NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Nolte Found 33 matches. 2007ST08 Nucl.Instrum.Methods Phys.Res. B259, 739 (2007) C.Stan-Sion, A.Letourneau, H.Reithmeier, V.Lazarev, M.Enachescu, E.Nolte AMS measurement of the neutron capture cross-section 209Bi(n, γ)210mBi NUCLEAR REACTIONS 209Bi(n, γ)210mBi, E=thermal; measured cross section using accelerator mass spectrometry.
doi: 10.1016/j.nimb.2007.01.211
2003RU05 Eur.Phys.J. A 17, 633 (2003) W.Ruhm, G.Rugel, T.Faestermann, K.Knie, A.Wallner, B.Heisinger, E.Nolte, A.A.Marchetti, R.E.Martinelli, K.L.Carroll, G.Korschinek Cosmic-ray-induced 63Ni - A potential confounder of fast-neutron-induced 63Ni in copper samples from Hiroshima
doi: 10.1140/epja/i2003-10034-2
2000HA33 Astropart.Phys. 14, 33 (2000) T.Hagner, R.von Hentig, B.Heisinger, L.Oberauer, S.Schonert, F.von Feilitzsch, E.Nolte Muon-Induced Production of Radioactive Isotopes in Scintillation Detectors NUCLEAR REACTIONS 12C(μ+, X)11C/10C/9C/8B/11Be/7Be/9Li/8Li/8He/6He, E=100, 190 GeV; measured σ; deduced energy-dependence parameter. Activation technique, implications for solar neutrino measurements discussed.
doi: 10.1016/S0927-6505(00)00103-1
1996ST39 Nucl.Instrum.Methods Phys.Res. B117, 26 (1996) C.Stan-Sion, D.Huggle, E.Nolte, A.Blinov, M.Dumitru AMS Measurements of the Production Cross Sections of 36Cl with Protons up to 1 GeV NUCLEAR REACTIONS 40Ar(p, nα), (p, 3n2p), E=17-1000 MeV; measured production σ. Accelerator mass spectrometry.
doi: 10.1016/0168-583X(96)00240-6
1994RU19 Planet.Space Sci. 42, 227 (1994) W.Ruhm, B.Schneck, K.Knie, G.Korschinek, L.Zerle, E.Nolte, D.Weselka, H.Vonach A New Half-Life Determination of 59Ni RADIOACTIVITY 55Fe, 59Ni(EC) [from 54Fe, 58Ni(n, γ)]; measured X-ray spectra, T1/2. NUCLEAR REACTIONS 60Ni(n, 2n), E=14.8 MeV; measured σ. Accelerator mass spectrometry. Comparison with model predictions. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22583. 1992NE08 Z.Phys. A341, 239 (1992) Neutrino Oscillations in the Sun and the 205Tl Solar Neutrino Experiment NUCLEAR REACTIONS 205Tl(ν, e-), E=solar source; calculated ν-induced transition rates to final nuclear states, capture rate; deduced ν(e) flavor oscillations dependent suppression factors. Hydrogen burning reactions in sun.
doi: 10.1007/BF01298487
1992TH07 Phys.Lett. 291B, 484 (1992) Limits on Small Violations of the Pauli Exclusion Principle in the Primordial Nucleosynthesis
doi: 10.1016/0370-2693(92)91408-2
1991NE04 Z.Phys. A340, 415 (1991) S.Neumaier, E.Nolte, H.Morinaga Feasibility Studies of the Geochemical Solar Neutrino Experiment 205Tl(ν, e-)205Pb NUCLEAR REACTIONS 205Tl(ν, e-), E not given; measured not given; deduced residual nucleus production, geochemical 205Tl solar neutrino experiment feasibility.
doi: 10.1007/BF01290330
1991NO05 Z.Phys. A340, 411 (1991) E.Nolte, T.Faestermann, A.Gillitzer, G.Korschinek, D.Muller, V.M.Novikov, A.A.Pomansky, A.Ljubicic, D.Miljanic Test of the Pauli Exclusion Principle for Nucleons and Atomic Electrons by Accelerator Mass Spectrometry
doi: 10.1007/BF01290329
1991NO08 J.Phys.(London) G17, S355 (1991) E.Nolte, T.Brunner, T.Faestermann, A.Gillitzer, G.Korschinek, D.Muller, B.Schneck, D.Weselka, V.N.Novikov, A.A.Pomansky, A.Ljubicic, D.Miljanic, H.Vonach Accelerator Mass Spectrometry for Tests of the Pauli Exclusion Principle and for Detection of ββ Decay Products NUCLEAR REACTIONS 60Ni(n, 2n), E=14.8 MeV; measured σ. Accelerator mass spectrometry technique. RADIOACTIVITY 59Ni(EC), (β+) [from 60Ni(n, 2n), E=14.8 MeV]; measured T1/2. Accelerator mass spectrometry technique.
