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Search: Author = V.R.Brown

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2003BR21      Eur.Phys.J. A 18, 289 (2003)

V.R.Brown, B.F.Gibson, J.A.Carlson, R.Schiavilla

Parity non-conservation in proton-proton elastic scattering

NUCLEAR REACTIONS 1H(polarized p, p), E=0-350 MeV; calculated parity-non-conserving longitudinal asymmetry.

doi: 10.1140/epja/i2002-10218-2
Citations: PlumX Metrics

2002CA15      Phys.Rev. C65, 035502 (2002)

J.Carlson, R.Schiavilla, V.R.Brown, B.F.Gibson

Parity-Violating Interaction Effects: The longitudinal asymmetry in pp elastic scattering

NUCLEAR REACTIONS 1H(p, p), E=0-350 MeV; calculated parity-violating longitudinal asymmetry; deduced reaction mechanism features. Comparisons with data.

doi: 10.1103/PhysRevC.65.035502
Citations: PlumX Metrics

1997MA34      Phys.Rev. C56, 365 (1997)

V.A.Madsen, J.D.Anderson, S.M.Grimes, V.R.Brown, P.M.Anthony

Minimum in the Forward Angle Quasielastic (p, n) Cross Section: A means of detecting rapid variations in the forward scattering amplitudes

NUCLEAR REACTIONS 90,91,92,94Zr(p, n), E=18, 25 MeV; analyzed reaction σ(θ). 140Ce(n, X), E=5-40 MeV; analyzed σ(total). DWBA calaculations, Ramsauer, nuclear surface effects.

doi: 10.1103/PhysRevC.56.365
Citations: PlumX Metrics

1996GR07      Phys.Rev. C53, 2709 (1996)

S.M.Grimes, R.W.Bauer, J.D.Anderson, V.R.Brown, B.A.Pohl, C.H.Poppe, V.A.Madsen, R.Langkau, W.Scobel, S.Stamer

Low-Lying Gamow-Teller States in 92Nb

NUCLEAR REACTIONS 90,92Zr(p, n), E=26 MeV; measured σ(E, θ). 90,92Nb levels deduced Gamow-Teller strength. Quasi-particle, shell models, RPA.

doi: 10.1103/PhysRevC.53.2709
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1993HO02      Phys.Rev. C47, 629 (1993)

D.J.Horen, R.L.Auble, J.Gomez del Campo, G.R.Satchler, R.L.Varner, J.R.Beene, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen

Systematics of Isospin Character of Transitions to the 2+1 and 3-1 States in 90,92,94,96Zr

NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li), (6Li, 6Li'), E=70 MeV; measured σ(θ); deduced model parameters. 90,92,94,96Zr levels deduced B(λ), neutron, proton matrix element ratio. Deformed optical model, folding model analyses.

doi: 10.1103/PhysRevC.47.629
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1176.

1993KO53      Nucl.Instrum.Methods Phys.Res. B79, 297 (1993)

J.E.Koster, R.O.Nelson, M.E.Schillaci, S.A.Wender, D.Mayo, F.P.Brady, J.Romero, D.Krofcheck, M.Blann, P.Anthony, V.R.Brown, L.Hansen, B.Pohl, T.C.Sangster, H.Nifenecker, J.A.Pinston

Neutron-Proton Bremsstrahlung Experiments

NUCLEAR REACTIONS 1H(n, γ), E=138-401 MeV; measured γ rays. Tof techniques.

doi: 10.1016/0168-583X(93)95348-9
Citations: PlumX Metrics

1993MA15      Phys.Rev. C47, 2077 (1993)

V.A.Madsen, R.W.Bauer, J.D.Anderson, V.R.Brown, B.A.Pohl, C.H.Poppe, S.Stamer, E.Mordhorst, W.Scobel, S.M.Grimes

Theoretical Treatment of Analog (p, n) Cross Sections for Odd Nuclei: Application to measurements of 105Pd at 26 MeV

