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NSR database version of April 11, 2024.

Search: Author = R.L.Huffman

Found 11 matches.

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1991MI13      Phys.Rev. C44, 1679 (1991)

R.A.Miskimen, H.Baghaei, P.E.Bosted, K.A.Dow, M.Frodyma, B.Frois, R.S.Hicks, A.Hotta, R.L.Huffman, K.S.Lee, J.Martino, G.A.Peterson, S.Platchkov, S.E.Rock, S.H.Rokni, W.Turchinetz, J.D.Zumbro

Elastic Magnetic Electron Scattering from 13C at Q2 = 1 (GeV)2/c2

NUCLEAR REACTIONS 13C(e, e), E not given; measured elastic σ upper limit. 13C deduced M1 form factor high-q enhancement. Shell model.

doi: 10.1103/PhysRevC.44.1679
Citations: PlumX Metrics

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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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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1987HI09      Phys.Rev. C36, 485 (1987)

R.S.Hicks, R.L.Huffman, R.A.Lindgren, G.A.Peterson, M.A.Plum, J.Button-Shafer

Electroexcitation of Discrete Levels in 12C and High Momentum Transfers

NUCLEAR REACTIONS 12,13C(e, e'), E=80-485 MeV; measured σ(E(e'), θ). 13,12C levels deduced transverse excitation form factors. Enriched 13C target. Shell model.

doi: 10.1103/PhysRevC.36.485
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1987HO25      Phys.Rev. C36, 2212 (1987)

A.Hotta, R.S.Hicks, R.L.Huffman, G.A.Peterson, R.J.Peterson, J.R.Shepard

Transverse Isoscalar Excitations in 24Mg by 180° Electron Scattering

NUCLEAR REACTIONS 24Mg(e, e'), E=80.1-200.5 MeV; measured σ(E(e')), θ=180°. 24Mg levels deduced form factors. Analysis including relativistic effects.

doi: 10.1103/PhysRevC.36.2212
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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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1986PA20      Phys.Rev. C34, 2354 (1986)

B.Parker, R.S.Hicks, A.Hotta, R.L.Huffman, G.A.Peterson, M.A.Plum, P.J.Ryan, R.P.Singhal

Transverse Quasielastic Electron Scattering from the Deuteron

NUCLEAR REACTIONS 2H(e, e'), E=220, 270, 320 MeV; measured σ(E(e'), θ); deduced isobar configuration role.

doi: 10.1103/PhysRevC.34.2354
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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
Citations: PlumX Metrics

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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1982HI10      Phys.Rev. C26, 920 (1982)

R.S.Hicks, R.L.Huffman, R.A.Lindgren, B.Parker, G.A.Peterson, S.Raman, C.P.Sargent

Inelastic Electron Scattering from 208Pb at 180°

NUCLEAR REACTIONS 208Pb(e, e'), E=40.5, 50.4, 60.3, 75.2 MeV; measured σ(θ=180°). 208Pb deduced levels, transverse form factors. Enriched target, magnetic spectrometer.

doi: 10.1103/PhysRevC.26.920
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