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NSR database version of April 11, 2024.

Search: Author = J.Dubach

Found 35 matches.

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1995CI02      Phys.Rev. C51, 2406 (1995)

A.Cichocki, J.Dubach, R.S.Hicks, G.A.Peterson, C.W.de Jager, H.de Vries, N.Kalantar-Nayestanaki, T.Sato

Electron Scattering from 10B

NUCLEAR REACTIONS 10B(e, e'), (e, e), E=223.53 MeV; measured spectra, longitudinal, transverse form factors. 10B levels deduced charge distribution, B(λ). Extensive model comparisons.

doi: 10.1103/PhysRevC.51.2406
Citations: PlumX Metrics

1993BA27      Phys.Rev. C48, 735 (1993)

H.Baghaei, J.Dubach, M.B.Frodyma, R.S.Hicks, R.A.Miskimen, G.A.Peterson, S.H.Rokni, A.Hotta, T.Suzuki

Transverse Form Factors of 117Sn

NUCLEAR REACTIONS 117Sn(e, e'), (e, e), E=100-221 MeV; measured σ(E, θ). 117Sn deduced transverse form factors. Enriched target. Comparison with shell model, core polarization calculations.

doi: 10.1103/PhysRevC.48.735
Citations: PlumX Metrics

1990LI21      Phys.Lett. 244B, 173 (1990)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

Multi-Nucleon Degrees of Freedom in Inelastic Form Factors of 7Li

NUCLEAR REACTIONS 7Li(e, e'), E=80-680 MeV; measured electromagnetic form factors; deduced multi-nucleon degrees of freedom role.

doi: 10.1016/0370-2693(90)90050-G
Citations: PlumX Metrics

1989DO15      Nucl.Phys. A503, 589 (1989)

T.W.Donnelly, J.Dubach, I.Sick

Isospin Dependences in Parity-Violating Electron Scattering

NUCLEAR REACTIONS 28Si(e, e), E not given; calculated form factor. Parity violating electron scattering.

NUCLEAR STRUCTURE 12C; calculated level T, parity violating asymmetry related isospin mixing effects. Parity violating electron scattering.

doi: 10.1016/0375-9474(89)90432-6
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1989LI09      Phys.Lett. 219B, 394 (1989)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

High Momentum Transfer Longitudinal and Transverse Form Factors of the 7Li Ground-State Doublet

NUCLEAR REACTIONS 7,6Li(e, e), (e, e'), E=80-680 MeV; measured longitudinal, transverse form factors.

doi: 10.1016/0370-2693(89)91083-6
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1989PL05      Phys.Rev. C40, 1861 (1989)

M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer

180° Electron Scattering from 14C

NUCLEAR REACTIONS 14C(e, e'), E=82-269 MeV; measured σ(E(e'), θ); deduced 14C, 14B Coulomb energy difference. 14C levels deduced structure coefficients, form factors, IAS.

doi: 10.1103/PhysRevC.40.1861
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1989SI18      Phys.Rev. C40, 2218 (1989)

R.R.Silbar, W.M.Kloet, L.S.Kisslinger, J.Dubach

Pion-Exchange Contribution to the Parity-Violating Asymmetry in p(pol)p Scattering

NUCLEAR REACTIONS 1H(polarized p, p), E=200-1000 MeV; calculated parity violating asymmetry vs E; deduced pion-exchange contribution.

doi: 10.1103/PhysRevC.40.2218
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1988DO09      Phys.Rev. C37, 2320 (1988)

T.W.Donnelly, J.Dubach, I.Sick

Determination of the Neutron Electric Form Factor from 1H(e(pol), e)1H

NUCLEAR REACTIONS 1H(polarized e, e'), E not given; calculated σ(θ), asymmetry; deduced neutron electric form factor estimate possibility.

doi: 10.1103/PhysRevC.37.2320
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1988HI02      Phys.Rev.Lett. 60, 905 (1988)

R.S.Hicks, J.Button-Shafer, B.Debebe, J.Dubach, A.Hotta, R.L.Huffman, R.A.Lindgren, G.A.Peterson, R.P.Singhal, C.W.de Jager

Determination of Single-Nucleon Wave Functions by Transverse Electron Scattering

NUCLEAR REACTIONS 10,11B(e, e), 10B(e, e'), E=203-416 MeV; measured form factors. 10B deduced 1p3/2 wave function radial shape.

