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Search: Author = R.A.Lindgren

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2007SO06      Phys.Rev. C 75, 034611 (2007)

D.S.Sorenson, J.L.Ullmann, A.Ling, B.K.Park, R.C.Haight, N.S.P.King, R.A.Lindgren, H.Baghaei, E.J.Stephenson, F.P.Brady, J.L.Romero, J.Rapaport, B.L.Clausen, C.Wuest, F.Sammarruca

Limitations of the distorted-wave impulse approximation in describing the energy dependence of the 10B(n, p)10Be(g.s.) reaction

NUCLEAR REACTIONS 10B(n, p), E=70240 MeV; measured σ(E, θ). Comparison with zero- and finite-range DWIA predictions.

doi: 10.1103/PhysRevC.75.034611
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14139.

2005BE43      Phys.Rev. C 71, 064607 (2005)

A.C.Betker, S.Chang, E.J.Stephenson, A.D.Bacher, S.M.Bowyer, W.A.Franklin, J.Liu, C.Olmer, D.L.Prout, S.P.Wells, S.W.Wissink, C.Yu, R.A.Lindgren, H.Baghaei, V.Gladyshev, J.A.Carr, S.K.Yoon, F.Petrovich, B.L.Clausen, J.Lisantti

Reaction mechanism for natural parity (p, p') transitions in 10B

NUCLEAR REACTIONS 10B(polarized p, p), (polarized p, p'), E=197 MeV; measured σ(E, θ), analyzing power, polarization transfer coefficients. Comparison with model predictions.

doi: 10.1103/PhysRevC.71.064607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1291.

2002UL01      Phys.Rev.Lett. 89, 062301 (2002)

P.E.Ulmer, K.A.Aniol, H.Arenhovel, J.-P.Chen, E.Chudakov, D.Crovelli, J.M.Finn, K.G.Fissum, O.Gayou, J.Gomez, J.-O.Hansen, C.W.de Jager, S.Jeschonnek, M.K.Jones, M.Kuss, J.J.LeRose, M.Liang, R.A.Lindgren, S.Malov, D.Meekins, R.Michaels, J.Mitchell, C.F.Perdrisat, V.Punjabi, R.Roche, F.Sabatie, A.Saha, R.Suleiman, L.Todor, B.B.Wojtsekhowski

2H(e, e'p)n Reaction at High Recoil Momenta

NUCLEAR REACTIONS 2H(e, e'p), E=3.110 GeV; measured Ep, σ vs recoil momentum. Comparison with model predictions.

doi: 10.1103/PhysRevLett.89.062301
Citations: PlumX Metrics

1997CL01      Phys.Rev. C55, 625 (1997)

B.L.Clausen, T.W.Johnson, R.A.Lindgren, K.Cromer, R.J.Peterson, A.D.Bacher, H.Ward, A.L.Williams

Pion Scattering to 6- Stretched States in 32S

NUCLEAR REACTIONS 32S(π+, π+), (π-, π-'), E=162 MeV; measured spectra, σ(θ). 32S levels deduced spectroscopic factors, isoscalar, isovector magnetic structure coefficients.

doi: 10.1103/PhysRevC.55.625
Citations: PlumX Metrics

1997OF01      Phys.Rev. C55, 1295 (1997)

B.G.Ofenloch, R.A.Giannelli, B.G.Ritchie, J.M.O'Donnell, J.N.Knudson, C.L.Morris, C.M.Kormanyos, A.Saunders, J.Z.Williams, R.A.Lindgren, B.L.Clausen

Pion-Nucleus Spin-Flip Strength at Low and Resonance Energies

NUCLEAR REACTIONS 10B(π+, π+'), E=65 MeV; measured σ(θ). 10B deduced isovector spin-flip strength parameter, B(λ). Other data analyzed.

doi: 10.1103/PhysRevC.55.1295
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
Citations: PlumX Metrics

1995SE02      Phys.Rev. C51, 1926 (1995)