NUCLEAR REACTIONS 105Pd(p, n), E=26 MeV; measured σ(θ), neutron spectra. 105Ag deduced IAS excitation mechanism. Model comparison.

doi: 10.1103/PhysRevC.47.2077
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1992HO12      Phys.Lett. 296B, 18 (1992)

D.J.Horen, R.L.Auble, J.Gomez del Campo, R.L.Varner, J.R.Beene, G.R.Satchler, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen

Different Effects of Valence Neutrons on the Isospin Character of Transitions to the First 2+ and 3- States of 90,92,94,96Zr

NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li'), E=70 MeV; measured σ(θ). 90,92,94,96Zr levels deduced neutron, proton matrix element ratio.

doi: 10.1016/0370-2693(92)90797-8
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1991BR18      Phys.Rev. C44, 1296 (1991)

V.R.Brown, P.L.Anthony, J.Franklin

Proton-Proton Bremsstrahlung Calculations at 280 MeV

NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated σ(θ1, θ2, θγ), analyzing power.

doi: 10.1103/PhysRevC.44.1296
Citations: PlumX Metrics

1991HO13      Phys.Rev. C44, 128 (1991)

D.J.Horen, R.L.Auble, J.R.Beene, F.E.Bertrand, M.L.Halbert, G.R.Satchler, M.Thoennessen, R.L.Varner, V.R.Brown, P.L.Anthony, V.A.Madsen

Isospin Character of Transitions to Bound States in 204,206,208Pb using Inelastic Scattering of 17O Ions

NUCLEAR REACTIONS 204,206,208Pb(17O, 17O'), E=375 MeV; measured σ(θ); deduced optical model parameters. 204,206,208Pb levels deduced B(λ), neutron, proton matrix element ratio. Enriched targets. DWBA analysis.

NUCLEAR STRUCTURE 204,206,208Pb; calculated B(λ), neutron, proton matrix element ratio. RPA method.

doi: 10.1103/PhysRevC.44.128
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1990AN10      Phys.Rev. C41, 1993 (1990)

J.D.Anderson, V.R.Brown, R.W.Bauer, B.A.Pohl, C.H.Poppe, S.Stamer, E.Mordhorst, W.Scobel, S.M.Grimes, V.A.Madsen

Analog (p, n) Cross Sections of Even-Even Palladium Isotopes at 26 MeV

NUCLEAR REACTIONS, ICPND 104,106,108,110Pd(p, n), E=26 MeV; measured σ(θ); deduced σ for analog states. Coupled-channels analyses.

doi: 10.1103/PhysRevC.41.1993
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2393.

1989HJ01      Phys.Rev.Lett. 62, 870 (1989)

E.L.Hjort, F.P.Brady, J.L.Romero, J.R.Drummond, M.A.Hamilton, B.McEachern, R.D.Smith, V.R.Brown, F.Petrovich, V.A.Madsen

Pb(n, n'X) at 65 MeV and the Isospin Structure of the Giant Quadrupole Resonance Region

NUCLEAR REACTIONS 208Pb(n, n'X), E=65 MeV; measured σ(θn, En). 208Pb deduced GQR isospin structure. Other data input.

doi: 10.1103/PhysRevLett.62.870
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13509.

1989MA44      Phys.Rev. C40, 1999 (1989)

V.A.Madsen, L.F.Hansen, V.R.Brown, D.G.Madland

Correction for Truncation in Coupled-Channels Optical Potentials

NUCLEAR REACTIONS 238U(n, n'), E=1, 4, 8 MeV; 238U(p, p'), E=18, 26 MeV; calculated σ. Coupled-channels formalism, truncation.

doi: 10.1103/PhysRevC.40.1999
Citations: PlumX Metrics

1988AN11      Phys.Rev. C38, 1601 (1988)

J.D.Anderson, R.W.Bauer, V.R.Brown, S.M.Grimes, V.A.Madsen, B.A.Pohl, C.H.Poppe, W.Scobel

Analog (p, n) Cross Sections of the Zirconium Isotopes at 18 and 25 MeV

NUCLEAR REACTIONS, ICPND 90,91,92,94Zr(p, n), E=18, 25 MeV; measured σ(θ); deduced reaction mechanism. 90,91,92,93Nb deduced analog excitation σ. 91Zr(p, n), E ≈ 12-40 MeV; analyzed σ(E).

doi: 10.1103/PhysRevC.38.1601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0027.