doi: 10.1088/0954-3899/17/S/037
1990RU11 Nucl.Instrum.Methods Phys.Res. B52, 557 (1990) W.Ruhm, K.Kato, G.Korschinek, H.Morinaga, A.Urban, L.Zerle, E.Nolte The Neutron Spectrum of the Hiroshima A-Bomb and the Dosimetry System 1986 NUCLEAR REACTIONS 40Ca(n, γ), E ≤ 3 keV; measured resonance integral. AMS, γ-spectroscopy techniques.
doi: 10.1016/0168-583X(90)90476-B
1989LJ01 Fizika(Zagreb) A21, 413 (1989) A.Ljubicic, D.Miljanic, B.A.Logan, E.H.Nolte Proposal for the Search of Small Violation of the Pauli Exclusion Principle in Nuclei
1987GI02 Z.Phys. A326, 107 (1987) A.Gillitzer, T.Faestermann, K.Hartel, P.Kienle, E.Nolte Groundstate Proton Radioactivity of Nuclei in the Tin Region NUCLEAR REACTIONS 58Ni, 54Fe(58Ni, X)113Cs/109I, E=250 MeV; measured delayed α-, proton yields; deduced residual production yields. RADIOACTIVITY 109I, 113Cs(p) [from 54Fe, 58Ni(58Ni, X), E=250 MeV]; measured proton decay energies, T1/2; deduced Qα, spectroscopic factors. 105Sb(p) [from 50Cr(58Ni, 2np), E=250 MeV]; measured proton decay branch; deduced no proton decay, decay energy. Annular gas detector system.
1985RY02 Z.Phys. A322, 263 (1985) K.Rykaczewski, I.S.Grant, R.Kirchner, O.Klepper, V.T.Koslowsky, P.O.Larson, E.Nolte, G.Nyman, E.Roeckl, D.Schardt, L.Spanier, P.Tidemand-Petersson, E.F.Zganjar, J.Zylicz The Gamow-Teller Transitions in the 96Pd → 96Rh Decay RADIOACTIVITY 96Pd(EC), (β+) [from 60Ni(40Ca, xnyp), E=167 MeV]; measured Eγ, Iγ, γγ-coin; deduced Q(EC), mass excess, (β+/(EC+β+)) branching ratios. 96Rh deduced levels, J, π, γ-multipolarity, Gamow-Teller transition strengths.
doi: 10.1007/BF01411890
1984FA04 Phys.Lett. 137B, 23 (1984) T.Faestermann, A.Gillitzer, K.Hartel, P.Kienle, E.Nolte Evidence for Proton Radioactivity of 113Cs and 109I RADIOACTIVITY 113Cs, 109I(p) [from 58Ni, 54Fe(58Ni, X), E=250 MeV]; measured Ep, Ip, p-decay T1/2. NUCLEAR REACTIONS 58Ni, 54Fe(58Ni, X), E=250 MeV; measured Ep, Ip; deduced evidence for proton decaying 113Cs, 109I.
doi: 10.1016/0370-2693(84)91098-0
1983KO07 Z.Phys. A310, 137 (1983) The 2.6 μs (21/2)+ Isomer in 93Ru RADIOACTIVITY 93Ru [from 58Ni, 56,57Fe(40Ca, xnyp), E=135-171 MeV]; measured Eγ, Iγ, γγ-coin; deduced levels, J, π, isomer T1/2, γ-branching, B(E2). Shell model.
doi: 10.1007/BF01433624
1983KO43 Z.Phys. A314, 135 (1983) The Level Scheme of 91Tc and the β Decay of 91Ru(9/2+) RADIOACTIVITY 91Ru(β+), (EC) [from 54Fe(40Ca, n2p), E=135 MeV]; measured γ-spectra, T1/2. 91Ru level deduced J, π. 91Tc deduced levels, J, π, γ-branching. NUCLEAR REACTIONS 54Fe(40Ca, n2p), E=135 MeV; 58Ni(40Ca, 3pα), E=140, 150, 160, 171 MeV; 54Fe(40Ca, 3p), E=135, 120, 129 MeV; measured Eγ, Iγ, γ(θ), σ(Eγ, E), γγ(t), γ-anisotropy, γ yield vs E. 91Tc deduced levels, J, π, γ-branching, B(λ).
