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Search: Author = L.W.Fagg

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2002HO02      Phys.Rev. C65, 024311 (2002)

F.Hofmann, P.von Neumann-Cosel, F.Neumeyer, C.Rangacharyulu, B.Reitz, A.Richter, G.Schrieder, D.I.Sober, L.W.Fagg, B.A.Brown

Magnetic Dipole Transitions in 32S from Electron Scattering at 180°

NUCLEAR REACTIONS 32S(e, e'), E=42-82 MeV; measured electron spectra, σ(E, θ=180°). 32S deduced B(M1) strength distribution, form factors. Comparison with model predictions.

doi: 10.1103/PhysRevC.65.024311
Citations: PlumX Metrics


1997WE01      Phys.Rev. C55, 2773 (1997)

J.Wesseling, C.W.de Jager, L.Lapikas, H.de Vries, L.W.Fagg, M.N.Harakeh, N.Kalantar-Nayestanaki, R.A.Lindgren, E.Moya De Guerra, P.Sarriguren

2s1/2 Occupancies in 30Si, 31P, and 32S

NUCLEAR REACTIONS 30Si, 31P, 32S(e, e'), E=454.3 MeV; measured form factors; deduced charge distribution, level occupancies. Hartree-Fock calculation.

doi: 10.1103/PhysRevC.55.2773
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1995LU25      Nucl.Instrum.Methods Phys.Res. A366, 325 (1995)

C.Luttge, C.Hofmann, J.Horn, F.Neumeyer, A.Richter, G.Schrieder, E.Spamer, A.Stiller, D.I.Sober, S.K.Matthews, L.W.Fagg

Large-Aperture System for High-Resolution 180° Electron Scattering

NUCLEAR REACTIONS 12C(e, e), (e, e'), E=62 MeV; measured σ(θ). 28Si(e, e), E=62 MeV; measured spectra, θ=180°. High resolution 180° scattering large aperture system.

doi: 10.1016/0168-9002(95)00497-1
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1995PE01      Phys.Rev. C51, 1014 (1995)

M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, S.Raman

Low-Multipolarity Magnetic Transitions in 40Ca Excited by 180° Electron Scattering

NUCLEAR REACTIONS Ca, S(e, e'), E=28.4-56.5 MeV; measured σ(θ); deduced σ. 40Ca levels deduced B(λ). Model comparison.

doi: 10.1103/PhysRevC.51.1014
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1994FO03      Phys.Rev. C49, 1359 (1994)

C.W.Foltz, D.I.Sober, L.W.Fagg, H.D.Graf, A.Richter, E.Spamer, B.A.Brown

Electroexcitation of Low-Multipolarity Magnetic Transitions in 36Ar and 38Ar

NUCLEAR REACTIONS 36,38Ar(e, e'), E=35-65 MeV; measured σ(E, θ). 36,38Ar deduced transition multipolarities, B(λ). Pressurized gas target. Shell-model calculations.

doi: 10.1103/PhysRevC.49.1359
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1994PE08      Phys.Rev. C49, 3000 (1994)

M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, R.Lindgren, S.Raman

Low-Multipolarity Magnetic Transitions in 30Si, 32S, and 34S Studied by 180° Electron Scattering

NUCLEAR REACTIONS 30Si, 32,34S(e, e'), E=28.4-63.4 MeV; measured spectra, σ. 32,34S, 30Si deduced M1, M2 transition strength fragmentation features.

doi: 10.1103/PhysRevC.49.3000
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1992CO03      Phys.Lett. 277B, 383 (1992)

J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, S.Raman, J.R.Deininger, S.E.Williamson

Magnetic Dipole Strength in 46Ca Observed with 180° Electron Scattering

NUCLEAR REACTIONS 46Ca(e, e'), E=32.9-63.1 MeV; measured σ(E(e')), θ=180°; deduced σ(θ). 46Ca level deduced reduced transition rate, transition radius, B(λ).

doi: 10.1016/0370-2693(92)91798-E
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1992CO07      Phys.Rev. C45, 2494 (1992)

J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, J.R.Deininger, S.E.Williamson

Low-Momentum-Tranfer 180° Electron Scattering from the 3.68 MeV (3/2)- and the 3.85 MeV (5/2)+ States in 13C

