NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.Siegert Found 29 matches. 2000FL04 Nucl.Phys. A663-664, 979c (2000) G.T.Fleming, P.Chen, N.Christ, A.Kaehler, T.Klassen, C.Malureanu, R.Mawhinney, G.Siegert, C.Sui, P.Vranas, L.Wu, Y.Zhestkov Dynamical Lattice QCD Thermodynamics with Domain Wall Fermions
doi: 10.1016/S0375-9474(99)00826-X
1998GU03 Nucl.Phys. A629, 93c (1998) S.Gusken, N.Eicker, U.Glassner, H.Hoeber, P.Lacock, G.Ritzenhofer, K.Schilling, G.Siegert, A.Spitz, P.Ueberholz, J.Viehoff Quark Masses with Full QCD Simulations
doi: 10.1016/S0375-9474(97)00671-4
1990WA16 Yad.Fiz. 51, 1521 (1990); Sov.J.Nucl.Phys. 51, 959 (1990) G.Wagner, P.Grabmayr, M.V.Evlanov, T.Kim, K.Knopfle, G.Mairle, V.M.Pugach, G.Siegert Energy and Angle Correlations of Products of the Reactions of 28Si(6Li, αc)X at Energy 156 MeV NUCLEAR REACTIONS 28Si(6Li, αX), E=156 MeV; measured σ(θα, Eα, fragment θ) for X=α, p, d, t, 3He; deduced reaction mechanism. Quasifree scattering model.
1988QU05 Nucl.Phys. A487, 1 (1988) U.Quade, K.Rudolph, S.Skorka, P.Armbruster, H.-G.Clerc, W.Lang, M.Mutterer, C.Schmitt, J.P.Theobald, F.Gonnenwein, J.Pannicke, H.Schrader, G.Siegert, D.Engelhardt Nuclide Yields of Light Fission Products from Thermal-Neutron Induced Fission of 233U at Differenct Kinetic Energies NUCLEAR REACTIONS, Fission 233U(n, F), E=thermal; measured fission fragment mass, nuclear charge distributions vs kinetic energy; deduced independent, fractional independent yields, odd-even effects, average kinetic energies of the elements, reaction Q.
doi: 10.1016/0375-9474(88)90127-3
1984WA19 Yad.Fiz. 40, 1396 (1984) G.Wagner, A.Vdovin, P.Grabmayr, T.Kim, G.Mairle, V.Pugach, G.Siegert, Ch.Stoyanov Fragmentation of Deep Hole States in the Reaction 58Ni(d, 3He)57Co at Deuteron Energy 52 MeV NUCLEAR REACTIONS 58Ni(d, 3He), E=52 MeV; measured σ(θ); deduced optical model parameters. 57Co levels deduced S, d3/2, d5/2 single particle strength functions, deep hole state fragmentation.
1982DE08 Nucl.Instrum.Methods 192, 261 (1982) R.Decker, K.-D.Wunsch, H.Wollnik, G.Jung, E.Koglin, G.Siegert A Hyperpure Germanium Detector for Precise Beta Endpoint Energy Determinations RADIOACTIVITY 28Al, 20F, 38Cl, 88Rb [from 27Al, 19F, 37Cl, 87Rb(d, p), E=1-6.5 MeV]; measured Eβ, βγ-coin, β-endpoint energies, Qβ. Hyperpure Ge detector, on-line separation.
doi: 10.1016/0029-554X(82)90831-X
1981DE25 Z.Phys. A301, 165 (1981) R.Decker, K.D.Wunsch, H.Wollnik, G.Jung, J.Munzel, G.Siegert, E.Koglin Prazise Qβ-Wert-Messungen mit einem Intrinsic-Germanium-Detektor an schweren, Neutronenreichen Spaltprodukten (Precise Q(β-) Values with an Intrinsic Germanium Detector for Heavy, Neutron-Rich Fission Products) RADIOACTIVITY 138,139,140,141,142,143,144,145,146Cs, 139,141,143,146Ba, 146La [from on-line fission product separation]; measured βγ-coin, β-end point energies; deduced Qβ. Intrinsic Ge detector.
doi: 10.1007/BF01419247
1980CA25 Z.Phys. A298, 219 (1980) F.Caitucoli, B.Leroux, G.Barreau, N.Carjan, T.Benfoughal, T.P.Doan, F.El Hage, A.Sicre, M.Asghar, P.Perrin, G.Siegert The Thermal-Neutron-Induced Alpha-Accompanied Fission of 235U Investigation of the Low Energy Part of the Alpha Spectrum NUCLEAR REACTIONS, Fission 235U(n, αF), E=thermal; measured σ(Eα); deduced asymmetry at low energies, multiplicative factor relative to binary fission.
