NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = D.Weber Found 23 matches. 2014FE09 Phys.Rev. C 90, 064005 (2014) Nucleon-nucleon potentials in phase-space representation
doi: 10.1103/PhysRevC.90.064005
2014WE01 Phys.Rev. C 89, 034002 (2014) D.Weber, H.Feldmeier, H.Hergert, T.Neff From nucleon-nucleon interaction matrix elements in momentum space to an operator representation
doi: 10.1103/PhysRevC.89.034002
1991KR05 Phys.Rev. A43, 4837 (1991) Doppler-Free Two-Photon Spectroscopy in Eu: Fine structure, hyperfine structures, and isotope shifts of odd levels between 34400 cm-1 and 36700 cm-1 NUCLEAR MOMENTS 151,153Eu; measured hfs, isotope shifts. Doppler-free two-photon spectroscopy.
doi: 10.1103/PhysRevA.43.4837
1991KR17 Phys.Rev. A44, 5737 (1991) H.-D.Kronfeldt, D.-J.Weber, J.Dembczynski, E.Stachowska J Off-Diagonal Effects in the Hyperfine-Structure Splitting in the Eu I Term e6D of 4f76s6d NUCLEAR MOMENTS 151,153Eu; measured hfs; deduced hfs anomaly mean value. Model calculations.
doi: 10.1103/PhysRevA.44.5737
1990KR02 J.Phys.(London) B23, 1107 (1990) H.-D.Kronfeldt, G.Klemz, D.-J.Weber On the J-Dependence of the Isotope Shift in the Ground Term of Gd I NUCLEAR MOMENTS 154,155,156,157,158,160Gd; measured isotope shift; deduced rms charge radii differences. 155Gd; measured hfs; deduced hyperfine constants. High resolution laser induced resonance fluorescence spectroscopy.
doi: 10.1088/0953-4075/23/7/008
1989SE11 Z.Phys. D14, 99 (1989) P.Seifert, D.-J.Weber, H.-D.Kronfeldt, R.Winkler Parametric Analysis of the Isotope Shift and Hyperfinestructure in the Eu I Configuration 4f7 5d6s NUCLEAR MOMENTS 153,151Eu; measured hfs, isotope shift; deduced hyperfine interaction parameters. Doppler-reduced intermodulated optogalvanic saturation laser spectroscopy.
doi: 10.1007/BF01399029
1988KR15 Z.Phys. D10, 103 (1988) H.-D.Kronfeldt, G.Klemz, D.-J.Weber J-Dependence of the Isotope Shift in Gd I 4f75d6s2(a9D) NUCLEAR MOMENTS 158,157,156,155,154Gd; measured isotope shift relative to 160Gd; deduced rms charge radii.
doi: 10.1007/BF01425586
1985FI05 Nucl.Phys. A441, 57 (1985) J.E.Finck, G.M.Crawley, D.Weber, P.A.Smith The 206,204Pb(p, α)203,201Tl Reactions at 35 MeV NUCLEAR REACTIONS 204,206Pb(p, α), E=35 MeV; measured σ(Eα), σ(θ). 201,203Tl deduced levels, J, π. Cluster model, DWBA analysis.
doi: 10.1016/0375-9474(85)90167-8
1983GA07 Nucl.Phys. A398, 19 (1983) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Neutron-Hole Strength Distributions in Heavy Nuclei (II). The 144,148,152Sm(3He, α)143,147,151Sm and the 144,148,150,152,154Sm(p, d)143,147,149,151,153Sm Reactions NUCLEAR REACTIONS 144,148,152Sm(3He, α), E=70 MeV; measured σ(Eα, θ); 144,148,150,152,154Sm(p, d), E=42 MeV; measured σ(Ed, θ). 143,147,149,151,153Sm deduced levels, L, J, π, C2S. Enriched target, magnetic spectrometer. Zero-range, finite-range DWBA calculations, inner-shells analysis. Comparison with the quasiparticle phonon, Nilsson models.
doi: 10.1016/0375-9474(83)90646-2
1982CR01 Phys.Lett. 109B, 8 (1982) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Pairing Model Predictions for (p, t) Experiments on the Cadmium Isotopes NUCLEAR REACTIONS 110,112,114,116Cd(p, t), E=42 MeV; measured σ(Et). 106Cd(p, t), E=42 MeV; measured σ(Et), Q. 110,112,114,116,106Cd deduced two-particle pickup from deep orbits. 104Cd deduced mass excess. Split-pole spectrograph, position sensitive proportional counter. Pairing model.
doi: 10.1016/0370-2693(82)90450-6
1982GA18 Nucl.Phys. A381, 173 (1982) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Neutron-Hole Strength Distributions in Heavy Nuclei (I): The reactions 124,130Te(3He, α)123,129Te and 122,124,130Te(p, d)121,123,129Te NUCLEAR REACTIONS 124,130Te(3He, α), E=70 MeV; measured σ(Eα, θ). 122,124,130Te(p, d), E=42 MeV; measured σ(θ). 121,123,129Te deduced levels, L, J, π, C2S. Enriched targets, magnetic spectrometer. DWBA, inner-shell analysis.
