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NSR database version of April 26, 2024.

Search: Author = B.L.Burks

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1990BE03      Phys.Rev. C41, 920 (1990)

J.R.Beene, F.E.Bertrand, D.J.Horen, R.L.Auble, B.L.Burks, J.Gomez del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien

Heavy-Ion Coulomb Excitation and Photon Decay of the Giant Dipole Resonance in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷O, ¹⁷O'), E=84 MeV/nucleon; measured σ(E(¹⁷O)), γ(particle)(θ, φ) following Coulomb excitation, σ(θ). ²⁰⁸Pb deduced giant resonance decay features, B(λ), M(n)/M(p).

doi: 10.1103/PhysRevC.41.920
Citations: PlumX Metrics

1989HO11      Z.Phys. A333, 39 (1989)

D.J.Horen, J.Lisantti, R.L.Auble, F.E.Bertrand, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson

T = 1, Spin-Dipole Strength in ⁴⁰Ca

NUCLEAR REACTIONS ⁴⁰Ca(p, p'), E=500 MeV; measured σ(θ), σ(Ep). ⁴⁰Ca deduced T=1 spin-dipole transition strength distribution.

1989LI03      Phys.Rev. C39, 568 (1989)

J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson

Collective Model Distored-Wave Born Approximation Analysis of 500-MeV Proton Scattering form ⁴⁰Ca

NUCLEAR REACTIONS ⁴⁰Ca(polarized p, p'), E=500 MeV; analyzed σ(θ), analyzing power vs θ; deduced optical model parameters. ⁴⁰Ca levels deduced deformation lengths, multipole matrix elements. Relativistic, non-relativistic DWBA analysis.

doi: 10.1103/PhysRevC.39.568
Citations: PlumX Metrics

1989LI15      Phys.Rev. C40, 211 (1989)

J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson

Giant Resonance Strength Distribution in ⁴⁰Ca from Inelastic Scattering of 500 MeV Protons

NUCLEAR REACTIONS ⁴⁰Ca(polarized p, p'), E=500 MeV; measured σ(θp, Ep), σ(θ). ⁴⁰Ca deduced giant resonance strength distribution.

doi: 10.1103/PhysRevC.40.211
Citations: PlumX Metrics

1989SW01      Phys.Rev. C40, 246 (1989)

L.W.Swenson, X.Y.Chen, J.Lisantti, D.K.McDaniels, I.Bergqvist, F.E.Bertrand, D.J.Horen, E.E.Gross, C.Glover, R.O.Sayer, B.L.Burks, O.Hausser, K.Hicks, M.J.Iqbal

Different Continuum Approaches to Giant Resonances in ²⁰⁸Pb with 400-MeV Protons

NUCLEAR REACTIONS ²⁰⁸Pb(p, p'), E=400 MeV; ²⁰⁸Pb(polarized p, p'), E=200 MeV; measured σ(θ). ²⁰⁸Pb deduced giant resonance L, Γ, EWSR. DWBA analysis, continuum models comparison.

doi: 10.1103/PhysRevC.40.246
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0166.

1988BA39      Phys.Lett. 209B, 182 (1988)

J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, D.J.Horen, J.R.Beene, F.E.Bertrand, R.L.Auble, B.L.Burks, J.Gomez Del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, B.Haas, J.P.Vivien

Coulomb Excitation of Giant Resonances in ²⁰⁸Pb by E = 84 MeV/Nucleon ¹⁷O Projectiles

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷O, ¹⁷O), (¹⁷O, ¹⁷O'), E=1428 MeV; measured σ(θ). ²⁰⁸Pb deduced giant resonance excitation mechanism, B(λ), EWSR.

doi: 10.1016/0370-2693(88)90929-X
Citations: PlumX Metrics

1988BU15      Phys.Rev. C38, 1680 (1988)

B.L.Burks, M.A.G.Fernandes, G.R.Satchler, D.J.Horen, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen

Optical Model and Coupled-Channels Analyses of the Elastic and Inelastic Scattering of ¹⁸O from ²⁸Si at 352 MeV

NUCLEAR REACTIONS ²⁸Si(¹⁸O, ¹⁸O), (¹⁸O, ¹⁸O'), E=351.7 MeV; measured σ(θ). Optical model, coupled-channels analyses.