R.M.Sellers, D.M.Manley, M.M.Niboh, D.S.Weerasundara, R.A.Lindgren, B.L.Clausen, M.Farkhondeh, B.E.Norum, B.L.Berman

Inelastic Electron Scattering from 18O at Backward Angles

NUCLEAR REACTIONS 18O(e, e'), E=140.3-275.2 MeV; measured electron spectra, form factors. 18O levels deduced reduced transition probabilities, J, π, T.

doi: 10.1103/PhysRevC.51.1926
Citations: PlumX Metrics

1994GA18      Phys.Rev. C50, 289 (1994)

L.A.C.Garcia, B.D.Anderson, D.M.Manley, A.R.Baldwin, R.Pourang, E.Steinfelds, J.W.Watson, R.A.Lindgren, B.L.Clausen, A.D.Bacher, C.C.Foster

Identification of 4- States in the 14C(p, n)14N Reaction at 135 MeV

NUCLEAR REACTIONS 14C(p, n), E=135 MeV; measured neutron spectra, σ(E(n), θ=135°), σ(θ) vs momentum. 14N deduced levels, J, π, T, isovector transition strengths.

doi: 10.1103/PhysRevC.50.289
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0131.

1993WA06      Phys.Rev. C47, 2123 (1993)

L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, R.A.Lindgren, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park

10B(p, n)10C Reaction at 186 MeV

NUCLEAR REACTIONS 10B(p, n), (polarized p, n), E=186 MeV; measured σ(θn, En), analyzing power, polarization, polarization transfer. 10C deduced resonances, J, π, possible IAS character.

doi: 10.1103/PhysRevC.47.2123
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0587.

1992BA76      Phys.Rev.Lett. 69, 2054 (1992)

H.Baghaei, R.A.Lindgren, P.Slocum, E.J.Stephenson, A.D.Bacher, S.Chang, J.Lisantti, J.Liu, C.Olmer, S.Wells, S.W.Wissink, B.L.Clausen, J.A.Carr, S.K.Yoon, F.Petrovich

Spin Transverse-Longitudinal Composition of the Isovector Effective NN Interaction from 10B(p(pol), p(pol)') at 200 MeV

NUCLEAR REACTIONS 10B(polarized p, p), E=200 MeV; measured σ(θ), analyzing power, induced polarization, polarization transfer coefficients vs θ; deduced large transverse to longitudinal spin-dependent interaction ratio.

doi: 10.1103/PhysRevLett.69.2054
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1327.

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
Citations: PlumX Metrics

1991LI35      Phys.Rev. C44, 2413 (1991)

R.A.Lindgren, B.L.Clausen, G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, B.H.Wildenthal, R.Gilman, J.A.Carr

Pion Scattering to 6- Stretched States in 24Mg and 26Mg

NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=116-180 MeV; measured pion spectra, σ(θ). 26,24Mg levels deduced stretched configuration isoscalar, isovector strength.

doi: 10.1103/PhysRevC.44.2413
Citations: PlumX Metrics

1990BL04      Phys.Rev. C41, 1625 (1990)

G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, R.A.Lindgren, B.H.Wildenthal, R.Gilman

Pion Elastic and Inelastic Scattering from 24Mg and 26Mg

NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=150, 180 MeV; measured σ(θ), σ(E(π)). 26,24Mg levels deduced deformation parameters, neutron, proton matrix elements.

doi: 10.1103/PhysRevC.41.1625
Citations: PlumX Metrics

1990CL02      Phys.Rev. C41, 2246 (1990)

B.L.Clausen, J.T.Brack, M.R.Braunstein, J.J.Kraushaar, R.A.Loveman, R.J.Peterson, R.A.Ristinen, R.A.Lindgren, M.A.Plum

Analysis of Pion Scattering to Stretched States in 60Ni and Other Nuclei using Woods-Saxon Wave Functions

NUCLEAR REACTIONS 60Ni(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ). 14C, 28Si, 54Fe, 60Ni deduced stretched state parameters. Other data input.

doi: 10.1103/PhysRevC.41.2246
Citations: PlumX Metrics

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
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
Citations: PlumX Metrics

