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Search: Author = J.W.Lightbody

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1994RE04      Phys.Rev. C49, 1263 (1994)

G.A.Retzlaff, H.S.Caplan, E.L.Hallin, D.M.Skopik, D.Beck, K.I.Blomqvist, G.Dodson, K.Dow, M.Farkhondeh, J.Flanz, S.Kowalski, W.W.Sapp, C.P.Sargent, D.Tieger, W.Turchinetz, C.F.Williamson, W.Dodge, X.K.Maruyama, J.W.Lightbody, Jr., R.Goloskie, J.McCarthy, T.S.Ueng, R.R.Whitney, B.Quinn, S.Dytman, K.Von Reden, R.Schiavilla, J.A.Tjon

Threshold Electrodisintegration in the A = 3 System

NUCLEAR REACTIONS 3He, 3H(e, e'X), E not given; measured double differential σ; deduced, analyzed longitudinal, transverse response functions. Models comparison.

doi: 10.1103/PhysRevC.49.1263
Citations: PlumX Metrics


1993SA03      Phys.Rev. C47, 459 (1993)

A.J.Sarty, K.G.R.Doss, G.Feldman, E.L.Hallin, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, H.R.Weller, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, C.C.Chang

Measurement of the Reaction 3He(γ, pp)n and Its Relation to Three-Body Forces

NUCLEAR REACTIONS 3He(γ, 2p), E=90-250 MeV bremsstrahlung; measured σ(θn, θp) vs neutron momentum; deduced two-pion-exchange, three-body absorption mechanisms role.

doi: 10.1103/PhysRevC.47.459
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1991MC12      Nucl.Instrum.Methods Phys.Res. B56/57, 496 (1991)

M.McCord, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.W.Lightbody, X.K.Maruyama, P.A.Treado

Preliminary Results of a New Determination of the rms Charge Radius of the Proton

NUCLEAR REACTIONS 1H(e, e), E=31-105 MeV; measured absolute, relative σ(θ). 1H deduced rms charge radius. High pressure, flowing gas target cell filled with H2, CH4 gas.

doi: 10.1016/0168-583X(91)96079-Z
Citations: PlumX Metrics


1990HA09      Phys.Rev. C41, 1619 (1990)

K.Hansen, J.-O.Adler, K.I.Blomqvist, D.Nilsson, A.Sandell, B.Schroder, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, J.R.Calarco, J.P.Connelly, F.W.Hersman, W.Kim, M.Leuschner

Electrofission in the Quasifree and Delta Regions

NUCLEAR REACTIONS 233,238U(e, e'F), E=720-830 MeV; measured σ(E, θ), fission probability; deduced mean nuclear excitation energy. Parallel plate avalanche detector.

doi: 10.1103/PhysRevC.41.1619
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1987OC01      Phys.Rev. C35, 1063 (1987)

J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn, J.H.Koch, N.Ohtsuka

Electromagnetic Excitation of the Delta Resonance in Nuclei

NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'X), E=537, 730 MeV; measured inclusive σ(E(e'), θ(e')); deduced quasifree peak positions, widths, average separation energies. Dispersion matched energy loss spectrometer. Model calculations.

doi: 10.1103/PhysRevC.35.1063
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1984BE46      Phys.Rev. C30, 1403 (1984)

D.H.Beck, S.B.Kowalski, M.E.Schulze, W.E.Turchinetz, J.W.Lightbody, Jr., X.K.Maruyama, W.J.Stapor, H.S.Caplan, G.A.Retzlaff, D.M.Skopik, R.Goloskie

Tritium Form Factors at Low q

NUCLEAR REACTIONS 3H(e, e), E=100 MeV; measured charge, magnetic form factors, σ(θ); deduced charge and magnetic radii. 3He, 3H deduced binding energy difference Coulomb contribution.

doi: 10.1103/PhysRevC.30.1403
Citations: PlumX Metrics


1984BU06      Phys.Rev. C29, 713 (1984)

P.E.Burt, L.W.Fagg, H.Crannell, D.I.Sober, W.Stapor, J.T.O'Brien, J.W.Lightbody, X.K.Maruyama, R.A.Lindgren, C.P.Sargent

Low Multipolarity Magnetic Transitions in 32S Excited by Electron Scattering

NUCLEAR REACTIONS 32S(e, e'), E=34-74 MeV; measured σ(θ). 32S levels deduced transition form factors, multipolarity, B(M1), Γ.

doi: 10.1103/PhysRevC.29.713
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1984OC01      Phys.Rev.Lett. 53, 1627 (1984)