doi: 10.1103/PhysRevC.38.1680
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1988HA26      Phys.Rev. C38, 572 (1988)

B.A.Harmon, D.Shapira, P.H.Stelson, B.L.Burks, K.A.Erb, B.Shivakumar, K.Teh, S.T.Thornton

Effect of Entrance Channel Asymmetry of Fusion Reactions Leading to Compound Nuclei with A = 40, 42

NUCLEAR REACTIONS ¹²C(²⁸Si, X), E=6.4, 7.8, 9.4 MeV/nucleon; ¹²C(³⁰Si, X), E=5.2, 5.7, 6.4, 7.5, 8.3 MeV/nucleon; measured fusion σ; deduced entrance channel asymmetry role.

doi: 10.1103/PhysRevC.38.572
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1988LI18      Phys.Rev. C37, 2408 (1988)

J.Lisantti, F.E.Bertrand, D.J.Horen, B.L.Burks, C.W.Glover, D.K.McDaniels, L.W.Swenson, X.Y.Chen, O.Hausser, K.Hicks

Excitation of Giant Resonances in ²⁸Si with 250 MeV Protons

NUCLEAR REACTIONS ²⁸Si(p, p), (p, p'), E=250 MeV; measured σ(θ). ²⁸Si deduced level deformation lengths, giant resonance EWSR.

doi: 10.1103/PhysRevC.37.2408
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1987BE02      Phys.Rev. C35, 111 (1987)

F.E.Bertrand, R.O.Sayer, R.L.Auble, M.Beckerman, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, J.Gomez del Campo, D.Shapira, H.P.Morsch

Excitation of the High Energy Nuclear Continuum in ²⁰⁸Pb by 22 MeV/Nucleon ¹⁷O and ³²S

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷O, ¹⁷O'), (³²S, ³²S'), E=22 MeV/nucleon; measured σ(E(¹⁷O)), σ(E(³²S)). Enriched targets, magnetic spectrograph.

doi: 10.1103/PhysRevC.35.111
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1987BE03      Phys.Rev.Lett. 58, 455 (1987)

M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, C.W.Glover, R.O.Sayer, G.R.Satchler, D.Shapira, R.L.Varner

Quasielastic Transfer of a Neutron between ⁵⁸Ni and ²⁰⁸Pb at Bombarding Energies of 598 and 1011 MeV

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁸Ni, ⁵⁹Ni), (⁵⁸Ni, ⁵⁷Ni), E=598, 1011 MeV; measured σ(E(⁵⁹Ni)), σ(E(⁵⁷Ni)), σ(θ). Enriched targets, tof. DWBA analyses.

doi: 10.1103/PhysRevLett.58.455
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1987BE23      Phys.Rev. C36, 657 (1987)

M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, R.O.Sayer, G.R.Satchler, D.Shapira, Y.Sugiyama, R.L.Varner

Elastic and Inelastic Scattering of ⁵⁸Ni + ²⁰⁸Pb at Bombarding Energies from 598 to 1011 MeV

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁸Ni, ⁵⁸Ni), (⁵⁸Ni, ⁵⁸Ni'), E=598-1011 MeV; measured σ(E), σ(θ). ²⁰⁸Pb, ⁵⁸Ni levels deduced B(E2), Coulomb deformation constants. Optical model, DWBA, coupled-channels calculations.

doi: 10.1103/PhysRevC.36.657
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1987FE04      Phys.Rev. C36, 108 (1987)

M.A.G.Fernandes, F.E.Bertrand, R.L.Auble, R.O.Sayer, B.L.Burks, D.J.Horen, E.E.Gross, J.L.Blankenship, D.Shapira, M.Beckerman

Single-Nucleon Transfer Reactions Induced by 376-MeV ¹⁷O on ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷O, ¹⁶O), (¹⁷O, ¹⁸F), E=376 MeV; measured σ(θ); deduced model parameters. ²⁰⁹Pb, ²⁰⁷Tl levels deduced spectroscopic factors. DWBA analysis.

doi: 10.1103/PhysRevC.36.108
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1987HO18      Z.Phys. A328, 189 (1987)

D.J.Horen, M.A.G.Fernandes, G.R.Satchler, B.L.Burks, R.L.Auble, F.E.Bertrand, E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira

Transfer Reactions at High Energy and Ambiguities in Heavy-Ion Potentials

NUCLEAR REACTIONS ²⁸Si(¹⁶O, ¹⁶O), E=56, 351.7 MeV; calculated σ(θ); deduced optical potential parameters. ²⁸Si(¹⁸O, ¹⁷O), E=352 MeV; ²⁸Si(¹⁸O, ¹⁹F), E=352 MeV; analyzed data; deduced model parameters. ²⁹Si, ²⁹Al levels deduced spectroscopic factors.

