NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Hayward Found 31 matches. 1994GO17 Phys.Rev. C50, 1528 (1994) M.A.Godwin, E.Hayward, G.Feldman, L.H.Kramer, H.R.Weller, W.R.Dodge Isovector Giant Quadrupole Resonance Observed in 89Y(p(pol), γ)90Zr NUCLEAR REACTIONS 89Y(polarized p, γ), E=18.5-28.5 MeV; measured Eγ, Iγ(θ), analyzing power (θ=90°) vs Ep; deduced model parameters. 90Zr deduced giant quadrupole resonances, widths, E2 strength distribution features.
doi: 10.1103/PhysRevC.50.1528
1993KR06 Phys.Lett. 304B, 208 (1993) L.H.Kramer, R.M.Chasteler, E.Hayward, R.M.Prior, D.R.Tilley, H.R.Weller Observation of p-Wave Capture Strength in the 2H(d(pol), γ)4He Reaction at E(d) = 80-0 KeV NUCLEAR REACTIONS 2H(polarized d, γ), E=80 keV; measured σ(θ), vector, tensor analyzing power vs θ; deduced p-wave capture dominance. Model comparison.
doi: 10.1016/0370-2693(93)90284-O
1993WH03 Phys.Rev. C48, 2355 (1993) R.M.Whitton, H.R.Weller, E.Hayward, W.R.Dodge, S.E.Kuhn 2H(d, γ)4He Polarization Observables at 20, 30, and 50 MeV NUCLEAR REACTIONS 2H(d, γ), E=30 MeV; measured σ(θ). 2H(polarized d, γ), E=20-50 MeV; measured tensor, vector analyzing power vs θ, σ(θ). 4He deduced D-state probability, two-deuteron component. Model analysis.
doi: 10.1103/PhysRevC.48.2355
1992FU06 Nucl.Phys. A548, 579 (1992) K.Fuhrberg, G.Martin, D.Hager, M.Ludwig, M.Schumacher, B.-E.Andersson, K.I.Blomqvist, H.Ruijter, A.Sandell, B.Schroder, E.Hayward, L.Nilsson, R.Zorro Compton Scattering by Mesons in Nuclei: Experiment on 208Pb NUCLEAR REACTIONS 208Pb(γ, γ), E=58, 73 MeV; measured σ(θ) for elastic photon scattering, θ from 60° to 150°. Predicted exchange seagull amplitudes are compared with experimental data, Compton scattering by mesons in nuclei.
doi: 10.1016/0375-9474(92)90643-X
1992LU01 Phys.Lett. 274B, 275 (1992) M.Ludwig, B.-E.Andersson, A.Baumann, K.I.Blomqvist, K.Fuhrberg, E.Hayward, G.Miller, D.Nilsson, A.Sandell, B.Schroder, M.Schumacher Electromagnetic Polarizabilities of Nucleons Bound in 12C and 16O NUCLEAR REACTIONS 12C, 16O(γ, γ), E=61, 77 MeV; measured σ(θ), Compton scattering; deduced bound nucleon electromagnetic polarizabilities.
doi: 10.1016/0370-2693(92)91986-J
1991FE01 Phys.Rev. C43, 223 (1991) G.Feldman, L.H.Kramer, H.R.Weller, E.Hayward, W.R.Dodge Isovector Giant Quadrupole Resonance Observed in 30Si(p(pol), γ)31P NUCLEAR REACTIONS 30Si(polarized p, γ), E=20-36 MeV; measured σ(θ), analyzing power vs θ. 31P deduced isovector GQR, parameters.
doi: 10.1103/PhysRevC.43.223
1989HA16 Phys.Lett. 223B, 133 (1989) On the Polarizability of the Proton NUCLEAR REACTIONS 1H(γ, X), E ≈ 200-1200 MeV; calculated electric, magneitc dipole, total σ(E), polarizabilities.
doi: 10.1016/0370-2693(89)90227-X
1988WE15 Phys.Lett. 213B, 413 (1988) H.R.Weller, R.M.Whitton, J.Langenbrunner, E.Hayward, W.R.Dodge, S.Kuhn, D.R.Tilley The Energy Dependence of Polarization Observables in the 2H(d, γ)4He Reaction NUCLEAR REACTIONS 2H(polarized d, γ), E=0.3-50 MeV; measured γ-spectra, tensor, vector analyzing power vs E.