doi: 10.1103/PhysRevLett.60.905
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1988HO11      Phys.Rev. C38, 1547 (1988)

A.Hotta, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, P.J.Ryan, R.P.Singhal, D.Halderson

Electroexcitation of 4He in the Near Continuum

NUCLEAR REACTIONS 4He(e, e'), E=130, 200 MeV; measured σ(E(e'), θ(e')). Shell model in continuum interpretation.

doi: 10.1103/PhysRevC.38.1547
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1987DO12      Nucl.Phys. A474, 307 (1987)

T.W.Donnelly, A.S.Raskin, J.Dubach

Prospects for using the (e, e'γ) Reaction to Explore Nuclear Structure

NUCLEAR REACTIONS 12C, 15N(e, e'γ), E not given; calculated γ(θ); deduced structure information.

doi: 10.1016/0375-9474(87)90620-8
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1987DU03      Nucl.Phys. A466, 573 (1987)

J.Dubach, W.M.Kloet, R.R.Silbar

NN → NNπ at Intermediate Energies: Predictions of a unitary model

NUCLEAR REACTIONS 1H(p, pπ+), (p, pπ0), (n, pπ-), (p, pX), (p, nX), E=800 MeV; calculated σ(Ep, θp, θπ), spin observables, σ(Ep, θp), σ(En, θn). Unitary model.

doi: 10.1016/0375-9474(87)90458-1
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1987HU01      Phys.Rev. C35, 1 (1987)

R.L.Huffman, J.Dubach, R.S.Hicks, M.A.Plum

Phenomenological Wave Functions for the Ground and 2.313 MeV States in 14N

NUCLEAR REACTIONS 14N(e, e), (e, e'), E=80-372.6 MeV; measured σ(E, θ). 14N level deduced form factors, wave functions; 14N(p, p'), (γ, π+), 14C(p, n), E=25-200 MeV; calculated σ(θ). 14N level deduced spectroscopic factors. Solid boron nitride, natural N2 gas targets. DWBA analysis.

doi: 10.1103/PhysRevC.35.1
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1987RI06      Phys.Lett. 197B, 23 (1987)

P.J.Riley, M.Bachman, C.L.Hollas, K.H.McNaughton, S.-W.Xu, B.E.Bonner, O.B.Van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet

Polarization Observables for the Reaction pp → ppπ0 at 800 MeV

NUCLEAR REACTIONS 1H(polarized p, pπ0), E=647, 733, 800 MeV; measured induced polarization, analyzing power, Wolfenstein parameters. Orthogonal beam polarization.

doi: 10.1016/0370-2693(87)90334-0
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1986DU01      Phys.Rev. C33, 373 (1986)

J.Dubach, W.M.Kloet, R.R.Silbar

Nucleon-Nucleon Final-State Interactions in NN → NNπ

NUCLEAR REACTIONS 1H(p, pπ+), (polarized p, pπ+), E=800 MeV; calculated σ(θp, θ(π)), spin observables, spin-spin correlation parameter vs proton momentum.

doi: 10.1103/PhysRevC.33.373
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1986DU08      Phys.Rev. C34, 944 (1986)

J.Dubach, W.M.Kloet, R.R.Silbar, J.A.Tjon, E.van Faassen

Model Dependence of Unitary Isobar Model Treatments of NN → NN(π) at Intermediate Energies

NUCLEAR REACTIONS 1H(polarized p, π+), E=800 MeV; calculated σ(θp, θ(π)) vs proton momentum, spin observables vs θ; deduced dibaryon resonance role. Unitary isobar model.

doi: 10.1103/PhysRevC.34.944
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1985HO16      Phys.Rev.Lett. 55, 29 (1985)

C.L.Hollas, K.H.McNaughton, P.J.Riley, Shen-wu Xu, B.E.Bonner, O.B.van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet

Wolfenstein Polarization Observables for the Reaction p(pol)p → p(pol)πn at 800 MeV

NUCLEAR REACTIONS 1H(polarized p, pπ+), E=650, 733, 800 MeV; measured Wolfenstein polarization parameters, induced polarization, σ(θ1, θ2) vs proton momentum.

doi: 10.1103/PhysRevLett.55.29
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1985TO21      Phys.Rev. C32, 2075 (1985)

E.L.Tomusiak, M.Kimura, J.L.Friar, B.F.Gibson, G.L.Payne, J.Dubach

Trinucleon Magnetic Moments

NUCLEAR STRUCTURE 3H, 3He; calculated μ, magnetic form factors; deduced dominant charge exchange effects. Various potential models, configuration space Faddeev equations.