NUCLEAR REACTIONS 13C(e, e'), E=28.5-56.5 MeV; measured σ(E(e')), σ(θ), transverse form factors. 13C levels deduced B(λ).

doi: 10.1103/PhysRevC.45.2494
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1992OB01      Nucl.Instrum.Methods Phys.Res. A312, 531 (1992)

J.T.O'Brien, D.I.Sober, L.W.Fagg, H.Crannell, M.Petraitis, J.P.Connelly, J.R.Deininger, S.E.Williamson

Design and Testing of Apparatus for 180° Electron Scattering at Low Momentum-Transfer

NUCLEAR REACTIONS 28Si, 13C(e, e), E=53 MeV; measured electron spectra, before, after focal plane corrections. Low momentum transfer, 180° electron scattering appartus design and testing.

doi: 10.1016/0168-9002(92)90201-E
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1992WE08      Nucl.Phys. A547, 519 (1992)

J.Wesseling, C.W.de Jager, L.Lapikas, H.de Vries, M.N.Harakeh, N.Kalantar-Nayestanaki, L.W.Fagg, R.A.Lindgren, D.Van Neck

Electron-Induced Proton Knock-Out from 30Si, 31P and 32S

NUCLEAR REACTIONS 30Si, 31P, 32S(e, e'p), E=330, 454 MeV; measured excitation spectra at given central missing momentum. 30Si, 31P, 32S deduced rms radii, momentum distributions, l=0, 1, 2 transitions spectral functions, integrated knockout spectroscopic strength. Shell model, quasiparticle phonon model calculations.

doi: 10.1016/0375-9474(92)90036-J
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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
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1990CL03      Phys.Rev.Lett. 65, 547 (1990)

B.L.Clausen, R.A.Lindgren, M.Farkhondeh, L.W.Fagg, D.I.Sober, C.W.de Jager, H.de Vries, N.Kalantar-Nayestanaki, B.L.Berman, K.S.Dhuga, J.A.Carr, F.Petrovich, P.E.Burt

Electroexcitation of 6- States in 32S

NUCLEAR REACTIONS 32S(e, e'), E=207 MeV; measured σ(E(e')), form factors; deduced spectator nucleons role. 32S levels deduced extreme single particle model strengths. Stretched state transitions.

doi: 10.1103/PhysRevLett.65.547
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1989MI01      Phys.Rev. C39, 14 (1989)

D.J.Millener, D.I.Sober, H.Crannell, J.T.O'Brien, L.W.Fagg, S.Kowalski, C.F.Williamson, L.Lapikas

Inelastic Electron Scattering from 13C

NUCLEAR REACTIONS 13C(e, e'), E=45-340 MeV; measured σ(E, θ). 13C levels deduced longitudinal, transverse form factors, multipole matrix elements. Shell model.

doi: 10.1103/PhysRevC.39.14
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1988SO07      Phys.Rev. C38, 654 (1988)

D.I.Sober, L.W.Fagg, B.Zeidman, R.D.Lawson, D.F.Geesaman, G.C.Morrison, O.Karban, X.K.Maruyama, H.de Vries, E.A.J.M.Offermann, C.W.de Jager, R.A.Lindgren, J.F.A.van Hienen

Electroexcitation of 8- States in 52Cr

NUCLEAR REACTIONS 52Cr(e, e'), E=170-260 MeV; measured σ(E(e')), θ=115°, 154°. 52Cr deduced B(M8), total T=2, T=3 strengths, sums for M8 transitions. Shell model.

doi: 10.1103/PhysRevC.38.654
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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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1984HI06      Phys.Rev. C30, 1 (1984)

R.S.Hicks, J.B.Flanz, R.A.Lindgren, G.A.Peterson, L.W.Fagg, D.J.Millener

Magnetic Multipole Excitations in 12C by Inelastic Electron Scattering

NUCLEAR REACTIONS 12C(e, e'), E=50.7-338 MeV; measured σ(E(e')), θ=180°, form factors. 12C deduced resonances, J, π, Γ. Shell model comparison.

doi: 10.1103/PhysRevC.30.1
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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


1982BU09      Phys.Rev. C26, 713 (1982)

P.E.Burt, L.W.Fagg, H.Crannell

Magnetic Electroexcitation of the 0.478 MeV State in 7Li at Low Momentum Transfer

NUCLEAR REACTIONS 7Li(e, e'), E=40-74 MeV; measured σ(θ), transverse form factors. 7Li deduced M1 transition width.

doi: 10.1103/PhysRevC.26.713
Citations: PlumX Metrics


1982FA11      Phys.Rev. C26, 1304 (1982)

L.W.Fagg, W.L.Bendel, E.C.Jones, Jr.

