NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Schrader Found 20 matches. 1993BA08 Nucl.Phys. A553, 313c (1993) H.Backe, H.Barth, J.Bonn, B.Degen, Th.Edling, L.Fleischmann, J.U.Grooss, A.Hermanni, G.Kube, P.Leiderer, Th.Loeken, A.Molz, R.B.Moore, A.Osipowicz, E.W.Otten, A.Picard, M.Przyrembel, M.Schrader, M.Steininger, Ch.Weinheimer A New Upper Limit of the Electron Antineutrino Rest Mass from Tritium β-Decay RADIOACTIVITY 3H(β-); measured β-endpoint spectrum; deduced ν(bar)(e) rest mass upper limit. Molecular tritium, new solenoid retarding spectrometer.
doi: 10.1016/0375-9474(93)90632-8
1993WE03 Phys.Lett. 300B, 210 (1993) Ch.Weinheimer, M.Przyrembel, H.Backe, H.Barth, J.Bonn, B.Degen, T.Edling, H.Fischer, L.Fleischmann, J.U.Grooss, R.Haid, A.Hermanni, G.Kube, P.Leiderer, Th.Loeken, A.Molz, R.B.Moore, A.Osipowicz, E.W.Otten, A.Picard, M.Schrader, M.Steininger Improved Limit on the Electron-Antineutrino Rest Mass from Tritium β-Decay RADIOACTIVITY 3H(β-); measured β-spectrum endpoint energy; deduced electron-antineutrino mass upper limit. 3H, 3He deduced atomic mass difference.
doi: 10.1016/0370-2693(93)90355-L
1992PI10 Z.Phys. A342, 71 (1992) A.Picard, H.Backe, J.Bonn, B.Degen, R.Haid, A.Hermanni, P.Leiderer, A.Osipowicz, E.W.Otten, M.Przyrembel, M.Schrader, M.Steininger, Ch.Weinheimer Precision Measurement of the Conversion Electron Spectrum of 83mKr with a Solenoid Retarding Spectrometer RADIOACTIVITY 83mKr(IT) [from 83Rb decay]; measured I(ce). 83Kr deduced transition energies. High precision, solenoid retarding spectrometer, submonolayer surface of 83mKr frozen onto a cold backing.
doi: 10.1007/BF01294491
1992PI11 Nucl.Instrum.Methods Phys.Res. B63, 345 (1992) A.Picard, H.Backe, H.Barth, J.Bonn, B.Degen, Th.Edling, R.Haid, A.Hermanni, P.Leiderer, Th.Loeken, A.Molz, R.B.Moore, A.Osipowicz, E.W.Otten, M.Przyrembel, M.Schrader, M.Steininger, Ch.Weinheimer A Solenoid Retarding Spectrometer with High Resolution and Transmission for keV Electrons RADIOACTIVITY 83mKr(IT); measured I(ce); deduced transition energy. Solenoid retarding spectrometer.
doi: 10.1016/0168-583X(92)95119-C
1983SZ03 Nucl.Phys. A404, 142 (1983) E.M.Szanto, A.Szanto De Toledo, H.V.Klapdor, G.Rosner, M.Schrader Yrast and High-Spin States in 22Ne NUCLEAR REACTIONS 11B(13C, d), 13C(11B, d), E(cm)=19 MeV; measured σ(θ). 22Ne deduced high-spin states. 24Na deduced critical angular momentum. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(83)90419-0
1979SC03 Z.Phys. A289, 193 (1979) M.Schrader, A.Szanto de Toledo, H.V.Klapdor A New Possibility of Identifying High-Spin States at High Excitation Energies NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; calculated probability of identifying high-spin states. Spin-dependent anisotropy of σ(θ) predicted by statistical model.
doi: 10.1007/BF01435937
1979SZ03 Phys.Rev. C19, 555 (1979) A.Szanto de Toledo, M.Schrader, E.M.Szanto, H.V.Klapdor Effect of the Critical Angular Momentum on the High Spin Selectivity of Heavy-Ion Compound Reactions NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; calculated σ(θ), σ(J); deduced σ(90°) is favored, useful for high spin spectroscopy. Statistical model.
doi: 10.1103/PhysRevC.19.555
1979SZ04 Nucl.Phys. A315, 500 (1979) A.Szanto de Toledo, M.Schrader, E.M.Szanto, G.Rosner, H.V.Klapdor High-Spin States in 24Mg and Upper Limits for Particle Spectroscopy of High Spins by Heavy-Ion Compound Reactions NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; measured σ(θ). 24Mg deduced high-spin states, critical angular momentum. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(79)90626-2
1978KL05 Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 64 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.1, 51 (1978) H.V.Klapdor, M.Schrader, G.Bergdolt, A.M.Bergdolt, Y.V.Naumov Analog-Antianalog Transitions in Arsenic Isotopes NUCLEAR REACTIONS 72Ge(p, γ), E=3.15-5.05 MeV; 74Ge(p, γ), E=3.25-5.29 MeV; 76Ge(p, γ), E=3.80-5.18 MeV; measured σ(E, Eγ). 73,75,77As deduced analog, antianalog states, γ-branching, B(M1).