doi: 10.1103/PhysRevC.32.2075
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1984HU07      Phys.Lett. 139B, 249 (1984)

R.L.Huffman, R.S.Hicks, J.Dubach, B.Parker, M.A.Plum, G.Lahm, R.Neuhausen, J.C.Bergstrom

Comparison of Isoscalar and Isovector (e, e') M1 Form Factors at High Momentum Transfer

NUCLEAR REACTIONS 14N(e, e), (e, e'), E not given; measured M1 form factors. 14N deduced isoscalar, isovector transition differences. Shell model comparison.

doi: 10.1016/0370-2693(84)91073-6
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1984PL02      Phys.Lett. 137B, 15 (1984)

M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer

Isoscalar and Isovector M4 Spin Transitions in 14C

NUCLEAR REACTIONS 14C(e, e'), E=100-300 MeV; measured σ(E(e')), transverse form factor. 14C levels deduced M4 spin transition density isoscalar, isovector amplitudes, σ(π+)/σ(π-). Pion data input.

doi: 10.1016/0370-2693(84)91096-7
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1983BH07      Phys.Rev. C28, 2071 (1983)

T.S.Bhatia, J.G.J.Boissevain, J.J.Jarmer, R.R.Silbar, J.E.Simmons, G.Glass, J.C.Hiebert, R.A.Kenefick, L.C.Northcliffe, W.B.Tippens, W.M.Kloet, J.Dubach

Analyzing Powers and Spin Correlations A(NN) and A(LL) for pp → npπ+ at 650 and 800 MeV

NUCLEAR REACTIONS 1H(polarized p, pπ), E=800, 650 MeV; measured analyzing power, spin correlation vs proton momentum. Born approximation calculations.

doi: 10.1103/PhysRevC.28.2071
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1983GA09      Phys.Rev. C28, 294 (1983)

M.M.Gazzaly, N.M.Hintz, M.A.Franey, J.Dubach, W.C.Haxton

Neutron and Proton Transition Matrix Elements for 90Zr from a Microscopic Analysis of 0.8 GeV Proton Inelastic Scattering

NUCLEAR REACTIONS 90Zr(p, p'), E=0.8 GeV; measured absolute σ(θ). 90Zr levels deduced core to total deformation parameter ratio, enhancement factors, neutron, proton matrix element ratios. DWIA, shell model transition densities.

doi: 10.1103/PhysRevC.28.294
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1294.

1983LI07      Phys.Lett. 121B, 377 (1983)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

The Low Lying Levels of 7Li Studied by Electron Scattering

NUCLEAR REACTIONS 7Li(e, e), (e, e'), E=80-300 MeV; measured M1, M3, E2 form factors. Shell model interpretation.

doi: 10.1016/0370-2693(83)91181-4
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1983RY03      Phys.Rev. C21, 2575 (1983)

P.J.Ryan, R.S.Hicks, A.Hotta, J.Dubach, G.A.Peterson, D.V.Webb

Electroexcitation of Even-Parity States in 27Al

NUCLEAR REACTIONS 27Al(e, e'), E=60-340 MeV; measured σ(E, θ), σ(E(e')). 27Al deduced levels, tentative J, π, form factors, effective charges.

doi: 10.1103/PhysRevC.27.2515
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1983SI11      Phys.Rev. C28, 513 (1983)

R.P.Singhal, J.Dubach, R.S.Hicks, R.A.Lindgren, B.Parker, G.A.Peterson

Electron Scattering at 180° from the ' Single-Hole ' States in 15N

NUCLEAR REACTIONS 15N(e, e), (e, e'), E=70-327 MeV; measured σ(E, θ). 15N levels deduced form factors. Shell, core polarization models comparison.

doi: 10.1103/PhysRevC.28.513
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1982HI07      Phys.Rev. C26, 339 (1982)

R.S.Hicks, J.Dubach, R.A.Lindgren, B.Parker, G.A.Peterson

Elastic Magnetic Scattering of Electrons from 13C

NUCLEAR REACTIONS 13C(e, e), E=80-338 MeV; measured σ(E, θ). 13C deduced M1 form factor. Shell model.

doi: 10.1103/PhysRevC.26.339
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1981DU17      Phys.Lett. 106B, 29 (1981)

