique, gas proportional counter.
doi: 10.1016/0167-5087(83)90470-2
1983VO13 Phys.Rev. C28, 2278 (1983) H.Vonach, R.C.Haight, G.Winkler (α, n) and Total α-Reaction Cross Sections for 48Ti and 51V NUCLEAR REACTIONS, ICPND 48Ti(α, n), E=6-13 MeV; 51V(α, n), E=6.5-12 MeV; measured residuals yield vs E; deduced σ(reaction). Optical model calculations.
doi: 10.1103/PhysRevC.28.2278
1983WI16 Ann.Nucl.Energy 10, 601 (1983) Precise Measurement of Cross Sections for the Reaction 65Cu(n, 2n)64Cu in the 14 MeV Region and Simultaneous Reevaluation of Some Important Cross Sections at 14.7 MeV NUCLEAR REACTIONS 65Cu(n, 2n), 27Al(n, α), E=13.692, 14, 473, 14.822 MeV; measured σ. 56Fe, 32S(n, p), 63Cu, 197Au, 93Nb(n, 2n), 1H(n, n), E=14.7 MeV; analyzed data; deduced σ.
doi: 10.1016/0306-4549(83)90063-4
1982PA15 J.Phys.(London) G8, 1283 (1982) A.Pavlik, G.Winkler, H.Vonach, A.Paulsen, H.Liskien Precise Measurement of Cross Sections for the 90Zr(n, 2n)89Zr Reaction from Threshold to 20 MeV NUCLEAR REACTIONS 90Zr(n, 2n), E=12.3-19.5 MeV; measured σ. Activation technique, natural target, 4π-γ, NaI detectors.
doi: 10.1088/0305-4616/8/9/012
1981WI06 Nucl.Sci.Eng. 78, 415 (1981) G.Winkler, V.Spiegel, C.M.Eisenhauer, D.L.Smith Measurement of the Average Activation Cross Section for the Reaction 63Cu(n, α)60Co in the Spontaneous Fission Neutron Field of Californium-252 NUCLEAR REACTIONS 63Cu(n, α), E=fission spectrum; measured average σ(E). Near-point 252Cf source, light mass source detector.
doi: 10.13182/NSE81-A21377
1980SM06 Nucl.Sci.Eng. 76, 357 (1980) A.Smith, P.Guenther, G.Winkler, R.McKnight Note on the Prompt-Fission-Neutron Spectra of Uranium-233 and -235 and Plutonium-239 and -240 Relative to that of Californium-252 NUCLEAR REACTIONS, Fission 235,233U(n, F), E=525 keV; 239,240Pu(n, F), E=850 keV; measured prompt σ(En) relative to 252Cf(SF). Tof.
doi: 10.13182/NSE80-A21327
1980WI14 Nucl.Sci.Eng. 76, 30 (1980) G.Winkler, D.L.Smith, J.W.Meadows Measurement of Cross Sections for the 63Cu(n, α)60Co Reaction from Threshold to 10 MeV NUCLEAR REACTIONS 63Cu(n, α), E=3.5-10 MeV; measured σ(E); deduced consistency between integral, differential data. Activation method.
doi: 10.13182/NSE80-A19290
1979SM09 Nucl.Phys. A332, 297 (1979) A.Smith, P.Guenther, G.Winkler, J.Whalen Fast-Neutron Total and Scattering Cross Sections of 107Ag in the MeV Region NUCLEAR REACTIONS 107Ag(n, X), (n, n), (n, n'), E=0.25-4.5 MeV; measured transmission σ(θ). Optical, statistical model analysis.
doi: 10.1016/0375-9474(79)90004-6
1978WI10 Nucl.Sci.Eng. 67, 260 (1978) Precise Measurement of the 63Cu(n, α)60Co Cross Section with 14-MeV Neutrons NUCLEAR REACTIONS 63Cu(n, α), E=14.80 MeV; measured σ. Activation technique, 27Al(n, α) used as standard.
doi: 10.13182/NSE78-A15443
1976SC16 Nucl.Phys. A264, 105 (1976) O.Schwerer, M.Winkler-Rohatsch, H.Warhanek, G.Winkler Measurement of Cross Sections for 14 MeV Neutron Capture NUCLEAR REACTIONS 37Cl, 41K, 50Ti, 51V, 55Mn, 71Ga, 87Rb, 89Y, 127I, 130Te, 138Ba, 139La, 142Ce, 186W, 198Pt, 197Au(n, γ), E=14.6 MeV; measured σ. Natural targets.
doi: 10.1016/0375-9474(76)90147-0
1974ST07 Nucl.Phys. A222, 605 (1974) Measurement of (n, p) Cross Sections on Isotopes of Cd, Sn and Te for 14 MeV Neutrons NUCLEAR REACTIONS 112,114Cd, 117,118,120,122Sn, 122,124,126,128,130Te(n, p), E=14.6 MeV; measured σ. Natural targets.
doi: 10.1016/0375-9474(74)90342-X
1972ED01 Z.Phys. 253, 335 (1972) On (n, p) Cross Sections for 14 MeV Neutrons
doi: 10.1007/BF01386167
1969WI26 Osterr.Akad.Wiss., Math.-Naturw.-Kl., Sitzber., Abt.II 177, 313 (1969) Messung von (n, 2n)-Wirkungsquerschnitten an Schweren Kernen NUCLEAR REACTIONS 140,142Ce, 160Dy, 166Er, 169Tm, 170Yb, 176Hf, 182W, 204Hg, 203Tl, 204Pb(n, 2n), E=14.7 MeV; measured σ.
1969WI28 Osterr.Akad.Wiss.Math.-Naturwiss.Kl., Anz. 105, 321 (1969) Messung von (n, 2n)-Wirkungsquerschnitten an schweren Kernen NUCLEAR REACTIONS 140,142Ce, 160Dy, 166Er, 169Tm, 170Yb, 176Hf, 182W, 204Hg, 203Tl, 204Pb(n, 2n), E=14.7 MeV; measured σ.
1968DI10 Nucl.Phys. A118, 9 (1968) W.Dilg, H.Vonach, G.Winkler, P.Hille Measurement of (n, 2n) reactions cross-sections on heavy nuclei NUCLEAR REACTIONS 140Ce(n, 2n), 142Ce(n, 2n), 142Nd(n, 2n), 154Gd(n, 2n), 160Dy(n, 2n), 165Ho(n, 2n), 166Er(n, 2n), 169Tm(n, 2n), 170Yb(n, 2n), 175Lu(n, 2n), 176Hf(n, 2n), 182W(n, 2n), 191Ir(n, 2n), 197Au(n, 2n), 198Hg(n, 2n), 204Hg(n, 2n), 203Tl(n, 2n), 204Pb(n, 2n), E=14.7 MeV; measured products, 139Ce, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry 20802.
doi: 10.1016/0375-9474(68)90182-6
1962PE14 Phys.Rev. 127, 524 (1962) S.Penselin, T.Moran, V.W.Cohen, G.Winkler Hyperfine Structure of the Electronic Ground States of Rb85 and Rb87 NUCLEAR STRUCTURE 85Rb, 87Rb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.127.524
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