1980DE02 Z.Phys. A294, 35 (1980) R.Decker, K.D.Wunsch, H.Wollnik, E.Koglin, G.Siegert, G.Jung Prazise Qβ-Wert-Messungen mit einem Intrinsic-Germanium Detektor an leichten, neutronenreichen Spaltprodukten RADIOACTIVITY 88,89,90,91,92,93,94,95,96,97Rb, 91,94,96Sr, 94,95,96Y [from on-line fission product separation]; measured Eβ, βγ-coin; deduced Q(β). Intrinsic Ge detector.
doi: 10.1007/BF01473120
1979BA62 Phys.Rev. C20, 2244 (1979) S.J.Balestrini, R.Decker, H.Wollnik, K.D.Wunsch, G.Jung, E.Koglin, G.Siegert Independent Yields of Rb and Cs Isotopes from Thermal-Neutron Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured relative abundancies of Rb, Cs isotopes. 88,89,90,91,92,93,94,95,96,97Rb, 137,138,139,140,141,142,143,144,145,146Cs deduced independent, fractional yields. Rb, Cs deduced charge displacement, dispersion, enhancement factor. Even-odd Z effect model. Mass separator, fast neutron detector.
doi: 10.1103/PhysRevC.20.2244
1978KO29 Z.Phys. A288, 319 (1978) E.Koglin, G.Jung, G.Siegert, R.Decker, K.D.Wunsch, H.Wollnik Half-Lives of the New Isotopes 100Rb, 100Sr, 145Cs and of 99Rb, 99Sr and 147Cs RADIOACTIVITY 100Rb, 100Sr, 148Cs, 99Rb, 99Sr, 147Cs [from 235U+n]; measured activity build-up, decay with β-multi-scaling, γ-multispectra; deduced T1/2.
doi: 10.1007/BF01415200
1978ST02 Z.Phys. A284, 95 (1978) R.Stippler, F.Munnich, H.Schrader, J.P.Bocquet, M.Asghar, G.Siegert, R.Decker, B.Pfeiffer, H.Wollnik, E.Monnand, F.Schussler Experimental Beta-Decay Energies of Short-Lived Light Fission Products RADIOACTIVITY 88Br, 90,92Kr, 90,92,93Rb, 93,95,96,97,98Sr, 96,97,97m,98,98mY, 98,100,101,102Nb, 99,100Zr; measured Eβ; deduced Qβ.
doi: 10.1007/BF01433881
1978WO09 Phys.Rev. C17, 2185 (1978) F.K.Wohn, K.D.Wunsch, H.Wollnik, R.Decker, G.Jung, E.Koglin, G.Siegert Identification of 147Cs and Half-Life Determinations for Cs and Ba Isotopes with A = 144-147 and Rb and Sr Isotopes with A = 96-98 RADIOACTIVITY 96,97,98Rb, 96,97,98Sr, 144,145,146,147Cs, 144,145,146,147Ba [from 235U(n, F)]; measured T1/2. Ge(Li), plastic scintillation detectors, mass separated activities.
doi: 10.1103/PhysRevC.17.2185
1978WU04 Z.Phys. A288, 105 (1978) K.D.Wunsch, R.Decker, H.Wollnik, J.Munzel, G.Siegert, G.Jung, E.Koglin Precision Beta Endpoint Energy Measurements of Rubidium and Cesium Fission Products with an Intrinsic Ge-Detector RADIOACTIVITY 88,89,90,91,92,93,94Rb, 138,139,140,141,142,143,144Cs; measured βγ-coin, Eβ; deduced Q.
