NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = V.A.Madsen Found 61 matches. 2000GR01 Nucl.Sci.Eng. 134, 77 (2000) S.M.Grimes, J.D.Anderson, R.W.Bauer, V.A.Madsen Dependence of Neutron Total Cross Sections on Energy for 100 ≤ En ≤ 500 MeV and Mass Number for 7 ≤ A ≤ 238 NUCLEAR REACTIONS Be, O, Si, Ti, Cu, Y, Sn, Ta, 197Au, Pb, Bi(n, X), E=100-500 MeV; analyzed total σ; deduced parameters.
doi: 10.13182/NSE00-A2101
1998BB08 Nucl.Sci.Eng. 130, 348 (1998) R.W.Bauer, J.D.Anderson, S.M.Grimes, D.A.Knapp, V.A.Madsen Application of a Simple Ramsauer Model for Neutron Total Cross Sections NUCLEAR REACTIONS Ca, Ti, Cu, Sn, 197Au, Pb(n, X), E=6-60 MeV; analyzed total σ; deduced parameters. Ramsauer model, global fits.
doi: 10.13182/NSE98-A2011
1998GR28 Nucl.Sci.Eng. 130, 340 (1998) S.M.Grimes, J.D.Anderson, R.W.Bauer, V.A.Madsen Justification of a Simple Ramsauer Model for Neutron Total Cross Sections NUCLEAR REACTIONS 140Ce, 208Pb(n, X), E=6-60 MeV; calculated total σ, scattering length; deduced refraction effects. Ramsauer model.
doi: 10.13182/NSE98-A2010
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
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
1995MA13 Phys.Rev. C51, 2011 (1995) Causality with Noncausal Optical Potenitals
doi: 10.1103/PhysRevC.51.2011
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
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
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
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
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
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
1989MA14 Phys.Rev. C39, 1215 (1989) Angular Momentum Dependence of the Absorptive Optical Potential NUCLEAR REACTIONS 40Ca(p, p), E not given; calculated potential parameters; deduced nonlocality projectile l dependence.
doi: 10.1103/PhysRevC.39.1215
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
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
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
1988MA41 Phys.Rev. C38, 1428 (1988) 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
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
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
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
1985OS04 Phys.Rev. C32, 108 (1985) Microscopic Calculation of the Imaginary Lane Isospin Potential W1 NUCLEAR REACTIONS 48Ca(p, n), E=25 MeV; calculated charge-exchange imaginary potential, σ(θ). Microscopic calculation.
doi: 10.1103/PhysRevC.32.108
1984DE03 Phys.Rev. C29, 1075 (1984) H.Dermawan, F.Osterfeld, V.A.Madsen Microscopic Calculation of the Imaginary Optical Potential for 208Pb(p, p) at 14 MeV NUCLEAR REACTIONS 208Pb(p, p), E=14 MeV; calculated σ(θ). Microscopic second-order imaginary potential, RPA transition densities.
doi: 10.1103/PhysRevC.29.1075
1984MA01 Phys.Rev.Lett. 52, 176 (1984) 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
1983DE12 Phys.Rev. C27, 1474 (1983) H.Dermawan, F.Osterfeld, V.A.Madsen Cross Section Calculations for Nucleon-40Ca and α-40Ca Elastic Scattering from Microscopic Nonlocal Optical Potentials NUCLEAR REACTIONS 40Ca(p, p), E=17.7, 25 MeV; 40Ca(n, n), E=17.7 MeV; 40Ca(α, α), E=31 MeV; calculated σ(θ), σ(elastic). Microscopic optical model, nonlocal potentials.
doi: 10.1103/PhysRevC.27.1474
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
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
1982DE04 Phys.Rev. C25, 180 (1982) H.Dermawan, F.Osterfeld, V.A.Madsen Nuclear Structure Approach to the Calculation of the Imaginary Alpha-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(α, α), E=31-100 MeV; calculated σ(θ), imaginary α-nucleus potential. RPA.