1988BR09      Phys.Rev. C37, 1539 (1988)

V.R.Brown, J.A.Carr, V.A.Madsen, F.Petrovich

Isospin Distribution of Quadrupole Strength in 118Sn: Comparison with pion, nucleon, and electron scattering

NUCLEAR REACTIONS 118Sn(π+, π+'), (π-, π-'), E=130 MeV; 118Sn(p, p'), E=24.5 MeV; 118Sn(n, n'), E=11 MeV; calculated σ(θ). 118Sn deduced quadrupole transition strength isospin features. Quasiparticle RPA.

doi: 10.1103/PhysRevC.37.1539
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1988MA41      Phys.Rev. C38, 1428 (1988)

V.A.Madsen, V.R.Brown

Sharing of Collective Multipole Strength in the Nuclear Particle-Hole Model

NUCLEAR STRUCTURE 118Sn; calculated giant quadrupole states, isocalar, isovector strength distributions. Particle-hole model.

doi: 10.1103/PhysRevC.38.1428
Citations: PlumX Metrics

1986BR03      Phys.Rev. C33, 1235 (1986)

V.R.Brown, C.Wong, C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, V.A.Madsen

Cross Sections for the Ti(p, n) Reaction to Analogs of Ground and 2+ Excited States

NUCLEAR REACTIONS, ICPND 46,47,48,49,50Ti(p, n), E=11.5-26 MeV; measured σ(En), σ(θ); deduced σ, β(n)/β(p). 46,48,50Ti levels deduced β.

doi: 10.1103/PhysRevC.33.1235
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0098.

1986SM02      Phys.Rev. C33, 847 (1986)

R.D.Smith, V.R.Brown, V.A.Madsen

Isovector Deformation Parameters from Coupled-Channel Analysis of (p, n) Reactions

NUCLEAR REACTIONS 54,55Fe(p, n), (p, p'), E=35 MeV; 54,55Fe(n, n), (n, n'), E=26 MeV; calculated σ(θ); deduced reaction mechanism. 54,56Fe deduced isovector deformation parameter. Lane model, optical potential, vibrational model couplings.

doi: 10.1103/PhysRevC.33.847
Citations: PlumX Metrics

1985BR20      Phys.Lett. 164B, 217 (1985)

V.R.Brown, A.M.Bernstein, V.A.Madsen

The Reversal Effect for Neutron and Proton Multipole Matrix Elements in Higher 2+ Transitions

NUCLEAR STRUCTURE 118Sn, 54Fe, 90Zr, 208Pb; calculated 2+ multipole neutron, proton matrix elements; deduced spin-orbit intruder role. RPA.

doi: 10.1016/0370-2693(85)90312-0
Citations: PlumX Metrics

1984BR03      J.Phys.(London) G10, 363 (1984)

F.P.Brady, G.A.Needham, J.L.Ullmann, C.M.Castaneda, T.D.Ford, N.S.P.King, J.L.Romero, M.L.Webb, V.R.Brown, C.H.Poppe

Excitation of Analogue Isovector Resonances via the (n, p) Reaction at 60 MeV

NUCLEAR REACTIONS 6,7Li, 12C, 16O, 28Si, 58,60,62,64Ni, 209Bi(n, p), E=60 MeV; measured σ(θ); deduced effective nucleon-nucleon interaction isovector spin-dependent component, analog isovector resonance excitation mechanism. 28Al deduced Gamow-Teller type transition. 7He deduced L=1 dipole strength contribution. 6He, 12B deduced L=1 strength spin character, Gamow-Teller type transition. 16N deduced L=1 strength spin character.

doi: 10.1088/0305-4616/10/3/011
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12784.

