NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.M.Laymon Found 19 matches. 1998WU05 Phys.Rev. C58, 517 (1998) E.A.Wulf, M.A.Godwin, J.F.Guillemette, C.M.Laymon, R.M.Prior, B.J.Rice, M.Spraker, D.R.Tilley, H.R.Weller Astrophysical S Factors for the 9Be(p(pol), γ)10B Reaction NUCLEAR REACTIONS 9Be(polarized p, γ), E=100 keV; measured Eγ, Iγ, A(y)(θ); deduced astrophysical S-factors. HPGe detector. Direct capture plus resonance calculation.
doi: 10.1103/PhysRevC.58.517
1997GO13 Phys.Rev. C56, 1605 (1997) M.A.Godwin, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller 7Li(p(pol), γ)8Be Reaction at E(p) = 80-0 keV NUCLEAR REACTIONS, ICPND 7Li(polarized p, γ), E=0-80 keV; measured σ(θ)/A0, A(y)(θ) for capture to ground, first-, third-excited states, total σ, astrophysical S-factor for capture to third-excited state; deduced M1 resonance capture role, implications to M1 capture in 7Be(p, γ) reaction. Direct capture model, other reactions discussed.
doi: 10.1103/PhysRevC.56.1605
1997SC31 Phys.Rev. C56, 2565 (1997) G.J.Schmid, B.J.Rice, R.M.Chasteler, M.A.Godwin, G.C.Kiang, L.L.Kiang, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller The 2H(p(pol), γ)3He and 1H(d(pol), γ)3He Reactions Below 80 keV NUCLEAR REACTIONS 2H(p, γ), (polarized p, γ), 1H(d, γ), (polarized d, γ), E=10-80 keV; measured Eγ, Iγ, σ(E, θ), vector, tensor analyzing power, astrophysical S-factor, γ polarization; deduced meson exchange current, Δ-isobar effects, astrophysical implications. 3He deduced asymptotic D- to S-state ratio. Three-body calculations. Ice targets.
doi: 10.1103/PhysRevC.56.2565
1996GO01 Phys.Rev. C53, R1 (1996) M.A.Godwin, R.M.Chasteler, C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller Search for p Waves in Low-Energy Proton Capture Reactions Relevant to the Solar Neutrino Problem NUCLEAR REACTIONS, ICPND 7Li(polarized p, γ), E=0-80 keV; measured αγ-coin, A(y)(θ), σ(θ)/A0; deduced p-wave strength, astrophysical implications.
doi: 10.1103/PhysRevC.53.R1
1996LA04 Phys.Rev. C53, 1167 (1996) C.M.Laymon, W.Amos, M.G.Burlein, H.T.Fortune, T.Ekenberg, A.Kotwal, J.M.O'Donnell, J.D.Silk, J.D.Zumbro, C.L.Morris, S.J.Seestrom, K.S.Dhuga, R.Garnett, M.W.Rawool-Sullivan, C.F.Moore, S.L.Morris, D.L.Watson Pion Elastic and Inelastic 2+1 Scattering on 58,60,62,64Ni at T(π) = 180 MeV NUCLEAR REACTIONS 58,60,62,64Ni(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ); deduced nucleon radii, deformation parameters. 58,60,62,64Ni levels deduced neutron, proton matrix elements.
doi: 10.1103/PhysRevC.53.1167
1996LA10 Phys.Rev. C53, 1977 (1996) C.M.Laymon, R.M.Prior, D.R.Tilley, H.R.Weller Low-Energy Polarized-Proton Capture on 6Li NUCLEAR REACTIONS, ICPND 6Li(polarized p, γ), E ≤ 80 keV; measured Eγ, Iγ, thick target yield, analyzing power vs θ; deduced s-, p-wave relative contributions, astrophysical S-factor.
doi: 10.1103/PhysRevC.53.1977
1996SC14 Phys.Rev.Lett. 76, 3088 (1996) G.J.Schmid, M.Viviani, B.J.Rice, R.M.Chasteler, M.A.Godwin, G.C.Kiang, L.L.Kiang, A.Kievsky, C.M.Laymon, R.M.Prior, R.Schiavilla, D.R.Tilley, H.R.Weller Effects of Non-Nucleonic Degrees of Freedom in the D(p(pol), γ)3He and p(d(pol), γ)3He Reactions NUCLEAR REACTIONS, ICPND 2H(polarized p, γ), 1H(polarized d, γ), E=80 keV; analyzed σ(θ), polarization observables, astrophysical S-factor data.
doi: 10.1103/PhysRevLett.76.3088
1996SC26 Nucl.Phys. A607, 139 (1996) G.J.Schmid, R.M.Chasteler, C.M.Laymon, H.R.Weller, E.F.Moore, C.R.Bybee, J.M.Drake, D.R.Tilley, G.Vavrina, P.M.Wallace Correction Factors for γ-Ray Relative Intensities in the 66Ga Radioisotope RADIOACTIVITY 66Ga(β+), (EC); measured γ spectra; deduced relative Iγ, detector efficiency, implications to 2H(p, γ) reaction astrophysical S-factor data.
doi: 10.1016/0375-9474(96)00214-X
1995SC40 Phys.Rev. C52, R1732 (1995) G.J.Schmid, R.M.Chasteler, C.M.Laymon, H.R.Weller, R.M.Prior, D.R.Tilley Polarized Proton Capture by Deuterium and the 2H(p, γ)3He Astrophysical S Factor NUCLEAR REACTIONS, ICPND 2H(polarized p, γ), E=0-80 keV; measured Eγ, Iγ, σ(θ), analyzing power vs E; deduced astrophysical S-factor vs E.