Low Multipolarity Magnetic Transitions in 90Zr Excited by 180° Electron Scattering

NUCLEAR REACTIONS 90Zr(e, e'), E=37.2, 60.6 MeV; measured σ(θ=180°). 90Zr deduced M2 transition, B(M1) upper limit.

doi: 10.1103/PhysRevC.26.1304
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1980JO03      Phys.Rev. C21, 1162 (1980)

E.C.Jones, Jr., W.L.Bendel, L.W.Fagg, R.A.Lindgren

Magnetic Electron Scattering from Deuterium at Low-Momentum Transfer

NUCLEAR REACTIONS 2H(e, e'), E=56.4 MeV; measured σ. 2H deduced magnetic form factor.

doi: 10.1103/PhysRevC.21.1162
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1979EN01      Phys.Rev. C19, 569 (1979)

N.Ensslin, L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr.

Inelastic Electron Scattering from 14N at 180°

NUCLEAR REACTIONS 14N(e, e'), E=40.6, 50.6, 60.2 MeV; measured σ(E), θ=180°; deduced Γ0, multipolarities.

doi: 10.1103/PhysRevC.19.569
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1979JO02      Phys.Rev. C19, 610 (1979)

E.C.Jones, Jr., W.L.Bendel, L.W.Fagg, R.A.Lindgren

180° Electron Scattering from 3He

NUCLEAR REACTIONS 3He(e, e'), E=40, 51, 61 MeV; measured σ(E, 180°); deduced magnetic radius.

doi: 10.1103/PhysRevC.19.610
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1977CR02      Nucl.Phys. A278, 253 (1977)

H.Crannell, J.M.Finn, P.Hallowell, J.T.O'Brien, N.Ensslin, L.W.Fagg, E.C.Jones, Jr., W.L.Bendel

Inelastic Electron Scattering at 180° from 14C

NUCLEAR REACTIONS 14C(e, e'), E=37, 50.5, 60.5 MeV; measured σ(Eγ, 180°). 14C deduced levels J, π, Γ, B(λ). Enriched target.

doi: 10.1016/0375-9474(77)90238-X
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1977FA02      Phys.Rev. C15, 1181 (1977)

L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr.

Form Factor for the Electroexcitation of the 5.36 MeV Transition in 6Li

NUCLEAR REACTIONS 6Li(e, e'), E=40.5, 50.5 MeV; measured σ. 6Li level deduced form factors.

doi: 10.1103/PhysRevC.15.1181
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1977FA05      Phys.Rev. C16, 923 (1977)

L.W.Fagg, W.L.Bendel, R.A.Lindgren, E.C.Jones, Jr.

Transitions in 27Al Excited by 180° Electron Scattering

NUCLEAR REACTIONS 27Al(e, e'), E=37.3, 50.9, 60.5 MeV; measured σ(E). 27Al transitions deduced λ, Γ.

doi: 10.1103/PhysRevC.16.923
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1976FA13      Phys.Rev. C14, 1727 (1976)

L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr.

Transitions Excited in 10B by 180° Electron Scattering

NUCLEAR REACTIONS 10B(e, e'), E=40-61 MeV; measured σ(E). 10B levels deduced Γ0, λ.

doi: 10.1103/PhysRevC.14.1727
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1976LI23      Phys.Rev. C14, 1789 (1976)

R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr., L.W.Fagg, X.K.Maruyama, L.W.Lightbody, Jr., S.P.Fivozinsky

Electroexcitation of the T(0) + 1 Giant M1 Resonance in 58,60Ni

NUCLEAR REACTIONS 58,60Ni(e, e'), E=40, 50, 60, 75 MeV; measured σ(E). 58,60Ni deduced levels, J, π, T, B(M1).

doi: 10.1103/PhysRevC.14.1789
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1975LI19      Phys.Rev.Lett. 35, 1423 (1975)

R.A.Lindgren, W.L.Bendel, L.W.Fagg, E.C.Jones, Jr.