1984MA01      Phys.Rev.Lett. 52, 176 (1984)

V.A.Madsen, V.R.Brown

Schematic Model for the Differences between Neutron and Proton Quadrupole Deformation Parameters in Open-Shell Nuclei

NUCLEAR STRUCTURE 88,86,76Sr; calculated neutron, proton quadrupole deformation parameter, matrix element ratios. Se, Sr, Zr, Mo, Cd, Sn, Te, Ba, Ce, Sm; calculated neutron, proton quadrupole deformation parameter ratio. Schematic model, open shell nuclei.

doi: 10.1103/PhysRevLett.52.176
Citations: PlumX Metrics

1983BR03      Phys.Rev.Lett. 50, 658 (1983)

V.R.Brown, S.Krewald, J.Speth

Crucial Test for the Δ(1232)-Hole Effect: (n, p) vs (p, n)

NUCLEAR REACTIONS 208Pb(n, p), E not given; calculated σ(θ); deduced isobar-hole state role in charge exchange process. Born approximation.

doi: 10.1103/PhysRevLett.50.658
Citations: PlumX Metrics

1983MA17      Phys.Lett. 123B, 13 (1983)

V.A.Madsen, T.Suzuki, A.M.Bernstein, V.R.Brown

Neutron and Proton Multipole Matrix Elements in 48Ca and 208Pb

NUCLEAR STRUCTURE 48Ca, 208Pb; calculated neutron, proton multipole matrix element ratios. RPA.

doi: 10.1016/0370-2693(83)90947-4
Citations: PlumX Metrics

1983MI25      Phys.Lett. 131B, 26 (1983)

R.A.Miskimen, A.M.Bernstein, B.Quinn, S.A.Wood, M.V.Hynes, G.S.Blanpied, B.G.Ritchie, V.R.Brown

DWIA Predictions of (p, p') Data using Electromagnetically Constrained Densities

NUCLEAR REACTIONS 28,30Si, 34S, 40,42Ca(polarized p, p'), E=650 MeV; measured σ(θ). 24,26Mg(polarized p, p'), E=800 MeV; analyzed σ(θ). DWIA, proton, neutron transition densities, electromagnetic constraints.

doi: 10.1016/0370-2693(83)91084-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0691.

1982BE32      Phys.Rev.Lett. 49, 451 (1982)

A.M.Bernstein, R.A.Miskimen, B.Quinn, S.A.Wood, M.V.Hynes, G.S.Blanpied, B.G.Ritchie, V.R.Brown

Determination of Relative Signs of Neutron and Proton Transition Matrix Elements: Strong cancellation observed for the 34S(O+ → 22+) transition

NUCLEAR REACTIONS 34S, 42Ca(polarized p, p'), E=650 MeV; 30Si(polarized p, p'), E=650, 800 MeV; measured σ(θ). 26Mg, 30Si, 42Ca, 34S deduced neutron, proton transition matrix element relative sign.

doi: 10.1103/PhysRevLett.49.451
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0772.

1982BR24      Phys.Rev. C26, 2247 (1982)

B.A.Brown, B.H.Wildenthal, W.Chung, S.E.Massen, M.Bernas, A.M.Bernstein, R.Miskimen, V.R.Brown, V.A.Madsen

Isovector E2 Matrix Elements from Electromagnetic Transitions in the s-d shell: Experiment and shell-model calculations.

NUCLEAR STRUCTURE A=17-39; calculated B(E2) for isovector transitions; deduced isovector effective charge. Shell model.

doi: 10.1103/PhysRevC.26.2247
Citations: PlumX Metrics

1982WO06      Phys.Rev. C26, 889 (1982)

C.Wong, S.M.Grimes, C.H.Poppe, V.R.Brown, V.A.Madsen

Excitation of 0+, 2+, (0+)', (2+)', 4+ Analog States in the Even Selenium Isotopes with 19-25 MeV Protons; Coupled-channel analysis

NUCLEAR REACTIONS 76,80,82Se(p, n), E=19, 20, 22, 25 MeV; measured σ(En), σ(θ). 76,80,82Br deduced analog excitation mechanism. Coupled-channels calculation.

doi: 10.1103/PhysRevC.26.889
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0524.