1977PF01 J.Phys.(Paris) 38, 9 (1977) B.Pfeiffer, J.P.Bocquet, J.A.Pinston, R.Roussille, M.Asghar, G.Bailleul, R.Decker, J.Greif, H.Schrader, G.Siegert, H.Wollnik, J.Blachot, E.Monnand, F.Schussler Gamma Spectroscopy of Some Short-Lived Fission Products with the Isotope Separator Lohengrin RADIOACTIVITY 100Y, 100Zr, 149,150Ce, 150Pr, 136Te, 87Se; measured Eγ, Iγ, T1/2. 149Pr, 135,137Te, 86Se; measured Eγ, Iγ. 88Se; measured Eγ, Iγ; deduced ground state β-branching. 85Se; measured Eγ, Iγ, T1/2; deduced ground state β-branching.
doi: 10.1051/jphys:019770038010900
1976SI18 Phys.Rev. C14, 1864 (1976) G.Siegert, H.Wollnik, J.Greif, R.Decker, G.Fiedler, B.Pfeiffer Nuclear Charge Distribution of Fission Products from 235U(n(th), f) of the Masses 79 to 100 NUCLEAR REACTIONS 235U(n, F), E=th; measured σ(A, Z); deduced proton, neutron odd-even effect.
doi: 10.1103/PhysRevC.14.1864
1975AS04 Nucl.Phys. A247, 359 (1975) M.Asghar, J.P.Gautheron, G.Bailleul, J.P.Bocquet, J.Greif, H.Schrader, G.Siegert, C.Ristori, J.Crancon, G.I.Crawford The p(n) Values of the 235U(n(th), f) Produced Precursors in the Mass Chains 90, 91, 93-95, 99, 134 and 137-139 RADIOACTIVITY 90,91Br, 91Se, 93,94Kr, 93,94,95Rb, 99Y, 99Sr, 134Sn, 137,138Te, 137,138,139I [from 235U(n, F), E=thermal]; measured delayed neutrons, β-activity, T1/2; deduced delayed neutron probability.
doi: 10.1016/0375-9474(75)90642-9
1975BA36 Z.Phys. A273, 283 (1975) G.Bailleul, J.P.Bocquet, H.Schrader, R.Stippler, B.Pfeiffer, M.Asghar, C.Chauvin, J.P.Gautheron, J.Greif, G.Siegert, P.Armbruster, H.Ewald, J.Blachot, E.Monnand, F.Schussler Gamma-Ray Spectroscopy of Short-Lived Fission Products Using the Recoil Separator 'Lohengrin' RADIOACTIVITY 90Br, 95,96Rb, 96Sr, 96Y, 132Sb, 132Sn; measured T1/2, Eγ, Iγ. 96Sr; measured Eβ; deduced Qβ. 90Kr, 95,96Sr, 96Y deduced levels.
doi: 10.1007/BF01410011
1975CL02 Nucl.Phys. A247, 74 (1975) H.-G.Clerc, K.-H.Schmidt, H.Wohlfarth, W.Lang, H.Schrader, K.E.Pferdekamper, R.Jungmann, M.Asghar, J.P.Bocquet, G.Siegert Nuclear Charge Distribution of Mass-Separated Isobars from Thermal-Neutron-Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured nuclear charge distributions of fission products; deduced nuclear charge distribution widths; on-line mass separation.
doi: 10.1016/0375-9474(75)90278-X
1975GU03 Nucl.Phys. A242, 56 (1975) H.Gunther, G.Siegert, K.Wunsch, H.Wollnik Gamma-Ray Energies of Short-Lived Rb, Sr, and Y Isotopes Indicating Delayed Neutron Emission to Excited States RADIOACTIVITY 95,96,97Rb, 95,96,97Sr, 95,97Y; measured Eγ, Iγ, βγ-coin. 96,97Sr, 95,97Y, 96,97Zr deduced transitions. 95Sr, 96Y deduced levels. 96,97Sr deduced delayed-neutron decay probability. On-line mass separator.