1989SE01      Phys.Rev. C39, 749 (1989)

R.E.Segel, A.Amusa, D.F.Geesaman, R.D.Lawson, B.Zeidman, C.Olmer, A.D.Bacher, G.T.Emery, C.W.Glover, H.Nann, W.P.Jones, S.Y.van der Werf, R.A.Lindgren

Fragmentation of High-Spin Particle-Hole States in 26Mg

NUCLEAR REACTIONS 26Mg(polarized p, p'), E=135 MeV; measured σ(θ), A(θ). 26Mg deduced levels, J, π. 28Si deduced levels, J, π, isoscalar, isovector excitation amplitudes. Other data input.

doi: 10.1103/PhysRevC.39.749
Citations: PlumX Metrics

1988CL03      Phys.Rev. C38, 589 (1988)

B.L.Clausen, R.J.Peterson, R.A.Lindgren

Electron Scattering Form Factors of Stretched Transitions Using Woods-Saxon Wave Functions

NUCLEAR REACTIONS 12,14C, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58,60Ni, 90Zr, 208Pb(e, e'), E not given; calculated form factors; deduced single particle sum rule strength fractions.

doi: 10.1103/PhysRevC.38.589
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1987LI30      Can.J.Phys. 65, 666 (1987)

R.A.Lindgren, M.Leuschner, B.L.Clausen, R.J.Peterson, M.A.Plum, F.Petrovich

Isovector Excitation of 1(h-bar x Omega) Stretched States in Nuclei: Effects of meson exchange currents, unbound wave functions, and knockout exchange amplitudes on the extraction of particle-hole strengths

NUCLEAR REACTIONS 14C, 26Mg, 28Si, 54Fe, 60Ni(e, e'), E ≈ 136-205 MeV; analyzed σ(E(e'), θ(e')). 14C, 26Mg, 28Si, 54Fe, 60Ni deduced form factors, particle-hole strengths, amplitudes, B(λ). Meson exchange currents.

doi: 10.1139/p87-095
Citations: PlumX Metrics

1987PE03      Phys.Rev. C35, 495 (1987)

R.J.Peterson, B.L.Clausen, J.J.Kraushaar, R.A.Lindgren, M.A.Plum, W.W.Jacobs, H.Nann

Proton Stripping to 8- Stretched States in 60Ni

NUCLEAR REACTIONS 59Co(α, t), E=80.9 MeV; measured σ(θ). 60Ni deduced levels, J, π, T, spectroscopic factors. Magnetic spectrometer. DWBA analyses.

doi: 10.1103/PhysRevC.35.495
Citations: PlumX Metrics

1986HI06      Phys.Rev. C34, 1161 (1986)

R.S.Hicks, R.A.Lindgren, M.A.Plum, G.A.Peterson, H.Crannell, D.I.Sober, H.A.Thiessen, D.J.Millener

M4 Excitations in 13C

NUCLEAR REACTIONS 13C(e, e'), E=78-338 MeV; measured σ(E, θ). 13C levels deduced from factors, isoscalar, isovector transition amplitudes. Shell model.

doi: 10.1103/PhysRevC.34.1161
Citations: PlumX Metrics

1986PE01      Phys.Rev. C33, 31 (1986)

R.J.Peterson, B.L.Clausen, J.J.Kraushaar, H.Nann, W.W.Jacobs, R.A.Lindgren, M.A.Plum

Proton Stripping to 6- Stretched States of 26Al

NUCLEAR REACTIONS 24,25Mg(α, t), E=80.9 MeV; measured σ(Et), σ(θ). 26Al deduced levels, J, π, T, spectroscopic factors, stretched transition characteristics.

doi: 10.1103/PhysRevC.33.31
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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
Citations: PlumX Metrics

1984GE06      Phys.Rev. C30, 952 (1984)

D.F.Geesaman, R.D.Lawson, B.Zeidman, G.C.Morrison, A.D.Bacher, C.Olmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, R.L.Boudrie, C.L.Morris, R.A.Lindgren, W.H.Kelly, R.E.Segel, L.W.Swenson