1981BE31      Phys.Lett. 103B, 255 (1981)

A.M.Bernstein, V.R.Brown, V.A.Madsen

Neutron and Proton Transition Matrix Elements and Inelastic Hadron Scattering

NUCLEAR STRUCTURE 26Mg, 48Ca, 208Pb; calculated neutron, proton transition matrix element ratio. Inelastic hadron scattering, electromagnetic transition rate input.

doi: 10.1016/0370-2693(81)90219-7
Citations: PlumX Metrics

1981BE49      Phys.Lett. 106B, 259 (1981)

A.M.Bernstein, V.R.Brown, V.A.Madsen

The Variation of βR with Probe in Inelastic Hadron Scattering and the Adequacy of First-Order Calculations

NUCLEAR REACTIONS 116Sn, 90Zr, 58Ni(p, p'), E=800 MeV, 1.047 GeV; 116Sn, 90Zr, 58Ni(π, π'), E=162 MeV; 116Sn, 90Zr, 58Ni(α, α'), E=65 MeV; analyzed data; deduced probe dependence of deformation length. Brown-Madsen, schematic models.

doi: 10.1016/0370-2693(81)90530-X
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1981BR23      Phys.Rev. C24, 2359 (1981)

V.R.Brown, C.Wong, S.M.Grimes, C.H.Poppe, V.A.Madsen

Comment on ' Isospin and Strong-Coupling Effects in Neutron Scattering from Even-A Se Isotopes '

NUCLEAR REACTIONS 76,80,82Se(n, n), (n, n'), E=8 MeV; calculated σ(θ); deduced isospin optical model parameters. 76,80,82Se level deduced deformation parameters. Coupled-channels analysis.

doi: 10.1103/PhysRevC.24.2359
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1979FI04      Phys.Lett. 84B, 169 (1979)

R.W.Finlay, J.Rapaport, V.R.Brown, V.A.Madsen, J.R.Comfort

Isovector Deformation Parameters and Core Polarization

NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n), (n, n'), E=11 MeV; analyzed σ. 116,118,120,122,124Sn levels deduced T=0, T=1, quadrupole deformation parameters. Shell-model interpretation, core polarization of valence neutrons.

doi: 10.1016/0370-2693(79)90275-2
Citations: PlumX Metrics

1979WO05      Phys.Rev. C20, 59 (1979)

C.Wong, V.R.Brown, V.A.Madsen, S.M.Grimes

(p, n) Reaction to Ground- and Excited-State Analogs on the Samarium Isotopes: Importance of Two-Phonon Coupling Effects

NUCLEAR REACTIONS 144,148,150,152Sm(p, n), E=20, 24.5, 26 MeV; measured σ(θ). 144,148,150,152Eu deduced analog states, deformation parameters. One-, two-phonon coupled channels calculations.

doi: 10.1103/PhysRevC.20.59
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1977BE54      Phys.Lett. 71B, 48 (1977)

A.M.Bernstein, V.R.Brown, V.A.Madsen

Explanation of the Near Equality of Isoscalar and Electromagnetic Transition Rates in Neutron-Excess Nuclei: Comparison with Data

NUCLEAR STRUCTURE 42,44Ca, 58,60,62,64Ni, 116,118,120Sn, 206Pb, 50Ti, 52Cr, 54Fe, 88Sr, 90Zr, 92Mo, 138Ba, 140Ce, 144Sm; calculated ratios of isoscalar, electromagnetic transition rates to lowest 2+ level.

doi: 10.1016/0370-2693(77)90736-5
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1976MA07      Phys.Rev. C13, 548 (1976)

V.A.Madsen, V.R.Brown, S.M.Grimes, C.H.Poppe, J.D.Anderson, J.C.Davis, C.Wong

Effect of Inelastic Coupling on 0+ Analog Transitions

NUCLEAR REACTIONS 92,98,100Mo(p, n), E=18, 22, 26 MeV; measured σ(θ). 92,98,100Mo(p, n), E=16, 26 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.13.548
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0285.