doi: 10.1103/PhysRevC.52.R1732
1994HU02 Phys.Rev. C49, 83 (1994) P.Hui, H.T.Fortune, R.Gilman, C.M.Laymon, J.D.Zumbro, P.A.Seidl, J.A.Faucett Pion Double Charge Exchange on (nat)Se NUCLEAR REACTIONS Se(π+, π-), E=132-294 MeV; measured spectra, σ(θ) vs E; deduced double IAS excitation evidence.
doi: 10.1103/PhysRevC.49.83
1993WE13 Nucl.Instrum.Methods Phys.Res. A336, 226 (1993) S.A.Wender, S.Balestrini, A.Brown, R.C.Haight, C.M.Laymon, T.M.Lee, P.W.Lisowski, W.McCorkle, R.O.Nelson, W.Parker, N.W.Hill A Fission Ionization Detector for Neutron Flux Measurements at a Spallation Source
doi: 10.1016/0168-9002(93)91102-S
1992LA01 Phys.Rev. C45, 576 (1992);Erratum Phys.Rev. C50, 3178 (1994) C.M.Laymon, K.D.Brown, D.P.Balamuth [16O(0+2) + α] Parentage of Continuum Levels in 20Ne NUCLEAR REACTIONS 16O(α, α'), E=10.2-18 MeV; measured σ(E) vs θ. 20Ne deduced resonances, J, π, Γα.
doi: 10.1103/PhysRevC.45.576
1992LA20 Phys.Rev. C46, 1880 (1992) C.M.Laymon, R.O.Nelson, S.A.Wender, L.R.Nilsson Isovector Giant Quadrupole Resonance in the 40Ca(n, γ0) Reaction NUCLEAR REACTIONS 40Ca(n, γ), E=8-44 MeV; measured σ(θ) vs E, γ-asymmetry. 41Ca deduced isovector GQR parameters.
doi: 10.1103/PhysRevC.46.1880
1991NE07 Nucl.Instrum.Methods Phys.Res. B56/57, 451 (1991) R.O.Nelson, C.M.Laymon, S.A.Wender High-Resolution Inelastic Gamma-Ray Measurements with a White Neutron Source from 1 to 200 MeV NUCLEAR REACTIONS 56Fe(n, X), E=27.1-29 MeV; measured Eγ, Iγ for X=2n, n, np, 3n, nα. 56Fe(n, n'), (n, 2n), E ≤ 200 MeV; measured σ(θ) vs E. White neutron source.
doi: 10.1016/0168-583X(91)96068-V
1987BA71 Phys.Rev. C36, 2235 (1987) D.P.Balamuth, K.D.Brown, T.Chapuran, C.M.Laymon Properties of the E1 Giant Resonance Built on the First Excited State of 16O NUCLEAR REACTIONS 15N(p, γ), E=10-17 MeV; measured Eγ, Iγ, σ(θγ) vs E. 16O deduced giant resonance parameters.
doi: 10.1103/PhysRevC.36.2235
1987GI04 Phys.Rev. C35, 1334 (1987) R.Gilman, H.T.Fortune, J.D.Zumbro, C.M.Laymon, G.R.Burleson, J.A.Faucett, W.B.Cottingame, C.L.Morris, P.A.Seidl, C.F.Moore, L.C.Bland, R.R.Kiziah, S.Mordechai, K.S.Dhuga Mass Dependence of Pion Double Charge Exchange NUCLEAR REACTIONS 40,44Ca(π+, π-), E=163, 210 MeV; 56Fe, 58Ni(π-, π+), E=164 MeV; 56Fe(π+, π-), E=100-292 MeV; 80Se(π+, π-), E=100-190 MeV; 90Zr(π+, π-), E=164, 211 MeV; 118Sn(π+, π-), E=165, 212 MeV; measured σ(θ=5°); deduced reaction mechanism. 44Ti, 56Ni, 56Cr, 58Fe, 80Kr, 90Mo, 118Te deduced nonanalog, double analog transition differences.
doi: 10.1103/PhysRevC.35.1334
1986CH41 Phys.Rev. C34, 2358 (1986) T.Chapuran, D.P.Balamuth, W.K.Wells, C.M.Laymon, D.P.Bybell Angular Momenta of Intermediate Width Structures in 12C + 16O NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E(cm)=14.9-27.6 MeV; measured σ(E, θ), yield vs E. 28Si deduced intermediate structure, possible J, π. Legendre polynomial analysis.
doi: 10.1103/PhysRevC.34.2358
1985BA60 Phys.Rev.Lett. 55, 2842 (1985) D.P.Balamuth, T.Chapuran, C.M.Laymon, W.K.Wells, D.P.Bybell Characterization of Gross-Structure Resonances in Angular-Momentum-Mismatched Channels in Heavy-Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O'), E(cm)=17-41 MeV; measured σ(θ), mutual, single excitations. 32S deduced resonances, L, J.
doi: 10.1103/PhysRevLett.55.2842
1984BA31 Phys.Lett. 140B, 295 (1984) D.P.Balamuth, W.K.Wells, T.Chapuran, D.P.Bybell, C.M.Laymon Failure of the Molecular Core-Particle Coupling Model in 13C + 13C Inelastic Scattering NUCLEAR REACTIONS 13C(13C, 13C'), E(cm)=8-25 MeV; measured σ(θ); deduced intermediate states role, molecular particle-core coupling model inadequacy. Single, mutual inelastic excitation.
doi: 10.1016/0370-2693(84)90756-1
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