J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn

Electron Scattering in the Excitation Region of the Delta Resonance on Nuclei with A = 1 to 16

NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'), E=730 MeV; measured σ vs energy loss; deduced (σ/A) in the quasifree, isobar resonance regions.

doi: 10.1103/PhysRevLett.53.1627
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1983LI02      Phys.Rev. C27, 113 (1983)

J.W.Lightbody, Jr., J.B.Bellicard, J.M.Cavedon, B.Frois, D.Goutte, M.Huet, Ph.Leconte, A.Nakada, Phan Xuan Ho, S.K.Platchkov, S.Turck-Chieze, C.W.de Jager, J.J.Lapikas, P.K.A.de Witt Huberts

Elastic and Inelastic Electron Scattering from 50,52,54Cr

NUCLEAR REACTIONS 50,52,54Cr(e, e), (e, e'), E=30-400 MeV; measured σ(E, θ). 50,52,54Cr deduced ground state charge distributions, inelastic form factors, rms radii, B(E2) estimates. Muonic atom data input, HFB, shell model comparisons.

doi: 10.1103/PhysRevC.27.113
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1983OC01      Phys.Rev. C27, 2492 (1983)

J.S.O'Connell, E.Hayward, J.W.Lightbody, Jr., X.K.Maruyama, P.Bosted, K.I.Blomqvist, G.Franklin, J-O.Adler, K.Hansen, B.Schroder

Total Nuclear Inelastic Electron Scattering Cross Sections Compared to Sum Rule Calculations

NUCLEAR REACTIONS 9Be, 12C, 27Al, 51V, 90Zr, 181Ta(e, e'), E=200-350 MeV; measured σ(θ, E(e')); deduced longitudinal response function.

doi: 10.1103/PhysRevC.27.2492
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1982BU05      Phys.Rev. C25, 2805 (1982)

P.E.Burt, L.W.Fagg, H.Crannell, D.I.Sober, W.Stapor, J.T.O'Brien, X.K.Maruyama, J.W.Lightbody, R.A.Lindgren

Electron Scattering Study of the 10.32 MeV Transition in 40Ca

NUCLEAR REACTIONS 40Ca(e, e'), E=31-65 MeV; measured σ(θ), σ(E(e')), form factors. 40Ca transition deduced B(M1), Γ.

doi: 10.1103/PhysRevC.25.2805
Citations: PlumX Metrics


1982ST17      Nucl.Instrum.Methods 203, 97 (1982)

W.J.Stapor, H.Crannell, J.W.Lightbody, Jr., X.K.Maruyama, T.O'Brien

A Flowing Gas Target System for Precision Electron Scattering Measurements

NUCLEAR REACTIONS 4He(e, e), E not given; measured not abstracted. 4He deduced ground state rms charge radius.

doi: 10.1016/0167-5087(82)90615-9
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1980CA07      Phys.Lett. 91B, 203 (1980)

L.S.Cardman, J.W.Lightbody, Jr., S.Penner, S.P.Fivozinsky, X.K.Maruyama, W.P.Trower, S.E.Williamson

The Charge Distribution of 12C

NUCLEAR REACTIONS 12C(e, e), E=25-115 MeV; measured absolute σ. 12C deduced ground-state charge distribution shape, rms charge radius.

doi: 10.1016/0370-2693(80)90431-1
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1979MA13      Phys.Rev. C19, 1624 (1979)

X.K.Maruyama, F.J.Kline, J.W.Lightbody, Jr., S.Penner, W.J.Briscoe, M.Lunnon, H.Crannell

Electroexcitation of 22Ne below E = 8.6 MeV

NUCLEAR REACTIONS 22Ne(e, e'), E=60-110 MeV; measured σ(E). 22Ne levels deduced J, π, B(λ). Enriched 22Ne target.

doi: 10.1103/PhysRevC.19.1624
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1978SZ02      Phys.Rev. C17, 435 (1978)

Z.M.Szalata, K.Itoh, G.A.Peterson, J.Flanz, S.P.Fivozinsky, F.J.Kline, J.W.Lightbody, Jr., X.E.Maruyama, S.Penner

Electroexcitation of 20Ne Giant Electric-Dipole and -Quadrupole Resonances

NUCLEAR REACTIONS 20Ne(e, e'), E=59.5-119.7 MeV; measured σ(E, θ). 20Ne giant resonance region deduced dipole, quadrupole strength.

doi: 10.1103/PhysRevC.17.435
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1977SZ02      Phys.Rev. C15, 1200 (1977)