1975BR09      Phys.Rev. C11, 1298 (1975)

V.R.Brown, V.A.Madsen

Core Polarization in Inelastic Scattering and Effective Charges

NUCLEAR REACTIONS 207Pb, 118Sn(α, α'), (p, p'), (n, n'); measured core polarization effect.

doi: 10.1103/PhysRevC.11.1298
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1975MA35      Phys.Rev. C12, 1205 (1975)

V.A.Madsen, V.R.Brown, J.D.Anderson

Differences of Deformation Parameter β for Different Transition Mechanisms; Comparison with Data

NUCLEAR STRUCTURE 40Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 88Sr, 90Zr, 92Mo, 112,116,118,120,122,124Sn, 138Ba; calculated deformation parameters β.

doi: 10.1103/PhysRevC.12.1205
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1975WO01      Phys.Rev. C11, 137 (1975)

C.Wong, V.R.Brown, J.D.Anderson, J.C.Davis, S.M.Grimes, C.H.Poppe, V.A.Madsen

Population of Analogs of Excited States in 63Cu(p, n) at 16, 19, and 22 MeV

NUCLEAR REACTIONS 63Cu(p, n), E=16, 19, 22 MeV; 64Zn(p, n), E=22 MeV; measured σ(En, θ). 63Zn deduced analog states.

doi: 10.1103/PhysRevC.11.137
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1975WO11      Phys.Rev. C12, 2115 (1975)

C.Wong, J.D.Anderson, V.R.Brown, J.C.Davis, S.M.Grimes, V.A.Madsen, C.H.Poppe

Excited Analogs in 62Ni and 63Cu(p, n) and the Weak-Coupling Model

NUCLEAR REACTIONS 62Ni(p, n), E=16, 19, 22 MeV; measured σ(θ) ground-state, excited-state analog; calculated σ(θ) using weak-coupling model.

doi: 10.1103/PhysRevC.12.2115
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0123.

1974MA07      Phys.Rev. C9, 1253 (1974)

V.A.Madsen, J.D.Anderson, V.R.Brown

Sensitivity of the Small-Angle Charge-Exchange Polarization-Transfer Reaction to Spin-Flip Forces

NUCLEAR REACTIONS 15N, 11B(p, n), E=16-28 MeV; calculated σ(E).

doi: 10.1103/PhysRevC.9.1253
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1972BR36      Phys.Rev. C6, 1110 (1972)


Proton-Proton Bremsstrahlung Calculations at Unequal Angles in the Coplanar Geometry

NUCLEAR REACTIONS 1H(p, p'γ), E=156 MeV; calculated σ(θ(p1), θ(p2), θ(γ)). Bryan-Scott, Hamada-Johnston potentials.

doi: 10.1103/PhysRevC.6.1110
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1972MA04      Phys.Rev.Lett. 28, 629 (1972)

V.A.Madsen, M.J.Stomp, V.R.Brown, J.D.Anderson, L.Hansen, C.Wong, J.J.Wesolowski

Channel-Coupling Effects in Analog Charge-Exchange Reactions

NUCLEAR REACTIONS 26Mg, 56Fe(p, n), E=17.4, 18 MeV; measured σ(θ); deduced two-step mechanism, channel-coupling effects.

doi: 10.1103/PhysRevLett.28.629
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1971MA06      Phys.Rev.Lett. 26, 454 (1971)

V.A.Madsen, V.R.Brown, F.Becchetti, G.W.Greenlees

Core-Polarization Effects in Charge-Exchange Reactions; Application to 58Ni(3He, t)

NUCLEAR REACTIONS 58Ni(3He, t), E=24.6 MeV; measured σ(θ); analyzed data using DWBA with tensor force.

doi: 10.1103/PhysRevLett.26.454
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