doi: 10.1103/PhysRevC.25.180
1982HA02 Phys.Rev. C25, 189 (1982) L.F.Hansen, I.D.Proctor, D.W.Heikkinen, V.A.Madsen Nuclear Deformation in the Actinide Region by Proton Inelastic Scattering NUCLEAR REACTIONS 232Th, 238U(p, p), (p, p'), E=26 MeV; measured σ(θ); deduced potential multipole moments. 232Th, 238U deduced β2, β4. Coupled-channels analysis.
doi: 10.1103/PhysRevC.25.189
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
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
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
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
1981OS01 Phys.Rev. C23, 179 (1981) F.Osterfeld, J.Wambach, V.A.Madsen Antisymmetrized, Microscopic Calculation for the 40Ca(n, n) Optical Potential NUCLEAR REACTIONS 40Ca(n, n), E=30 MeV; calculated σ(θ); deduced collective, intermediate charge-exchange state effects. Antisymmetrized, microscopic optical potential.
doi: 10.1103/PhysRevC.23.179
1981OS10 Phys.Rev. C24, 2468 (1981) Nuclear Structure Approach to the Coulomb Correction of the Imaginary Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=17.7, 25 MeV; calculated imaginary optical potential. RPA transition densities, inelastic, charge-exchange intermediate states.
doi: 10.1103/PhysRevC.24.2468
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
1979WA09 Nucl.Phys. A324, 77 (1979) J.Wambach, F.Osterfeld, J.Speth, V.A.Madsen Theoretical Investigation of Giant Resonances by Inelastic Proton Scattering NUCLEAR REACTIONS 16O(p, p'), E=45 MeV; 40Ca(p, p'), E=156 MeV; 208Pb(p, p'), E=60, 156 MeV; calculated σ(θ) in giant resonance region. Antisymmetrized microscopic DWBA, RPA wave functions deduced breathing mode character of giant resonance.
doi: 10.1016/0375-9474(79)90079-4
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
1978BA11 Phys.Rev. C17, 819 (1978) G.Baur, V.A.Madsen, F.Osterfeld Microscopic Theory of the Imaginary Inelastic Transition Form Factor NUCLEAR REACTIONS 40Ca(n, n'), E=30 MeV; calculated form factor.
doi: 10.1103/PhysRevC.17.819
1978WO14 Phys.Rev. C18, 2052 (1978) C.Wong, S.D.Bloom, S.M.Grimes, R.F.Hausman, Jr., V.A.Madsen Population of the 1+ Levels in 58Co via the 58Fe(p, n) Reaction NUCLEAR REACTIONS 58Fe(p, n), E=16, 19.1, 20.2 MeV; measured σ(θ). 58Co deduced 1+ strength distribution, fractional M1 strengths. Compared with reaction data, shell model calculations.
doi: 10.1103/PhysRevC.18.2052
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
1977PE09 Phys.Lett. 68B, 55 (1977) G.Perrin, D.Lebrun, J.Chauvin, P.Martin, P.De Saintignon, D.Eppel, H.V.Geramb, H.L.Yadav, V.A.Madsen The Octupole Giant Resonance Strength in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=42.5, 44.0, 49.3 MeV; measured σ(Ep', θ), A(θ). 16O deduced octupole strength.
doi: 10.1016/0370-2693(77)90033-8
1977WA13 Phys.Rev.Lett. 39, 1443 (1977) J.Wambach, V.A.Madsen, G.A.Rinker, J.Speth Has the Breathing Mode Been Known for Many Years (Question) NUCLEAR REACTIONS 208Pb(e, e'), E=90 MeV; 208Pb(α, α'), E=120 MeV; 208Pb(d, d'), E=80 MeV; calculated σ.
doi: 10.1103/PhysRevLett.39.1443
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
1975BR09 Phys.Rev. C11, 1298 (1975) 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
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
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
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
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
1973HA54 Phys.Rev. C8, 2072 (1973) L.F.Hansen, S.M.Grimes, J.L.Kammerdiener, V.A.Madsen Analysis of Inelastic Proton Scattering from 14N between 8.60 and 26.0 MeV NUCLEAR REACTIONS 14N(p, p), (p, p'), E=8.6, 10.6, 12.6, 14.6 MeV; measured σ(E, θ); θ=15-165°; coupled-channel analysis. 14N(p, p'), E=18, 21, 23, 26 MeV, previous data compared with coupled-channel calculation.