doi: 10.1007/BF01879871
1982CH08 Lett.Nuovo Cim. 33, 159 (1982) I.Chiodi, S.Lunardi, M.Morando, C.Signorini, G.Fortuna, W.Starzecki, A.M.Stefanini, G.Korschinek, H.Morinaga, E.Nolte, W.Schollmeier Multinucleon Transfer in the Interaction of 58Ni with 124Sn around the Coulomb Barrier NUCLEAR REACTIONS 124Sn(58Ni, X), E=249 MeV; measured σ(fragment E, mass); deduced multi-nucleon transfer, kinematic effects.
doi: 10.1007/BF02725528
1982GU07 Z.Phys. A305, 297 (1982) A 150 ms 10+ Isomer in 146Dy NUCLEAR REACTIONS 90,91Zr(58Ni, xnypzα)146Ho/146Dy/145Dy/145Tb/144Tb/143Tb/142Tb/144Gd/142Gd/, E=233, 250 MeV; measured Eγ, Iγ, σ(Eγ), γγ-, γ(ce)-coin; deduced relative yields for 146Ho, 146,145Dy, 145,144,143,142Tb, 144,142Gd. 146Dy deduced levels, ICC, γ-branching, γ-multipolarity, isomer J, π, T1/2, B(λ). RADIOACTIVITY 146Ho [from 90Zr(58Ni, np), E=250 MeV]; measured β-decay T1/2; deduced Q(EC), log ft. 146Dy deduced levels, γ-branching, Iβ.
doi: 10.1007/BF01419077
1982KU15 Z.Phys. A308, 21 (1982) W.Kurcewicz, E.F.Zganjar, R.Kirchner, O.Klepper, E.Roeckl, P.Komninos, E.Nolte, D.Schardt, P.Tidemand-Petersson Investigations of very Neutron-Deficient Isotopes below 100Sn in 40Ca-Induced Reactions RADIOACTIVITY 94Rh(β+p), 94Pd(β+), (EC), 95mPd(β+p), 96Pd(β+), (EC), 96Ag(β+p), 97Cd(β+p), 97Ag(β+), 98Ag(β+), 99Cd(β+p), 99mAg(β+), (EC), 102In(β+), (EC), 100In(β+p) [from 58,60,62Ni, 63,65Cu(40Ca, xnyp), E=4 MeV/nucleon]; measured T1/2, Eγ, Iγ, β-delayed Ep, Ip, βγ-, p(X-ray)-coin, E(X-ray), I(X-ray); deduced log ft. 95,96Rh, 96,98Pd deduced levels, J, π, γ-branching. On-line mass separation. NUCLEAR REACTIONS 58,62Ni, 63Cu(40Ca, xnyp), E=4 MeV/nucleon; measured Eγ, Iγ, β-delay Ep, Ip, βγ-, p(X-ray)-coin, E(X-ray), I(X-ray); deduced evidence for 94Rh, 96Ag, 97Cd, 100In. 94Pd precursors.
doi: 10.1007/BF01415845
1982NO06 Z.Phys. A305, 289 (1982) Beta Delayed Proton Emission from the 14s 21/2+ Spin Gap Isomer in 95Pd NUCLEAR REACTIONS 58Ni(40Ca, n2p), E=135 MeV; measured Eγ, Iγ, γγ-coin, β-delayed Ep, Ip, pγ-coin, pγ(t). 95Pd deduced isomer decay, J, π, T1/2, Q(EC), log ft, γ-multipolarity. 95Rh deduced Iγ, γ-branching. 94Ru level deduced J, π, γ-branching. Enriched target.