1987MC03      Nucl.Phys. A467, 557 (1987)

D.K.McDaniels, J.Lisantti, I.Bergqvist, L.W.Sewnson, X.Y.Chen, D.J.Horen, F.E.Bertrand, E.E.Gross, C.Glover, R.Sayer, B.L.Burks, O.Hausser, K.Hicks

Validity of Collective Model DWBA Analysis for Intermediate Energy Proton Scattering to Low-Lying States of ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(p, p'), E=200, 400 MeV; measured σ(θ). ²⁰⁸Pb levels deduced deformation lengths, multipole moments, neutron, proton matrix element ratio. DWBA analysis.

doi: 10.1016/0375-9474(87)90386-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0228.

1986BU14      Nucl.Phys. A457, 337 (1986)

B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, B.C.Karp, Y.Aoki

A DWBA Analysis of the ⁸⁶Sr(d(pol), p)⁸⁷Sr Reaction and Implications for a ⁸⁷Rb Solar Neutrino Detector

NUCLEAR REACTIONS ⁸⁶Sr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), vector analyzing power versus θ. ⁸⁷Sr deduced levels, J, π, S. DWBA, optical model analyses.

doi: 10.1016/0375-9474(86)90382-9
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1986BU18      Phys.Rev. C34, 2316 (1986)

B.L.Burks, R.L.Varner, E.J.Ludwig

Q-Value Determination for the ⁸⁰Kr(d, p)⁸¹Kr Reaction

NUCLEAR REACTIONS ⁸⁰Kr(d, p), E=11 MeV; measured σ(Ep); deduced Q. ⁸⁰Kr deduced mass excess. Ion implanted foil target.

doi: 10.1103/PhysRevC.34.2316
Citations: PlumX Metrics

1986FE03      Phys.Rev. C33, 1971 (1986)

M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen

One-Nucleon-Transfer Reactions Induced by 352-MeV ¹⁸O on ²⁸Si

NUCLEAR REACTIONS ²⁸Si(¹⁸O, ¹⁷O), (¹⁸O, ¹⁹F), E=352 MeV; measured σ(θ); deduced model parameters. ²⁹Si, ²⁷Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.

doi: 10.1103/PhysRevC.33.1971
Citations: PlumX Metrics

1986HO27      Phys.Lett. 181B, 38 (1986)

D.J.Horen, B.L.Burks, M.A.G.Fernandes, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, G.R.Satchler, D.Shapira, T.P.Sjoreen, F.Petrovich

Investigation of the One-Step Direct Contribution to the ²⁸Si(¹⁸O, ¹⁸F)²⁸Al Reaction at 19.6 MeV/Nucleon

NUCLEAR REACTIONS, MECPD ²⁸Si(¹⁸O, ¹⁸F), E=352 MeV; measured σ(E(¹⁸F)), σ(θ); deduced reaction mechanism. Magnetic spectrometer system, particle identification ionization chamber. Microscopic DWIA calculations.

doi: 10.1016/0370-2693(86)91250-5
Citations: PlumX Metrics

1986KA27      Nucl.Phys. A457, 15 (1986)

B.C.Karp, E.J.Ludwig, J.E.Bowsher, B.L.Burks, T.B.Clegg, F.D.Santos, A.M.Eiro

Alpha-Particle D-State and Configuration-Mixing Effects in the ⁸⁹Y(d, α)⁸⁷Sr Reaction

NUCLEAR REACTIONS ⁸⁹Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. ⁸⁹Y(polarized d, d), E=12 MeV; measured σ(θ), vector analyzing power vs θ. ⁸⁷Sr(α, α), E=19.5 MeV; measured σ(θ). ⁸⁷Sr levels deduced L, J, configuration mixing, α-particle D-state parameter. Finite range DWBA.