Z.M.Szalata, J.M.Finn, J.Flanz, F.J.Kline, G.A.Peterson, J.W.Lightbody, Jr., X.K.Maruyama, S.Penner

Low-Momentum-Transfer Elastic Electron Scattering from 3He

NUCLEAR REACTIONS 3He(e, e), E=28.8-95.0 MeV; measured σ(E) at 75°. 3He deduced rms charge radius.

doi: 10.1103/PhysRevC.15.1200
Citations: PlumX Metrics


1976LI19      Phys.Rev. C14, 952 (1976)

J.W.Lightbody, Jr., S.Penner, S.P.Fivozinsky, P.L.Hallowell, H.Crannell

Electron Scattering from Vibrational Nuclei

NUCLEAR REACTIONS 52Cr, 110Pd, 114Cd, 116Sn(e, e), E=40-110 MeV; measured σ; deduced form factors. 110Pd, 114Cd, 116Sn deduced charge distribution parameters, B(λ), quadrupole moment.

doi: 10.1103/PhysRevC.14.952
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1976NE06      Nucl.Phys. A263, 249 (1976)

R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Electron Scattering Studies of Low-Lying Collective States of Even Zn Isotopes

NUCLEAR REACTIONS 64,66,68,70Zn(e, e'), E=40-112 MeV; measured σ(E, Ee', θ). 64,66,68,70Zn deduced B(E2), B(E3). Application of anharmonic vibrator model. Enriched targets.

doi: 10.1016/0375-9474(76)90171-8
Citations: PlumX Metrics


1975KA02      Phys.Rev. C11, 323 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electroexcitation of 11B

NUCLEAR REACTIONS 11B(e, e'), E=52.3-90 MeV; measured σ(E, Ee', θ). 11B giant resonances, levels deduced B(E2), B(M1), form factors.

doi: 10.1103/PhysRevC.11.323
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1975KA04      Phys.Rev.Lett. 34, 899 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, Z.M.Szalata, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Observation of Electric Monopole Strength in the Electrodisintegration Of 3He

NUCLEAR REACTIONS 3He(e, e'), E=60, 75, 90, 110, 120 MeV; 4He(e, e'), E=elastic peak to breakup threshold; measured σ. 3He deduced E0 excitation.

doi: 10.1103/PhysRevLett.34.899
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1975KA28      Phys.Rev. C12, 1118 (1975)

P.T.Kan, G.A.Peterson, D.V.Webb, Z.M.Szalata, J.S.O'Connell, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electrodisintegration of 3He

NUCLEAR REACTIONS 3He(e, e'), E=60-120 MeV; measured σ(E, Ee', θ). 3He deduced form factors, strength functions.

doi: 10.1103/PhysRevC.12.1118
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1974EN01      Phys.Rev. C9, 1705 (1974)

N.Ensslin, W.Bertozzi, S.Kowalski, C.P.Sargent, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electron Scattering from Excited States in 14N and 9Be

NUCLEAR REACTIONS 9Be, 14N(e, e'), E=117, 122 MeV; measured σ(Ee', θ). 9Be, 14N levels deduced form factors, B(EL), B(ML).

doi: 10.1103/PhysRevC.9.1705
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1974FI05      Phys.Rev. C9, 1533 (1974)

S.P.Fivozinsky, S.Penner, J.W.Lightbody, Jr., D.Blum

Electron Scattering from 88Sr and 89Y

NUCLEAR REACTIONS 88Sr, 89Y(e, e'), E=45-121 MeV; measured σ(E, θ), deduced form factors. 88Sr, 89Y levels deduced B(EL).

doi: 10.1103/PhysRevC.9.1533
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1974KL12      Nuovo Cim. 23A, 137 (1974)

F.J.Kline, H.Crannell, J.M.Finn, P.L.Hallowell, J.T.O'Brien, C.W.Werntz, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Search for the Lowest T = 2 State in 14C by Inelastic Electron Scattering

NUCLEAR REACTIONS 14C(e, e'), E=61, 81 MeV; measured σ(Ee'). 14C deduced upper limit for T=2 level.

doi: 10.1007/BF02748297
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1973CH16      Phys.Rev. C8, 23 (1973)

B.T.Chertok, C.Sheffield, J.W.Lightbody, Jr., S.Penner, D.Blum

Low-q2 Electron Scattering from the 15.109-MeV State of 12C and the Conserved-Vector-Current Test

NUCLEAR REACTIONS 12C(e, e'), E=150 MeV; measured σ(Ee', θ). 12C deduced B(M1), γ-width.

doi: 10.1103/PhysRevC.8.23
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1973HA13      Phys.Rev. C7, 1396 (1973)

