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NSR database version of April 11, 2024.

Search: Author = D.Weber

Found 23 matches.

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2014FE09      Phys.Rev. C 90, 064005 (2014)

H.Feldmeier, T.Neff, D.Weber

Nucleon-nucleon potentials in phase-space representation

doi: 10.1103/PhysRevC.90.064005
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1991KR05      Phys.Rev. A43, 4837 (1991)

H.-D.Kronfeldt, D.-J.Weber

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0068.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1349.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2082.


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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0666.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1349.


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
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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
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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
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter D.Weber: , D.J.WEBER