doi: 10.1016/0375-9474(86)90517-8
Citations: PlumX Metrics

1985BU14      Nucl.Phys. A442, 300 (1985)

B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, R.L.Varner

Spins and Parities of Low-Lying States in ⁸¹Kr from the ⁸⁰Kr(d(pol), p)⁸¹Kr Reaction and Implications for a ⁸¹Br Solar Neutrino Detector

NUCLEAR REACTIONS ⁸⁰Kr(polarized d, p), (polarized d, d), E=11 MeV; ⁸⁰Kr(polarized p, p), E=16 MeV; measured σ(θ), A(θ). ⁸¹Kr levels deduced J, π, S. Enriched gas, ion-implanted foil target. Optical model, DWBA analyses.

doi: 10.1016/0375-9474(85)90147-2
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1984BU23      Phys.Rev. C30, 742 (1984)

B.L.Burks, R.E.Anderson, Y.Aoki, B.C.Karp, E.J.Ludwig, W.J.Thompson, R.L.Varner

⁸¹Kr-⁸¹Br Ground-State Mass Difference and Implications for Calibration of a ⁸¹Br Solar Neutrino Detector

NUCLEAR REACTIONS ⁸²Kr(d, t), (d, ³He), E=17 MeV; measured σ(Et), σ(E(³He)); deduced Q-value difference. ⁸¹Kr, ⁸¹Br deduced mass difference.

doi: 10.1103/PhysRevC.30.742
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1984DE01      Nucl.Phys. A414, 113 (1984)

J.P.Delaroche, R.L.Varner, T.B.Clegg, R.E.Anderson, B.L.Burks, E.J.Ludwig, J.F.Wilkerson

Structure of Low-Lying States of ^76,78,80,82Se Deduced from (p(pol), p') Scattering at 16 MeV

NUCLEAR REACTIONS ^76,78,80,82Se(polarized p, p), (polarized p, p'), E=16 MeV; measured σ(θ), A(θ). ^76,78,80,82Se deduced deformation parameters. Coupled-channels calculations.

doi: 10.1016/0375-9474(84)90500-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0781.

1984HA22      Nucl.Phys. A419, 45 (1984)

M.Haller, W.Kretschmer, R.E.Anderson, B.L.Burks, T.B.Clegg, E.J.Ludwig, R.L.Varner, J.F.Wilkerson

Investigation of the Reactions ⁵⁸Ni(d, α)⁵⁶Co and ⁵⁰Ti(d, α)⁴⁸Sc with Vector and Tensor Polarized Deuterons

NUCLEAR REACTIONS ⁵⁸Ni, ⁵⁰Ti(d, α), E=16 MeV; measured σ(θ), relative vector, tensor analyzing power vs θ. ⁵⁶Co, ⁴⁸Sc levels deduced L-transfer, J, π. DWBA analysis.

doi: 10.1016/0375-9474(84)90284-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1640.

1982BU01      Nucl.Phys. A377, 105 (1982)

B.L.Burks, R.R.Cadmus, Jr., T.B.Clegg, E.J.Ludwig

Spins and Parities of Low-Lying States in ⁷⁹Kr from the ⁷⁸Kr(d(pol), p)⁷⁹Kr Reaction

NUCLEAR REACTIONS ⁷⁸Kr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), A(θ). ⁷⁹Kr deduced levels, J, π, S. Enriched target. DWBA, optical model analyses.

doi: 10.1016/0375-9474(82)90323-2
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1982BU03      Phys.Rev. C25, 1168 (1982)

B.L.Burks, R.E.Anderson, T.B.Clegg, H.Paetz gen.Schieck, E.J.Ludwig, R.L.Varner, J.F.Wilkerson

Test of the Polarization-Analyzing Power Equality in Two (p(pol), d) Reactions and Their Inverses

NUCLEAR REACTIONS ¹¹B(polarized p, d), E=11.34-11.94 MeV; ¹³C(polarized p, d), E=13.79-14.39 MeV; measured analyzing power vs E, θ; deduced no definitive time-reversal invariance violation.

doi: 10.1103/PhysRevC.25.1168
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