Quenching of Isoscalar Spin-Flip Strength in 54Fe

NUCLEAR REACTIONS 54Fe(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 54Fe levels deduced isoscalar, isovector strengths.

doi: 10.1103/PhysRevC.30.952
Citations: PlumX Metrics

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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1984LI25      J.Phys.(Paris), Colloq.C-4, 433 (1984)


Stretched Excitations as a Means to Study the Spin Modes of the Nucleus with Electromagnetic and Hadronic Probes

NUCLEAR REACTIONS 51V, 50Ti, 52Cr, 54Fe(e, e'), (p, p'), E not given; analyzed B(M1) data. 12,13,14C, 14N(e, e'), E=196.5-225 MeV; analyzed σ(Ee', θe'). 12,14C, 14N, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58Ni, 90Zr, 208Pb(e, e'), E not given; analyzed σ(Ee', θe'). 12,14C, 14N, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58Ni, 90Zr, 208Pb deduced stretched states spectroscopic strength, transverse factors.

1984MI14      Nucl.Phys. A430, 189 (1984)

H.Miessen, H.Rothhaas, G.Luhrs, G.A.Peterson, R.S.Hicks, R.A.Lindgren, B.L.Berman, S.Kowalski, C.F.Williamson

Elastic Magnetic Electron Scattering from 29Si and 31P

NUCLEAR REACTIONS 29Si, 31P(e, e), E=90-280 MeV; measured transverse electric σ(θ) vs E, form factors. 29Si, 31P deduced radial current densities, occupation probabilities, 2s1/2 neutron, proton orbitals. Enriched 29Si, natural 31P targets. Particle-core coupling, shell model interpretations.

doi: 10.1016/0375-9474(84)90200-8
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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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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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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
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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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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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1981LI05      Phys.Rev.Lett. 46, 706 (1981)

R.A.Lindgren, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson, R.D.Lawson, W.Teeters, C.F.Williamson, S.Kowalski, X.K.Maruyama

Comparison of Inelastic Electron Scattering with [g9/2 x (f1/2-3)(J)] (8)- Shell-Model Calculations for the T=1 and T=2, 8-States in 54Fe

NUCLEAR REACTIONS 54Fe(e, e'), E=205.1 MeV; measured σ(E(e')), form factors. 54Fe levels deduced J, π, T, γ-multipolarity, B(M8) strength distribution. Shell model calculations.

doi: 10.1103/PhysRevLett.46.706
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1981LI19      Phys.Rev.Lett. 47, 1266 (1981)

R.A.Lindgren, M.A.Plum, W.J.Gerace, R.S.Hicks, B.Parker, G.A.Peterson, R.Singhal, C.F.Williamson, X.K.Maruyama, F.Petrovich

Isospin Splitting of Isovector High-Spin ' Stretched ' Particle-Hole Excitations in Non-Self-Conjugate Nuclei

NUCLEAR REACTIONS 60Ni(e, e'), E=205 MeV; measured σ(θ(e), E(e)). 60Ni deduced levels, J, π, T, B(M8), isospin splitting. Lane model parametrization, stretched particle-hole excitations.

NUCLEAR STRUCTURE 13C, 15N, 54,56Fe, 58,60Ni; calculated isospin splitting. Lane model parametrization, stretched particle-hole excitation.

doi: 10.1103/PhysRevLett.47.1266
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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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1979AN01      Nucl.Phys. A313, 445 (1979)

N.Anantaraman, H.E.Gove, R.A.Lindgren, J.Toke, J.P.Trentelman, J.P.Draayer, F.C.Jundt, G.Guillaume

Alpha-Particle Strengths from the 16O(6Li, d)20Ne Reaction

NUCLEAR REACTIONS 16O(6Li, d), E=20, 32, 38 MeV; measured σ(Ed, θ). 20Ne levels deduced Sα. DWBA analysis. Natural target.