doi: 10.1007/BF01419075
1982NO07 Z.Phys. A306, 211 (1982) E.Nolte, G.Colombo, S.Z.Gui, G.Korschinek, W.Schollmeier, P.Kubik, S.Gustavsson, R.Geier, H.Morinaga Very Proton Rich Nuclei with N ≈ 82 I. In-Beam γ Spectroscopy: Seniority isomerism in 150 Er NUCLEAR REACTIONS 92,94Mo, 93Nb(58Ni, xnypzα)/148Tm/150Tm/147Er/148Er/149Er/150Er/145Ho/149Ho/148Ho/146Ho/147Ho/144Dy/146Dy/148Dy, E=233-250 MeV; 92Mo(60Ni, xnypzα), E=240-259 MeV; measured σ(Eγ), γγ-coin, Eγ, Iγ, γ(t), relative yields for residuals; deduced two proton evaporation dominance. 148,150Er, 147Ho deduced levels, J, π, T1/2. Bunched, pulsed beam techniques.
doi: 10.1007/BF01415123
1982NO08 Z.Phys. A306, 223 (1982) E.Nolte, S.Z.Gui, G.Colombo, G.Korschinek, K.Eskola Very Proton Rich Nuclei with N ≈ 82 II. Beta Decay Studies RADIOACTIVITY 144,145,146Tb, 145,146Dy, 147,148,150Ho, 148,150Er, 148,150Tm [from 90,91,92Zr, 93Nb, 92,94Mo(58Ni, xnyp), E=233-250 MeV]; measured γγ-coin, EC/β+, Eγ, Iγ, β-decay T1/2; deduced log ft, Iβ. 150Er deduced Q(EC). 144,145,146Gd, 147,148,150Dy, 146Tb, 148,150Ho deduced levels, γ-branching.
doi: 10.1007/BF01415124
1982NO13 Z.Phys. A309, 33 (1982) E.Nolte, G.Korschinek, Ch.Setzensack Seniority Isomerism in the N = 82 Isotone 152Yb; Favoured β transitions πh11/2 → νh9/2 RADIOACTIVITY 152Yb(β+) [from 96Ru(58Ni, 2p), E=238, 250 MeV]; 151Tm(β+) [from 96Ru(58Ni, 3p), E=250 MeV]; 152mTm [from 152Yb decay]; measured Eγ, Iγ, γγ-coin, γγ(t). 152Yb deduced isomer T1/2, Q(EC), log ft. 151,152Tm deduced Q(EC), log ft. 152Tm, 152,151Er levels deduced γ-branching. NUCLEAR REACTIONS 96Ru(58Ni, 2p), (58Ni, n2p), (58Ni, 3p), (58Ni, n3p), (58Ni, 4p), (58Ni, 2pα), E=238, 250 MeV; measured Eγ, Iγ, γγ-coin, γγ(t); deduced residuals relative yield. 151Tm deduced levels, isomer T1/2, γ-branching. 152Yb deduced levels, isomer T1/2, B(E2), γ-branching. Thick target.
doi: 10.1007/BF01420148
1981SP03 Z.Phys. A299, 113 (1981) L.Spanier, S.Z.Gui, H.Hick, E.Nolte The Mass of the Nucleus 148Dy RADIOACTIVITY 148Dy [from 93Nb(58Ni, X), E=249 MeV]; measured γγ-coin, EC/β+. 148Dy deduced mass excess. 152Er, 156Yb, 160Hf, 164W; analyzed Qα; deduced mass excess.
doi: 10.1007/BF01440912
1980NO05 Phys.Lett. B97, 55 (1980) β Delayed Proton Emission from a Long-Lived High-Spin Isomer in 95Pd RADIOACTIVITY 95Pd [from 58Ni(40Ca, n2p), E=135 MeV]; measured Eγ, Iγ, γγ-coin, γ(θ), T1/2, β-delay Ep, Ip; deduced log ft, total β-branching. 95Rh deduced levels, J, π, γ-branching, T1/2. 95Pd deduced high-spin isomer, proton precursor character.
doi: 10.1016/0370-2693(80)90545-6
1980NO06 Z.Phys. A298, 191 (1980) Investigation of Very Neutron Deficient Ru and Rh Nuclei with the Help of (40Ca; yp + zαγ) Reactions RADIOACTIVITY 94Rh [from 58Ni(40Ca, ypzα), E=135, 160 MeV]; measured Eγ, Iγ; deduced log ft. 94Ru deduced levels, J, π, γ-branching. NUCLEAR REACTIONS 58Ni(40Ca, ypzα), E=135, 160 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DSA, recoil, γγ(t), σ(Eγ). 92,94Ru, 95Rh deduced levels, J, π, T1/2, γ-branching, B(λ), δ.