J.Dubach, W.M.Kloet, A.Cass, R.R.Silbar

Exclusive Spin-Dependent Pion Production in Medium-Energy Nucleon-Nucleon Collisions: The role of unitarity

NUCLEAR REACTIONS 1H(polarized p, π+p), E=800 MeV; calculated asymmetry vs θp, θ(π). Unitarity, relativistic model dynamics.

doi: 10.1016/0370-2693(81)91073-X
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1980DU08      Nucl.Phys. A340, 271 (1980)


Exchange Current Effects in Magnetic Electron Scattering from 49Ti, 51V, 59Co, 87Sr, and 92Nb

NUCLEAR REACTIONS 49Ti, 51V, 59Co, 87Sr, 92Nb(e, e), E not given; calculated magnetic form factors; deduced exchange current contributions to neutron, proton radii. Density dependent Hartree-Fock-Bogoliubov calculations.

doi: 10.1016/0375-9474(80)90275-4
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1979DU01      Phys.Lett. 81B, 124 (1979)


Exchange Currents and the Radial Distribution of Valence Nucleons as Determined from Elastic Electron Scattering

NUCLEAR STRUCTURE 51V; calculated squared magnetic form factor at high momentum transfer in electron scattering. Density dependent interaction, meson exchange currents, Hartree-Fock-Bogoliubov formalism.

doi: 10.1016/0370-2693(79)90503-3
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1979DU06      Phys.Rev. C20, 725 (1979)

J.F.Dubach, E.J.Moniz, G.D.Nixon

Dynamical Polarization in Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 48Ti, 104Ru, 110Pd, 112Cd, 150Sm; pionic atoms; measured X-rays.

NUCLEAR REACTIONS 48Ti, 104Ru, 110Pd, 112Cd, 150Sm(π-, X), E ≈ 0; measured dynamic nuclear polarization; deduced interference between nuclear, atomic transition.

doi: 10.1103/PhysRevC.20.725
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1979FL08      Phys.Rev.Lett. 43, 1922 (1979)

J.B.Flanz, R.S.Hicks, R.A.Lindgren, G.A.Peterson, J.Dubach, W.C.Haxton

Electron Scattering, Isospin Mixing, and the Structure of the 12.71- and 15.11-MeV Levels in 12C

NUCLEAR REACTIONS 12C(e, e'), E not given; measured form factors at θ=180°; deduced charge-dependent isospin-mixing matrix element. 12C levels deduced isospin mixing, structure.

doi: 10.1103/PhysRevLett.43.1922
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1978DU12      Phys.Rev.Lett. 41, 1453 (1978)

J.Dubach, W.C.Haxton

Nuclear Structure and (e, e') Reactions: The Significance of High-Momentum-Transfer Data and Meson-Exchange Currents

NUCLEAR STRUCTURE 12C; calculated inelastic electron scattering form factor.

doi: 10.1103/PhysRevLett.41.1453
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1976DU05      Nucl.Phys. A271, 279 (1976)

J.Dubach, J.H.Koch, T.W.Donnelly

Exchange Currents in Electron Scattering from Light Nuclei

NUCLEAR REACTIONS 3He, 6,7Li, 9Be, 10B(e, e'); calculated meson exchange currents.

doi: 10.1016/0375-9474(76)90246-3
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1975DO10      Nucl.Phys. A251, 353 (1975)

T.W.Donnelly, J.Dubach, W.C.Haxton

Semi-Leptonic Weak and Electromagnetic Interactions in the Goldhaber-Teller Model

NUCLEAR STRUCTURE 12C, 16O; T=1 giant resonances calculated β+, β- decay rates.

NUCLEAR REACTIONS 16O(e, e); calculated form factors. 16O(ν, e), (ν-bar, e+), E=250 MeV; 40Ca(ν, e), (ν-bar, e+), E=500 MeV; calculated σ. 12C, 16O, 28Si, 40Ca(μ-, X); calculated muon capture rates.

doi: 10.1016/0375-9474(75)90535-7
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1974DO14      Nucl.Phys. A232, 355 (1974)

T.W.Donnelly, J.Dubach, J.D.Walecka

Heavy-Ion Scattering at Intermediate and High Energies

NUCLEAR REACTIONS 60Ni(16O, 16O), E(cm)=150, 225, 500, 1000 MeV; calculated σ(θ).

doi: 10.1016/0375-9474(74)90626-5
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Note: The following list of authors and aliases matches the search parameter J.Dubach: , J.F.DUBACH