Evidence for Giant M2 States in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=37.5, 40.5, 50.5, 60.5 MeV; measured σ(E, Ee'). 208Pb resonances deduced J, π.

doi: 10.1103/PhysRevLett.35.1423
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1975UB01      Acta Phys.Austr. 41, 341 (1975)

H.Uberall, A.Nagl, R.A.Lindgren, L.W.Fagg

Giant Multipole Spin Flip Resonances and Spin Flip Sum Rules

NUCLEAR REACTIONS 20Ne, 24Mg, 58Ni(e, e'), E=60 MeV; 12C, 24Mg, 58Ni(e, e'), E=100, 200, 300 MeV; calculated σ. 12C, 24Mg, 58Ni calculated E2 spin flip strengths.


1975WE15      Phys.Rev. C12, 330 (1975)

D.V.Webb, G.A.Peterson, W.L.Bendel, E.C.Jones, Jr., L.W.Fagg

Search for a l-Forbidden M1 Transition in 39K by Electroexcitation

NUCLEAR REACTIONS 39K(e, e'), E=50.98, 60.65 MeV; measured σ(Ee'). 39K level deduced λ, γ-width.

doi: 10.1103/PhysRevC.12.330
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1974CE01      Phys.Rev. C9, 798 (1974)

F.E.Cecil, L.W.Fagg, W.L.Bendel, E.C.Jones, Jr.

Measurement of the Radiative Width of the 12.71-MeV Level in 12C

NUCLEAR REACTIONS 12C(e, e'), p=50.5 MeV/c; measured level-width(λ); 12C levels deduced isospin mixing.

doi: 10.1103/PhysRevC.9.798
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1974MA43      Phys.Rev. C10, 2257 (1974); Erratum Phys.Rev. C17, 856 (1978)

X.K.Maruyama, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr., L.W.Fagg

Excitation of M1 and M2 States in 22Ne by 183° Electron Scattering

NUCLEAR REACTIONS 22Ne(e, e'), E=37, 50, 60 MeV; measured σ(Ee'). 22Ne levels deduced J, π, B(λ).

doi: 10.1103/PhysRevC.10.2257
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1973FA04      Phys.Lett. 44B, 163 (1973)

L.W.Fagg, W.L.Bendel, N.Ensslin, E.C.Jones, Jr.

Search for Solar-Neutrino Related M1 Transitions in 6Li Using 180° Electron Scattering

NUCLEAR REACTIONS 6Li(e, e'), E=37, 50, 60 MeV; measured σ(E, Ee'). 6Li deduced no M1 resonance.

doi: 10.1016/0370-2693(73)90511-X
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1972FA02      Phys.Rev. C5, 120 (1972); Erratum Phys.Rev. C5, 1143 (1972)

L.W.Fagg, W.L.Bendel, E.C.Jones, Jr., L.Cohen, H.F.Kaiser

States in 36Ar Excited by 180° Electron Scattering

NUCLEAR REACTIONS 36Ar(e, e'), E=39, 56 MeV; measured σ(Ee'). 36Ar deduced levels, J, π, transition radii, level-width, M1, M2 transitions.

doi: 10.1103/PhysRevC.5.120
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1971BE18      Phys.Rev. C3, 1821 (1971)

W.L.Bendel, L.W.Fagg, S.K.Numrich, E.C.Jones, Jr., H.F.Kaiser

Excitation of 20Ne by 180° Electron Scattering

NUCLEAR REACTIONS 20Ne(e, e'), E=39, 56 MeV; measured σ(Ee'). 20Ne deduced levels, level-width, transition radii.

doi: 10.1103/PhysRevC.3.1821
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1971FA15      Phys.Rev. C4, 2089 (1971)

L.W.Fagg, W.L.Bendel, L.Cohen, E.C.Jones, Jr., H.F.Kaiser, H.Uberall

Magnetic Transition Strength in 32S and 40Ca from 180° Electron Scattering

NUCLEAR REACTIONS 32S, 40Ca(e, e'), E=39, 56 MeV; measured σ(Ee'). 32S, 40Ca deduced levels, level-width, transition radii.