doi: 10.1007/BF01418657
1979AU03 Z.Phys. A289, 255 (1979) P.Auger, T.H.Chiang, J.Galin, B.Gatty, D.Guerreau, E.Nolte, J.Pouthas, X.Tarrago, J.Girard Observation of New Nuclides 37Si, 40P, 41S, 42S Produced in Deeply Inelastic Reactions Induced by 40Ar on 238U NUCLEAR REACTIONS 238U(Ar, X), E=263 MeV; measured fractional-charge parameter versus A; deduced evidence for 37Si, 30P, 41,42S. Tof measurements.
doi: 10.1007/BF01415785
1977KO05 Z.Phys. A281, 409 (1977) G.Korschinek, E.Nolte, H.Hick, K.Miyano, W.Kutschera, H.Morinaga Investigation of Neutron Deficient Zr and Nb Nuclei with Heavy Ion Induced Compound Reactions RADIOACTIVITY 87,84,86Nb, 87Mo; measured T1/2. NUCLEAR REACTIONS Fe, Ni, Se(32S, X), (12C, X); measured in-beam γ, γγ-coin, γ(θ). 84,86Zr deduced levels, J, π. 87Nb, 87Zr deduced transitions.
doi: 10.1007/BF01408190
1975NO11 Z.Phys. A275, 33 (1975) Rotational Bands in 77Kr NUCLEAR REACTIONS 63Cu(16O, pnγ), E=42 MeV; measured γγ-coin, σ(Eγ, θ). 64Ni(16O, 3nγ), E=42, 47, 52, 57 MeV; measured Eγ, Iγ, recoil distance DSA. 64Zn(16O, n2pγ), 66Zn(16O, nαγ), E=44, 51, 58 MeV; measured Eγ, Iγ. 77Kr deduced levels, K, J, π, T1/2, B(λ).
doi: 10.1007/BF01409497
1974NO08 Z.Phys. 268, 267 (1974) E.Nolte, Y.Shida, W.Kutschera, R.Prestele, H.Morinaga Investigation of Neutron Deficient Nuclei in the Region 28 < N, Z < 50 With the Help of Heavy Ion Compound Reactions RADIOACTIVITY 69Se, 77Rb; measured T1/2, Eγ, Iγ. 70Se measured T1/2. 69As deduced levels. NUCLEAR REACTIONS 40Ca(32S, 2pαγ), (32S, 4pγ), (32S, 3pγ), (32S, n3pγ), E=90, 100 MeV; 58Ni(14N, npγ), E=36 MeV; 40Ca(40Ca, 2pαγ), E=115 MeV; measured Eγ, Iγ, γγ-coin; 54Fe(14N, npγ), E=36 MeV; 66,68Zn(16O, 2nγ), E=44, 51, 58 MeV; measured Eγ, Iγ; 58Ni(12C, 2pγ), E=36 MeV; measured γγ-coin, σ(Eγ, θ); 62,64Ni, 66Zn(16O, 2nγ), E=42 MeV; measured DSA. 66,68Ge, 69As, 70Se, 74Kr, 80,82Sr deduced levels, J, π. 76,78Kr, 80Sr levels deduced B(E2), T1/2.
doi: 10.1007/BF01669462
1972NO14 Z.Phys. 256, 243 (1972) The Decay of 78Rb and the Level Scheme of 78Kr RADIOACTIVITY 78Rb; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 78Kr deduced levels, J, π. NUCLEAR REACTIONS 64Ni(16O, 2nγ), E=42 MeV; 64Zn(16O, 2p), E=47 MeV; measured Iγ, σ(θ(γ)), γγ-coin. 78Kr deduced levels, J, π.
doi: 10.1007/BF01392097
1970NO03 Phys.Lett. 33B, 294 (1970) E.Nolte, W.Kutschera, Y.Shida, H.Morinaga Neutron Deficient Even-Even Isotopes of Kr, Se, Ge and Pseudo SU3 Coupling RADIOACTIVITY 72Br; measured T1/2. NUCLEAR REACTIONS Ni(16O, Xγ), E=24-57 MeV; 58Ni(12C, Xγ), E=36 MeV; measured σ(E;Eγ), (16O)(γ)-, (12C)(γ)-delay. 68Ge, 72,74Se, 74,76,78Kr deduced levels.
doi: 10.1016/0370-2693(70)90273-X
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