doi: 10.1016/0375-9474(79)90512-8
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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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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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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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1979LI06      Phys.Rev.Lett. 42, 1524 (1979)

R.A.Lindgren, W.J.Gerace, A.D.Bacher, W.G.Love, F.Petrovich

Tensor Force and Inelastic Electron and Proton Scattering to Unnatural-Parity States of Stretched Configurations

NUCLEAR STRUCTURE 12C, 16O, 24Mg, 28Si, 58Ni, 208Pb; analyzed(e, e'), (p, p') transitions involving unnatural parity states; deduced high-momentum components of tensor term of nucleon-nucleon force.

doi: 10.1103/PhysRevLett.42.1524
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1978FL09      Phys.Rev.Lett. 41, 1642 (1978)

J.B.Flanz, R.S.Hicks, R.A.Lindgren, G.A.Peterson, A.Hotta, B.Parker, R.C.York

Convection Currents and Spin Magnetization in E2 Transitions of 12C

NUCLEAR REACTIONS 12C(e, e'); measured square of electromagnetic form factors; 12C 4.439-MeV level deduced contribution of nuclear convection currents. 12C 16.107-MeV level deduced spin magnetization contributions.

doi: 10.1103/PhysRevLett.41.1642
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1978LI02      Phys.Rev.Lett. 40, 504 (1978)

R.A.Lindgren, C.F.Williamson, S.Kowalski

Fragmentation of Isovector M8 Strength in 58Ni

NUCLEAR REACTIONS 58Ni(e, e), E=153.6, 167.6, 172.2, 196.3, 221.0, 228.1, 242.6, 263.9 MeV; measured σ(E). 58Ni deduced levels, form factors, M8 strength.

doi: 10.1103/PhysRevLett.40.504
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1978LI25      Phys.Rev.Lett. 41, 1705 (1978)

R.A.Lindgren, J.B.Franz, W.J.Gerace, R.S.Hicks, A.Hotta, D.Huse, G.A.Peterson, R.C.York, C.F.Williamson, S.Kowalski

Isoscalar Character of the Jπ = 6+, E(x) = 5.125 MeV State in 58Ni

NUCLEAR REACTIONS 58Ni(e, e'), E=189.6-251.1 MeV; measured σ(E, θ). 58Ni 5.12-MeV level deduced transverse, longitudinal form factors, configuration.

doi: 10.1103/PhysRevLett.41.1705
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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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1977FU03      Nucl.Phys. A284, 329 (1977)

H.W.Fulbright, C.L.Bennett, R.A.Lindgren, R.G.Markham, S.C.McGuire, G.C.Morrison, U.Strohbusch, J.Toke

Four-Nucleon Transfer via the (6Li, d) Reaction

NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 50,52,54Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28-38 MeV; measured σ(Ed, θ). 44Ti, 54,58,56Fe, 58,60Ni, 62,64,66Zn deduced levels, Sα, L, J, π. DWBA analysis.

doi: 10.1016/0375-9474(77)90127-0
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1977ZA02      Phys.Rev.Lett. 38, 750 (1977)

H.Zarek, B.O.Pich, T.E.Drake, D.J.Rowe, W.Bertozzi, C.Creswell, A.Hirsch, M.V.Hynes, S.Kowalski, B.Norum, F.N.Rad, C.P.Sargent, C.F.Williamson, R.A.Lindgren

Discovery of a 6-, T = 1 Resonance in 24Mg via High-Resolution Inelastic Electron Scattering

NUCLEAR REACTIONS 24Mg(e, e'), E=108-260 MeV; measured spectra. 24Mg deduced resonance, J, π, t.

doi: 10.1103/PhysRevLett.38.750
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1976BO24      Phys.Rev. C14, 4 (1976)

R.N.Boyd, D.Elmore, W.P.Alford, J.P.Draayer, R.A.Lindgren

Levels in 28Si via the 26Mg(3He, n) Reaction

NUCLEAR REACTIONS 26Mg(3He, n), E=15 MeV; measured σ(En, θ). 28Si levels deduced S. DWBA analysis.

doi: 10.1103/PhysRevC.14.4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0469.

