NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = U.Quade Found 12 matches. 1992ST05 Z.Phys. A341, 145 (1992) M.Steinmayer, K.E.G.Lobner, L.Corradi, U.Lenz, U.Quade, P.R.Pascholati, K.Rudolph, W.Schomburg Fission and Gamma-Ray Decay of the 238U Shape Isomer RADIOACTIVITY 238mU [from 238U(d, np), E=18 MeV]; measured γ(ce)-coin; deduced delayed fission T1/2. 238U deduced transitions.
doi: 10.1007/BF01298474
1990CO06 Z.Phys. A335, 55 (1990) L.Corradi, S.J.Skorka, U.Lenz, K.E.G.Lobner, P.R.Pascholati, U.Quade, K.Rudolph, W.Schomburg, M.Steinmayer, H.G.Thies, G.Montagnoli, D.R.Napoli, A.M.Stefanini, A.Tivelli, S.Beghini, F.Scarlassara, C.Signorini, F.Soramel Near-Barrier Transfer and Fusion of the Systems 33S + 90,91,92Zr NUCLEAR REACTIONS, ICPND 90,91,92Zr(33S, X), E=110.6-118.7 MeV; measured σ(fragment θ, E), fragment mass spectra; deduced reaction, fusion σ.
1990MA49 Nucl.Phys. A515, 433 (1990) G.Martinez, G.Barreau, A.Sicre, T.P.Doan, P.Audouard, B.Leroux, W.Arafa, R.Brissot, J.P.Bocquet, H.Faust, P.Koczon, M.Mutterer, F.Gonnenwein, M.Asghar, U.Quade, K.Rudolph, D.Engelhardt, E.Piasecki Mass and Nuclear Charge Yields for 237Np(2n(th), f) at Different Fission Fragment Kinetic Energies NUCLEAR REACTIONS 239Np(n, F), E=thermal; measured light fission product mass versus kinetic energies; deduced fractional independent fission yields, odd-even effects of elements, isotones. Double neutron capture on 237Np target.
doi: 10.1016/0375-9474(90)90593-B
1990ST29 Z.Phys. A337, 371 (1990) M.Steinmayer, K.E.G.Lobner, L.Corradi, U.Lenz, P.R.Pascholati, U.Quade, K.Rudolph, W.K.Schomburg, S.J.Skorka Isomeric State at 945.3 keV in 237Np NUCLEAR REACTIONS 238U(p, 2n), E=12.6 MeV; measured γ(electron)-coin, γ(electron)(t). 237Np deduced isomer, T1/2, decay, J, π, configuration, transitions γ-multipolarity, hindrance factors.
1989DJ01 Nucl.Phys. A496, 346 (1989) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.
doi: 10.1016/0375-9474(89)90179-6
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
1987LO10 Nucl.Instrum.Methods Phys.Res. B26, 301 (1987) K.E.G.Lobner, U.Lenz, U.Quade, K.Rudolph, W.Schomburg, S.J.Skorka, M.Steinmayer Munich High-Frequency Recoil Spectrometer NUCLEAR REACTIONS 24Mg(58Ni, X)76Rb/77Rb/79Rb/77Sr/79Sr/80Sr/76Kr/78Kr/79Y/80Y/80Zr, E=177 MeV; measured residue production σ. Recoil spectrometer.
doi: 10.1016/0168-583X(87)90767-1
1986CL02 Nucl.Phys. A452, 277 (1986) H.-G.Clerc, W.Lang, M.Mutterer, C.Schmitt, J.P.Theobald, U.Quade, K.Rudolph, P.Armbruster, F.Gonnenwein, H.Schrader, D.Engelhardt Cold Fragmentation in Thermal-Neutron-Induced Fission of 233U and 235U NUCLEAR REACTIONS 233,235U(n, F), E=thermal; measured light fission product mass yields at high kinetic energies; deduced influence of nucleon pairing, reaction Q.
doi: 10.1016/0375-9474(86)90310-6
1984SK03 Nuovo Cim. 81A, 331 (1984) S.J.Skorka, D.Evers, K.E.G.Lobner, R.Pengo, U.Quade, K.Rudolph, I.Weidl Experiments with the Munich Recoil Spectrometer NUCLEAR REACTIONS, ICPND 100,98,96,94,92Mo(32S, X), (36S, X), E(cm) ≈ 74-90 MeV; measured fusion σ(E). 12C(16O, p), E(cm)=19-26 MeV; measured σ(Ep), σ(θ) vs E. 27Al deduced high-spin state decay characteristics. Recoil spectrometer.
doi: 10.1007/BF02724173
1984WE16 Z.Phys. A319, 67 (1984) I.Weidl, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, K.Rudolph, S.J.Skorka Properties of Unbound High-Spin States in 27Al NUCLEAR REACTIONS 12C(16O, p), E(cm)=18.7-30.1 MeV; measured σ(Ep), σ(θ) vs E, recoil velocity spectra. 27Al deduced resonances, J, π, α-, γ-, n-branching ratios, shape characteristics, (Γγ/Γ), (Γn/Γ).
doi: 10.1007/BF01429769
1983PE19 Nucl.Phys. A411, 255 (1983) R.Pengo, D.Everts, K.E.G.Lobner, U.Quade, K.Rudolph, S.J.Skorka, I.Weidl Nuclear Structure Effects in Sub-Barrier Fusion Cross Sections NUCLEAR REACTIONS, ICPND 92,94,96,98,100Mo, 100,101,102,104Ru, 103Rh, 104,105,106,110Pd(32S, X), (36S, X), E=72-93 MeV; measured evaporation residues; deduced fusion σ(E) around, below Coulomb barrier, zero-point motion, two-neutron transfer reaction role. Enriched targets, heavy ion recoil spectrometer.
doi: 10.1016/0375-9474(83)90392-5
1983RU01 Nucl.Instrum.Methods 204, 407 (1983) K.Rudolph, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, S.J.Skorka, I.Weidl The Munich RF-Recoil Spectrometer for the Observation of Heavy-Ion Reaction Products at Zero Degree NUCLEAR REACTIONS 12C(16O, X), E=53.6 MeV; measured σ(fragment) vs Z, σ(fragment) vs mass for Mg isotopes, (24Mg)(α)-coin; 12C(16O, p), (16O, pn), E=53.6 MeV; measured residual nuclei recoils. 104Ru(36S, X), E=100 MeV; measured evaporation residue transmission. RF recoil spectrometer.
doi: 10.1016/0167-5087(83)90069-8
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