P.L.Hallowell, W.Bertozzi, J.Heisenberg, S.Kowalski, X.Maruyama, C.P.Sargent, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electron Scattering from 19F and 40Ca

NUCLEAR REACTIONS 19F, 40Ca(e, e), (e, e'), E=120 MeV; measured σ(Ee), form factors; 19F, 40Ca deduced levels, charge radius, deformation parameters.

doi: 10.1103/PhysRevC.7.1396
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1973HE28      Proc.Int.Conf.Nuclear Physics, Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.629 (1973)

J.Heisenberg, W.Bertozzi, T.Cooper, N.Ensslin, P.L.Hallowell, S.Kowalski, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformed Charge Distributions of Some Rotational Heavy Nuclei

NUCLEAR REACTIONS 166Er, 176Yb, 232Th, 238U(e, e), E=35-110 MeV; measured σ(θ). 166Er, 176Yb, 232Th, 238U deduced charge distribution.


1972BE26      Phys.Rev.Lett. 28, 1711 (1972)

W.Bertozzi, T.Cooper, N.Ensslin, J.Heisenberg, S.Kowalski, M.Mills, W.Turchinetz, C.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformation Parameters of 152Sm by Electron Scattering

NUCLEAR REACTIONS 152Sm(e, e'), E=50-105 MeV; measured σ(Ee'). 152Sm deduced nuclear charge distribution, deformation parameters β(L).

doi: 10.1103/PhysRevLett.28.1711
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1972LI12      Phys.Lett. 38B, 475 (1972)

J.W.Lightbody, Jr.

Electron Scattering from One- and Two-Phonon Vibrational States

NUCLEAR REACTIONS 48Ti, 60Ni, 64,70Zn(e, e'), calculated form factors; deduced 1-, 2-phonon state admixtures.

doi: 10.1016/0370-2693(72)90520-5
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1972NE01      Phys.Rev. C5, 124 (1972)

R.Neuhausen, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Elastic Electron Scattering from Zn Isotopes

NUCLEAR REACTIONS 64,66,68,70Zn(e, e), E=61-120 MeV; measured σ(E;θ). 64,66,68,70Zn deduced rms radii, charge distribution parameters.

doi: 10.1103/PhysRevC.5.124
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1971BE51      Phys.Rev. C4, 1514 (1971)

J.C.Bergstrom, H.Crannell, F.J.Kline, J.T.O'Brien, J.W.Lightbody, Jr., S.P.Fivozinsky

Electroexcitation of the Giant Resonance of 13C

NUCLEAR REACTIONS 12,13C(e, e'), E=55, 77, 81, 106 MeV; measured σ(Ee'). 13C deduced resonances, level-width, giant resonance structure.

doi: 10.1103/PhysRevC.4.1514
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1971RO20      Nucl.Phys. A173, 124 (1971)

E.F.Romberg, N.S.Wall, D.Blum, J.W.Lightbody, Jr., S.Penner

Elastic Scattering of 60-120 MeV Electrons from 46,48,50Ti

NUCLEAR REACTIONS 46,48,50Ti(e, e), E=60-120 MeV; measured σ(E;θ=127.50°). 46,48,50Ti deduced relative charge density. Enriched targets.

doi: 10.1016/0375-9474(71)90751-2
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1970BE03      Phys.Rev.Lett. 24, 152 (1970)

J.C.Bergstrom, W.Bertozzi, S.Kowalski, X.K.Maruyama, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Electroexcitation of the Low-Lying States of O16

NUCLEAR REACTIONS 16O(e, e'), E=51-105 MeV; measured σ(E;E'); deduced inelastic form factors. 16O levels deduced deformation parameters.

doi: 10.1103/PhysRevLett.24.152
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1970LI02      Phys.Rev.Lett. 24, 274 (1970)

J.W.Lightbody, Jr., S.Penner

Electroexcitation of the C12 Giant Resonance

NUCLEAR REACTIONS 12C(e, e'), E=52-102 MeV; measured σ(E;Ee', θ); deduced form factors. 12C deduced reduced matrix elements for giant resonance region.

doi: 10.1103/PhysRevLett.24.274
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1970LI18      Phys.Lett. 33B, 129 (1970)

J.W.Lightbody, Jr.

Electron Scattering Sum Rule for 12C - Experiment and Theory

NUCLEAR REACTIONS 12C(e, e'), E=0-37 MeV; measured σ(Eγ, θ); deduced integrated σ, longitudinal, transverse form factors.

doi: 10.1016/0370-2693(70)90280-7
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