1978SZ04 Phys.Rev. C17, 2253 (1978) A.Szanto de Toledo, H.V.Klapdor, H.Hafner, W.Saathoff, E.M.Szanto, M.Schrader Masses of 121,123,125I and Energy Levels of the Highly Neutron-Deficient 121I NUCLEAR REACTIONS 120,122,124Te(3He, d), E=36 MeV; measured σ(Ed, θ); deduced Q. 120,122,124,126,128,130Te(α, t), 126,128,130Te(3He, d), E=36 MeV; measured σ. 121I deduced mass excess, levels. 123,125I deduced mass excess.
doi: 10.1103/PhysRevC.17.2253
1978SZ09 J.Phys.(London) G4, L187 (1978) A.Szanto de Toledo, H.V.Klapdor, H.Hafner, W.Saathoff, E.M.Szanto, M.Schrader, H.Dias Structure of the Neutron-Deficient Nuclide 121I NUCLEAR REACTIONS 120Te(3He, d), E=36 MeV; measured σ(Ed, θ); deduced Q. 121I deduced mass excess, levels, L, J, π, S. DWBA analysis.
doi: 10.1088/0305-4616/4/7/007
1978SZ10 Phys.Lett. 78B, 58 (1978) A.Szanto de Toledo, M.Schrader, G.Rosner, E.M.Szanto, H.V.Klapdor Yrast States in 24Mg up to 24 MeV Excitation Energy NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; measured σ(Ed, θ). 24Mg deduced levels, J, π.
doi: 10.1016/0370-2693(78)90347-7
1976BE30 Nucl.Phys. A263, 477 (1976) G.Bergdolt, A.M.Bergdolt, H.V.Klapdor, M.Schrader The M1 Strength Distribution in the γ-Decay of the g9/2 Analogue State in 61Cu NUCLEAR REACTIONS 60Ni(p, γ), E=3690-3790 keV; measured Eγ, Iγ, absolute γ yields. 61Cu deduced resonances, Γγ, Coulomb energy differences. T.
doi: 10.1016/0375-9474(76)90201-3
1976SC13 Nucl.Phys. A263, 193 (1976) M.Schrader, H.Reiss, G.Rosner, H.V.Klapdor Investigation of the Level Schemes of 73,75,77As via the (3He, d) Reaction NUCLEAR REACTIONS 72,74,76Ge(3He, d), E=23 MeV; measured σ(Ed, θ); deduced Q. 73,75,77As deduced levels, L(p), C2S. Enriched targets.
doi: 10.1016/0375-9474(76)90168-8
1975KL05 Nucl.Phys. A244, 157 (1975) H.V.Klapdor, G.Rosner, H.Reiss, M.Schrader Prediction of the High-Spin Selectivity of Compound Reactions Induced by Heavy Ions NUCLEAR REACTIONS 10B, 12C(12C, d), 12C(14N, d), E=40-52 MeV; calculated σ(E, Ed, θ). 11B, 13C(14N, p), E=40-52 MeV; calculated σ(E, Ep, θ). 10B(14N, α), E=35 MeV; calculated σ(Eα, θ). 12C(14N, 6Li), E=52-120 MeV; calculated σ(E, E(6Li), θ); deduced reaction selectivity.
doi: 10.1016/0375-9474(75)90015-9
1975KL06 Nucl.Phys. A245, 133 (1975) H.V.Klapdor, M.Schrader, G.Bergdolt, A.M.Bergdolt The γ-Decay of the g9/2 Analogue State in 59Cu NUCLEAR REACTIONS 58Ni(p, γ), E=3483, 3532, 3547 keV; measured Eγ, Iγ, σ(Eγ, θ). 59Cu deduced new levels, isobaric analog state, J of resonances, bound states, γ-width. Enriched target.
doi: 10.1016/0375-9474(75)90085-8
1975SC44 Phys.Lett. 60B, 39 (1975) M.Schrader, H.V.Klapdor, G.Bergdolt, A.M.Bergdolt Systematics of Analogue-to-Antianalogue M1 Transitions up to g9/2 and d5/2 Analogue States in As Isotopes NUCLEAR REACTIONS 72,74Ge(p, γ), E=3.3-5.3 MeV; measured σ(E, Eγ). 73,75As hindered transitions deduced poor fit to systematics of analog-to-antianalog M1 transitions.
doi: 10.1016/0370-2693(75)90521-3
1974KL05 Phys.Lett. 49B, 431 (1974) H.V.Klapdor, H.Reiss, G.Rosner, M.Schrader Spectroscopy with High Spin Selective Compound Reactions Induced by Heavy Ions NUCLEAR REACTIONS 10B(12C, d), E=45 MeV; measured σ(Ed). 20Ne deduced levels.
doi: 10.1016/0370-2693(74)90627-3
1974SC17 Nucl.Phys. A223, 365 (1974) M.Schrader, K.Buchholz, H.V.Klapdor The γ-Decay of a p3/2 Analogue State in 51Mn NUCLEAR REACTIONS 50Cr(p, γ), E=1059, 1071 keV; measured Eγ, Iγ, γ(θ); deduced Q. 51Mn deduced levels, IAR, J, π, γ-mixing, level-width, β(ground-state).
doi: 10.1016/0375-9474(74)90420-5
1973SC29 Nucl.Phys. A213, 173 (1973) M.Schrader, K.Buchholz, H.V.Klapdor Das Niveauschema von 47V aus dem γ-Zerfall von Analogresonanzen NUCLEAR REACTIONS 46Ti(p, γ), E=1.546, 1.549, 1.565, 1.572 MeV; measured Eγ, Iγ, (p, γ)(θ). 47V deduced levels, isobaric analog states, J, π, γ-mixing ratios, γ-width. Enriched target.
doi: 10.1016/0375-9474(73)90190-5
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