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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
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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
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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 ^{104,106,108,110}Pd(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
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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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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
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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 ^{46,47,48,49,50}Ti(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
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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
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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
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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
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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
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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
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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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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
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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 ^{116,118,120,122,124}Sn(n, n), (n, n'), E=11 MeV; analyzed σ. ^{116,118,120,122,124}Sn 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
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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 ^{144,148,150,152}Sm(p, n), E=20, 24.5, 26 MeV; measured σ(θ). ^{144,148,150,152}Eu 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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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, ^{112,116,118,120,122,124}Sn, 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)

V.R.Brown

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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