doi: 10.1016/0375-9474(75)90033-0
1975SI04 Phys.Rev.Lett. 34, 1034 (1975) G.Siegert, J.Greif, H.Wollnik, G.Fiedler, R.Decker, M.Asghar, G.Bailleul, J.P.Bocquet, J.P.Gautheron, H.Schrader, P.Armbruster, H.Ewald Nuclear Charge Distributions in the Isobars 92 to 100 Resulting from Thermal Neutron Fission of Uranium-235 NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fractional yields; deduced nuclear charge distribution in isobars A=92-100.
doi: 10.1103/PhysRevLett.34.1034
1974CR06 J.Phys.(London) A7, L141 (1974) G.I.Crawford, S.J.Hall, J.D.Kellie, M.Asghar, G.Bailleul, J.P.Bocquet, C.Chauvin, J.P.Gautheron, H.Schrader, G.Siegert, J.Crancon, C.Ristori Population of Excited States in Delayed Neutron Emission RADIOACTIVITY 85As, 90Br, 95Rb; measured nγ-coin. 94Sr, 89Kr deduced levels.
doi: 10.1088/0305-4470/7/12/001
1974SI23 Phys.Lett. 53B, 45 (1974) G.Siegert, H.Wollnik, J.Greif, G.Fiedler, M.Asghar, G.Bailleul, J.P.Bocquet, J.P.Gautheron, H.Schrader, H.Ewald, P.Armbruster Direct Determination of the Nuclear Charge Distribution of Mass Separated Fission Products from 235U(n(th), f) NUCLEAR REACTIONS 235U(n, F), E=thermal; measured charge distribution of A=90-91 isobaric chains.
doi: 10.1016/0370-2693(74)90339-6
1974WU02 Phys.Rev. C10, 2523 (1974) K.Wunsch, H.Wollnik, G.Siegert Qβ Values of Neutron-Rich Cs Isotopes RADIOACTIVITY 141,142,143,144,145Cs [from 235U(n, F)]; measured Eβ; deduced Eβ max, Qβ. Mass separated Cs activities.
doi: 10.1103/PhysRevC.10.2523
1973WU03 J.Phys.(London) A6, L93 (1973) K.Wunsch, H.Gunther, G.Siegert, H.Wollnik Gamma Ray Energies of 143-145Cs and of their Beta Decay Products RADIOACTIVITY 143,144,145Cs, Ba, 144La [from 235U(n, F)]; measured Eγ, Iγ, βγ-coin, T1/2.
doi: 10.1088/0305-4470/6/7/005
1972GU18 Nucl.Phys. A196, 401 (1972) H.Gunther, G.Siegert, R.L.Ferguson, H.Ewald, E.Konecny Fission-Fragment Charge Distributions in Thermal-Neutron Induced Fission of 239Pu and 235U NUCLEAR REACTIONS, Fission 239Pu, 235U(n, F), E=thermal; measured fission-fragment charge distributions.
doi: 10.1016/0375-9474(72)90974-8
1972KO10 Nucl.Phys. A187, 426 (1972) E.Konecny, H.J.Specht, J.Weber, H.Weigmann, R.L.Ferguson, P.Osterman, M.Waldschmidt, G.Siegert Search for Conversion Electrons Populating the 236U Fission Isomer NUCLEAR REACTIONS, Fission 235U(n, γF), E=thermal; measured (fragment)(ce)-coin, -delay; deduced upper limit for isomeric/prompt fission ratio.
doi: 10.1016/0375-9474(72)90586-6
1970KO03 Z.Phys. 231, 59 (1970) E.Konecny, H.Gunther, H.Rosler, G.Siegert, H.Ewald Nuclear Charge Distribution of Heavy Fission Fragments from Thermal-Neutron-Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment charge, mass distributions.
doi: 10.1007/BF01394549
1967KO32 Nucl.Phys. A100, 465 (1967) E.Konecny, H.Gunther, G.Siegert, L.Winter Pairing effect in fission fragment charge distributions NUCLEAR REACTIONS 235U(n, F), E thermal; measured reaction products; deduced Nuclear charge distributions for fission fragments of A=137-139, ratio of the sum of the yields of doubly even nuclei to the sum of the yields of doubly odd nuclei.
doi: 10.1016/0375-9474(67)90423-x
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