doi: 10.1103/PhysRevC.4.2089
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1970FA04      Phys.Rev. C1, 1137 (1970)

L.W.Fagg, W.L.Bendel, S.K.Numrich, B.T.Chertok

Evidence for ΔT = 1 Magnetic Quadrupole Transitions in 24Mg Excited by 180° Electron Scattering

NUCLEAR REACTIONS 24Mg(e, e'), E=39, 56 MeV; measured nothing. 24Mg deduced levels, J, π, level-width, transition radii. Reanalysis of data.

doi: 10.1103/PhysRevC.1.1137
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1969CH10      Phys.Rev.Letters 23, 34 (1969)

B.T.Chertok, E.C.Jones, W.L.Bendel, L.W.Fagg

180° Electron Scattering from 3He and 4He at 56 MeV

NUCLEAR REACTIONS 3He(p, p), E=56.6 MeV; measured σ(E). 3He deduced magnetic form factor, magnetic radius.

doi: 10.1103/PhysRevLett.23.34
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1969FA11      Phys.Rev. 187, 1378 (1969)

L.W.Fagg, W.L.Bendel, E.C.Jones, Jr., S.Numrich

Magnetic Transitions in 28Si Excited by 180° Electron Scattering

NUCLEAR REACTIONS 28Si(e, e'), E=39, 56 MeV; measured σ(Ee'). 28Si deduced levels, level-width, J, π, L, transition radii.

doi: 10.1103/PhysRev.187.1378
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1969FA12      Phys.Rev. 187, 1384 (1969)

L.W.Fagg, W.L.Bendel, E.C.Jones, Jr., H.F.Kaiser, T.F.Godlove

States of 25Mg Excited by 180° Electron Scattering

NUCLEAR REACTIONS 25Mg(e, e'), E=39, 56 MeV; measured σ(Ee'). 25Mg deduced levels, J, π, level-width, T, transition radii.

doi: 10.1103/PhysRev.187.1384
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1968BE33      Phys.Rev. 173, 1103 (1968)

W.L.Bendel, L.W.Fagg, R.A.Tobin, H.F.Kaiser

Inelastic Electron Scattering from 26Mg at 180°

NUCLEAR REACTIONS 26Mg(e, e'), E=39.56 MeV; measured σ(Ee'). 26Mg deduced levels.

doi: 10.1103/PhysRev.173.1103
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1968FA05      Phys.Rev. 171, 1250 (1968)

L.W.Fagg, W.L.Bendel, R.A.Tobin, H.F.Kaiser

Inelastic Electron Scattering from 24Mg at 180°

NUCLEAR REACTIONS 24Mg(e, e'), E=39, 65 MeV; measured σ(Ee'). 24Mg levels deduced level-width.

doi: 10.1103/PhysRev.171.1250
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1959BU81      Phys.Rev. 113, 268 (1959)

J.W.Butler, L.W.Fagg, H.D.Holmgren

Energy Levels in F19 from the O18(d, nγ)F19 Reaction

doi: 10.1103/PhysRev.113.268
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1958FA01      Phys.Rev. 109, 100 (1958)

L.W.Fagg

Coulomb Excitation of Sb, Cs and Ba

doi: 10.1103/PhysRev.109.100
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1957WO32      Phys.Rev. 105, 238 (1957)

E.A.Wolicki, L.W.Fagg, E.H.Geer

Coulomb Excitation of Bromine and Rhenium

doi: 10.1103/PhysRev.105.238
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1956FA29      Phys.Rev. 104, 1073 (1956)

L.W.Fagg, E.H.Geer, E.A.Wolicki

Coulomb Excitation of V, Ni, Ga, and Rb

doi: 10.1103/PhysRev.104.1073
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1955FA40      Phys.Rev. 100, 1299 (1955)

L.W.Fagg, E.A.Wolicki, R.O.Bondelid, K.L.Dunning, S.Snyder

Coulomb Excitation of Tellurium and Silver

doi: 10.1103/PhysRev.100.1299
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1948MO33      Phys.Rev. 74, 1536 (1948)

D.L.Mock, B.C.Waddell, L.W.Fagg, R.A.Tobin

Photo-Induced Reactions at 20 MeV

doi: 10.1103/PhysRev.74.1536
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