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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1975AL05      Nucl.Phys. A243, 269 (1975)

W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd

Jπ = 0+ States in the (fp) Shell Excited in the (3He, n) Reaction

NUCLEAR REACTIONS 46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni(3He, n), E=15 MeV; measured σ(θ, En). 48,50,52Cr, 52,54,56Fe, 56,58,60Ni, 60,62,64,66Zn levels deduced J, π, L, S. DWBA analysis, model comparison. Enriched targets.

doi: 10.1016/0375-9474(75)90248-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0510.

1975FU02      Phys.Lett. 53B, 449 (1975)

H.W.Fulbright, U.Strohbusch, R.G.Markham, R.A.Lindgren, G.C.Morrison, S.C.McGuire, C.L.Bennett

(6Li, d) Spectroscopy in the f-p Shell

NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 52Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28, 32 MeV; measured σ(Ed, θ). 58Ni levels deduced J.

doi: 10.1016/0370-2693(75)90215-4
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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.

1974AL14      Phys.Rev. C10, 1013 (1974)

W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd

Structure of 42Ti from the 40Ca(3He, n)42Ti Reaction

NUCLEAR REACTIONS 40Ca(3He, n), E=15 MeV; measured σ(En, θ). 42Ti deduced levels, J, π, L, analogs. DWBA analysis.

doi: 10.1103/PhysRevC.10.1013
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1974LI01      Phys.Lett. 48B, 209 (1974)

R.A.Lindgren, R.G.Markham, H.W.Fulbright

The 6Li-Induced Three-Nucleon Transfer Reaction on 40Ca

NUCLEAR REACTIONS 40Ca(6Li, 3He), (6Li, t), E=34.0, 36.0 MeV; measured σ(E(3He), E(3H), θ). 43Sc, 43Ti deduced levels, L, J, π, S.

doi: 10.1016/0370-2693(74)90012-4
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1974LI02      Phys.Lett. 49B, 263 (1974)

R.A.Lindgren, J.P.Trentelman, N.Anantaraman, H.E.Gove, J.C.Jundt

Odd-Parity Levels Excited in 32S and 36Ar via 'Alpha-Particle' Transfer

NUCLEAR REACTIONS 28Si, 32S(6Li, d), E=32 MeV; measured σ(Ed). 32S, 36Ar deduced levels, J, π.

doi: 10.1016/0370-2693(74)90429-8
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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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1973AL23      Phys.Lett. 46B, 356 (1973)

W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd

Two-Particle, Two-Hole Jπ = 0+ States in 40Ca

NUCLEAR REACTIONS 38Ar(3He, n), E=15 MeV; measured σ(En, θ). 40Ca deduced levels, J, π.

doi: 10.1016/0370-2693(73)90138-X
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1973PA14      Phys.Rev. C8, 1557 (1973); Erratum Phys.Rev. C9, 1673 (1974)

Y.S.Park, A.Niiler, R.A.Lindgren

Spectroscopy of 10B Levels from the 9Be(d, n)10B Reaction

NUCLEAR REACTIONS 9Be(d, n), E=7, 12, 15, 16 MeV; measured σ(E;En, θ). 10B deduced levels, J, π, L, S.

doi: 10.1103/PhysRevC.8.1557
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0110.

1972AL48      Phys.Lett. 42B, 60 (1972)

W.P.Alford, R.A.Lindgren, D.Elmore

A Comparison of (3He, n) Ground-State Transitions in the (fp) Shell with Predictions of the Pairing Vibrational Model

NUCLEAR REACTIONS 46Ti, 54Fe, 58Ni(3He, n), E=15 MeV; measured σ(θ).

doi: 10.1016/0370-2693(72)90716-2
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1972LI02      Nucl.Phys. A180, 1 (1972)