doi: 10.1103/PhysRevC.8.2072
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
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
1971WO03 Phys.Rev. C3, 1904 (1971) C.Wong, J.D.Anderson, V.A.Madsen, F.A.Schmittroth, M.J.Stomp Polarization and Angular Distribution of the Neutrons from 14C(p, n) Reaction and the Tensor Force NUCLEAR REACTIONS 14C(p, n), E=7.2-13.3 MeV; measured σ(E;θ), P(n)(E;θ); deduced integrated σ.
doi: 10.1103/PhysRevC.3.1904
1970CR03 Phys.Lett. 32B, 92 (1970) G.M.Crawley, S.M.Austin, W.Benenson, V.A.Madsen, F.A.Schmittroth, M.J.Stomp Evidence for a Tensor Effective Two-Body Interaction in the 14N(p, p') 2.31 MeV Excitation NUCLEAR REACTIONS 14N(p, p'), E=24.8 MeV; measured σ(Ep', θ).
doi: 10.1016/0370-2693(70)90594-0
1970ZI02 Phys.Lett. 33B, 205 (1970) J.Zimanyi, I.Halpern, V.A.Madsen On the Effective Charge Factor for the Radiative Capture of Fast Nucleons NUCLEAR REACTIONS 206Pb(n, γ), E=1.5-8.5 MeV; measured nothing; analyzed σ(E;Eγ). 207Pb deduced effective charge factors for levels.
doi: 10.1016/0370-2693(70)90572-1
1969AN06 Phys.Rev. 177, 1416(1969) J.D.Anderson, S.D.Bloom, C.Wong, W.F.Hornyak, V.A.Madsen Effective Two-Body Force Inferred from the (p, n) Reaction on 17O, 18O, 27Al, and Other Light Nuclei NUCLEAR REACTIONS 17,18O, 27Al(p, n), E=7-13.5 MeV; measured σ(Ep; En, θ); deduced optical-model parameters.
doi: 10.1103/PhysRev.177.1416
1968HA30 Phys.Rev. 174, 1155 (1968) L.F.Hansen, M.L.Stelts, J.G.Vidal, J.J.Wesolowski, V.A.Madsen Study of the Two-Body Force Through the (He3, t) Charge-Exchange Reaction on O17 and O18 NUCLEAR REACTIONS 17,18O(3He, t), E=17.3 MeV; measured σ(Et, θ).
doi: 10.1103/PhysRev.174.1155
1967WO05 Phys.Rev. 160, 769 (1967) C.Wong, J.D.Anderson, J.McClure, B.Pohl, V.A.Madsen, F.Schmittroth C14(p, n)N14 Reaction and the Two-Body Force NUCLEAR STRUCTURE 14N, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.160.769
1966BA11 Phys.Rev. 146, 861 (1966) N.Baron, R.F.Leonard, J.L.Need, W.M.Stewart, V.A.Madsen Inelastic Alpha-Particle Excitation in the Even Tin Isotopes NUCLEAR STRUCTURE 118Sn, 116Sn, 120Sn, 122Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.146.861
1966EC03 Phys.Rev. 141, 1067 (1966) S.F.Eccles, H.F.Lutz, V.A.Madsen Study of the Stongly Excited 2+ and 3- States in the Fe54,56 and Ni58,60,62 Isotopes by Proton Scattering at 18.6 and 19.1 MeV NUCLEAR STRUCTURE 56Fe, 54Fe, 62Ni, 60Ni, 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.141.1067
1965MA29 Phys.Rev. 139, B864 (1965) Calculation of Inelastic Alpha-Particle Scattering by Ni58 NUCLEAR STRUCTURE 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B864
1964LU06 Bull.Am.Phys.Soc. 9, No.6, 650, Q7 (1964) H.F.Lutz, S.F.Eccles, V.A.Madsen, J.B.Mason Elastic and Inelastic Scattering of 18.6-MeV Protons by Ni58, Ni60, and Ni62 NUCLEAR STRUCTURE 62Ni, 60Ni, 58Ni; measured not abstracted; deduced nuclear properties.
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