doi: 10.1016/0375-9474(82)90139-7
1982ZW02 Nucl.Phys. A389, 301 (1982) B.Zwieglinski, W.Benenson, G.M.Crawley, S.Gales, D.Weber Study of 11B at High Excitations with the 9Be(3He, p)11B and 9Be(α, d)11B Reactions NUCLEAR REACTIONS 9Be(3He, p), E=38 MeV; 9Be(α, d), E=48 MeV; measured σ(E(p), θ), σ(E(d)). 11B deduced levels, widths, isospin purity, L, normalization factors. DWBA analysis, shell-model form factors. Natural targets.
doi: 10.1016/0375-9474(82)90521-8
1981CR01 Phys.Rev. C23, 589 (1981) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Hole States in the Tin Isotopes Observed by the (p, t) Reaction NUCLEAR REACTIONS 112,116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ); 117,119Sn(p, d), E=42 MeV; measured σ(Ed). 110,114,116,118,120,122Sn deduced broad resonances, Γ. DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.23.589
1980CR02 Phys.Rev. C22, 316 (1980) G.M.Crawley, S.Gales, D.Weber, B.Zwieglinski, W.Benenson, D.Friesel, A.Bacher, B.M.Spicer Deep Hole States Observed in (p, t) Reactions NUCLEAR REACTIONS 120,122,124Sn(p, t), E=89 MeV; measured σ(Et, θ). 118,120,122Sn deduced levels, Γ. DWBA, enriched targets.
doi: 10.1103/PhysRevC.22.316
1980IW02 Phys.Rev. C22, 456 (1980) Y.Iwasaki, A.Galonsky, D.J.Weber 48Ca(d, n)49Sc Reaction at Ed=20 MeV; Proton Single-Particle States in 49Sc NUCLEAR REACTIONS 48Ca(d, n), E=20 MeV; measured σ(θ). 49Sc levels deduced C2S. DWBA analysis.
doi: 10.1103/PhysRevC.22.456
1979WE02 Nucl.Phys. A313, 385 (1979) D.J.Weber, G.M.Crawley, W.Benenson, E.Kashy, H.Nann Study of 60Zn and 61Zn NUCLEAR REACTIONS 58Ni(12C, 10Be), 58Ni(12C, 9Be), E=77 MeV; measured σ(E(10Be), θ), σ(E(9Be), θ). 60Zn, 61Zn deduced levels. 64Zn(3He, 6He), E=70 MeV; measured σ; deduced Q. 61Zn deduced mass excess, levels. Enriched targets. Atomic mass 61Zn.
doi: 10.1016/0375-9474(79)90508-6
1978GA09 Phys.Rev.Lett. 41, 292 (1978) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Observation of the T > = 45/2 Components of Deep Hole States in 207Pb via the (3He, α) Reaction at 70 MeV NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(Eα, θ). 207Pb deduced levels, S.
doi: 10.1103/PhysRevLett.41.292
1978GA23 Phys.Rev. C18, 2475 (1978) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Inner Hole States in 207Pb via the 208Pb(3He, α)207Pb Reaction at 70 MeV NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(E, θ). 207Pb deduced levels, L, J, π, C2S, inner shell S. Enriched target, magnetic spectrometer.
doi: 10.1103/PhysRevC.18.2475
1978SM06 Phys.Rev. C18, 2486 (1978) P.A.Smith, G.M.Crawley, G.G.Markham, D.Weber 208Pb(p, α)205Tl Reaction NUCLEAR REACTIONS 208Pb(p, α), E=35 MeV; measured σ(θ). 205Tl deduced levels, J, π. Enriched target. Cluster model DWBA analysis. Compared with weak coupling model.
doi: 10.1103/PhysRevC.18.2486
1977CR04 Phys.Rev.Lett. 39, 1451 (1977) G.M.Crawley, W.Benenson, D.Weber, B.Zwieglinski Observation of Hole States at High Excitation in (p, t) Reactions NUCLEAR REACTIONS 106Cd, 104Pd, 116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ). 114,116,118,120,122Sn deduced enhancements, widths.
doi: 10.1103/PhysRevLett.39.1451
1977KU04 Phys.Rev.Lett. 38, 817 (1977) S.Kubono, D.Dehnhard, D.A.Lewis, T.K.Li, J.L.Artz, D.J.Weber, P.J.Ellis, A.Dudek-Ellis j Dependence of the (19F, 16O) Reaction and Spin-Orbit Forces in the Heavy-Ion Optical Potential NUCLEAR REACTIONS 28,30Si(19F, 16O), E=60 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.38.817
1976DE03 Phys.Rev. C13, 164 (1976) D.Dehnhard, J.L.Artz, D.J.Weber, V.Shkolnik, R.M.DeVries 29,30Si(16O, 15N) Proton Stripping Reaction at 60 MeV NUCLEAR REACTIONS 29,30Si(16O, 15N), E=60 MeV; measured σ(E(15N), θ). 30,31P levels deduced S.
doi: 10.1103/PhysRevC.13.164
1975WE14 Nucl.Instrum.Methods 124, 317 (1975) D.J.Weber, N.M.Hintz, D.Dehnhard Equilibrium Charge-State Distributions for 16O Ions at 20-65 MeV NUCLEAR REACTIONS Au(16O, 16O), E=20-65 MeV; measured charge-state distribution.
doi: 10.1016/0029-554X(75)90578-9
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