R.A.Lindgren, R.G.Hirko, J.G.Pronko, A.J.Howard, M.W.Sachs, D.A.Bromley

A Study of 23Na

NUCLEAR REACTIONS 23Na(α, α'γ), 26Mg(p, αγ), Eα=16.85 MeV, Ep=14.25 MeV; measured αγ(θ), pγ(θ), Iγ. 23Na levels deduced J, branching, multipole mixing ratios. Enriched 26Mg target.

doi: 10.1016/0375-9474(72)90152-2
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1972LI24      Phys.Rev.Lett. 29, 798 (1972)

R.A.Lindgren, H.H.Gutbrod, H.W.Fulbright, R.G.Markham

Odd-Parity Three-Particle, One-Hole Structure in 18F via the Reaction 15N(6Li, t)18F

NUCLEAR REACTIONS 15N(6Li, t), E=30 MeV; measured σ(Et, θ). 18F deduced odd-parity, 3p-1h structure.

doi: 10.1103/PhysRevLett.29.798
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1972PR06      Nucl.Instrum.Methods 98, 445 (1972)

J.G.Pronko, R.A.Lindgren

Angular Correlations of Sequential Particle Decay for Aligned Nuclei

doi: 10.1016/0029-554X(72)90226-1
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1971HI05      Particles and Nuclei 1, 372 (1971)

R.G.Hirko, R.A.Lindgren, A.J.Howard, J.G.Pronko, M.W.Sachs, D.A.Bromley

Nuclear Structure Studies on 29Al

NUCLEAR REACTIONS 27Al(t, p), E=3.34 MeV; measured σ(Ep, θ). 26Mg(α, pγ), E=13.82, 14 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). 29Al deduced levels, J, π, γ-mixing, γ-branching.

1971LI27      Phys.Lett. 37B, 358 (1971)

R.A.Lindgren, F.C.Young, B.Cotton

Spins of the Isospin Mixed 5.61 and 5.67 MeV Levels in 18F

NUCLEAR REACTIONS 19F(3He, α), E=5-6 MeV; measured σ(E;Eα, θ(αα)). 18F levels deduced J, π.

doi: 10.1016/0370-2693(71)90201-2
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1971LI34      Bull.Am.Phys.Soc. 16, No.10, 1177 EB8 (1971)

R.A.Lindgren, R.M.Tapphorn

Colinear Particle-Particle Angular Correlations on the Ca40 (p, α) K37 (po) Ar36 Reaction

RADIOACTIVITY 37K(p) [from 40Ca(p, α), E=15.75 MeV]; measured Ep, Ip, Eα, Iα; deduced levels, J, angular correlation of p in coincidence with α-particles from 40Ca(p, α), σ(θ).

1971YO05      Nucl.Phys. A176, 289 (1971)

F.C.Young, R.A.Lindgren, W.Reichart

Spin-Parity Determinations of 10B Levels by 11B(3He, α)10B(α0)6Li Correlations

NUCLEAR REACTIONS 11B(3He, α), α + 6Li, E=5.0, 4.55, 2.8 MeV; measured σ(Eα;E(αα), θ(αα)), σ(Eα;E(6Li)θ(6Li)). 10B deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(71)90271-5
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1970LI08      Phys.Lett. 32B, 103 (1970)

R.A.Lindgren, J.G.Pronko, A.J.Howard, D.A.Bromley

The Identification of Mirror State Structure in 21Na and 21Ne

NUCLEAR REACTIONS 24Mg(p, α); E=17.5 MeV; measured σ(Eα, Ep), αp(θ). 21Na levels deduced J.

doi: 10.1016/0370-2693(70)90598-8
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1970PR01      Nucl.Phys. A140, 465 (1970)

J.G.Pronko, R.A.Lindgren, D.A.Bromley

Structure of 21Na from the 24Mg(p, α)21Na Reaction

NUCLEAR REACTIONS 24Mg(p, α), E=17.5 MeV; measured αγ(θ), Iγ, σ(Eα, θ(α)). 21Na levels deduced J, γ-branching, γ-mixing . Enriched target.

doi: 10.1016/0375-9474(70)90337-4
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