doi: 10.1016/0370-2693(88)91283-X
1985DO15 Phys.Rev. C32, 781 (1985) W.R.Dodge, E.Hayward, M.N.Martins, E.Wolynec (e, p) and (e, α) Reactions in 90Zr and 92Zr NUCLEAR REACTIONS 92,90Zr(e, p), (e, α), E=20-130 MeV; measured σ(θp, Ep), σ(θα, Eα), proton, α yields; deduced σ(γ, p), σ(γ, α). Enriched targets. DWBA, virtual photon spectra.
doi: 10.1103/PhysRevC.32.781
1984HA08 Nucl.Phys. A414, 333 (1984) Photon Scattering from 12C and 208Pb in the Δ-Region NUCLEAR REACTIONS 12C, 208Pb(γ, γ), E=150-400 MeV; measured σ(E, θ=115°).
doi: 10.1016/0375-9474(84)90606-7
1984MA53 Phys.Rev. C30, 1855 (1984) M.N.Martins, E.Hayward, G.Lamaze, X.K.Maruyama, F.J.Schima, E.Wolynec Experimental Test of the Bremsstrahlung Cross Section NUCLEAR REACTIONS 63Cu(e, n), E=13.5-60 MeV; measured electrodisintegration σ(E); deduced bremsstrahlung σ(E), σ(γ, n). Activation technique, thin Cu, Mo, Ta, Th radiators. Virtual photon theory.
doi: 10.1103/PhysRevC.30.1855
1983DO05 Phys.Rev. C28, 8 (1983) W.R.Dodge, E.Hayward, R.G.Leicht, M.McCord, R.Starr Nuclear Photon Scattering by 12C and 16O NUCLEAR REACTIONS 12C(γ, γ), E=23.5-39 MeV; 16O(γ, γ), E=25-39 MeV; measured σ(E). 12C(γ, γ'), E=23.5 MeV; measured σ(θ). 16O deduced EWSR isoscalar, isovector E2 strength, photonuclear absorption σ. 12C deduced EWSR isoscalar, isovector E2 strength, Γγ1/Γγ0, photonuclear absorption σ.
doi: 10.1103/PhysRevC.28.8
1983DO06 Phys.Rev. C28, 150 (1983) W.R.Dodge, E.Hayward, E.Wolynec Experimental Test of Virtual Photon Theory NUCLEAR REACTIONS 90Zr(e, p), E=17-105 MeV; measured σ(θp, Ep); deduced E1 virtual photon spectrum, nuclear size effects. 90Zr deduced IAS decay, parameters Γp0Γγ/Γ, Γγ, Γp2/Γp0.
doi: 10.1103/PhysRevC.28.150
1983OC01 Phys.Rev. C27, 2492 (1983) J.S.O'Connell, E.Hayward, J.W.Lightbody, Jr., X.K.Maruyama, P.Bosted, K.I.Blomqvist, G.Franklin, J-O.Adler, K.Hansen, B.Schroder Total Nuclear Inelastic Electron Scattering Cross Sections Compared to Sum Rule Calculations NUCLEAR REACTIONS 9Be, 12C, 27Al, 51V, 90Zr, 181Ta(e, e'), E=200-350 MeV; measured σ(θ, E(e')); deduced longitudinal response function.
doi: 10.1103/PhysRevC.27.2492
1981DO12 Phys.Rev. C24, 1952 (1981) W.R.Dodge, R.G.Leicht, E.Hayward, E.Wolynec Electrodisintegration of 56Fe, 59Co and 64Zn NUCLEAR REACTIONS 56Fe, 59Co, 64Zn(e, p), (e, α), E=16-100 MeV; measured σ(θ, Ep), σ(θ, Eα); deduced σ(γ, p), σ(γ, α). 56Fe, 59Co, 64Zn deduced integrated E1 transition strength. DWBA, virtual photons.
doi: 10.1103/PhysRevC.24.1952
1980DO04 Phys.Rev.Lett. 44, 1040 (1980) W.R.Dodge, E.Hayward, R.G.Leicht, B.H.Patrick, R.Starr E2 Strength in 12C Determined by Elastic Photon Scattering NUCLEAR REACTIONS 12C(γ, γ), E=23.5-39 MeV; measured σ. 12C deduced E2 strength.
doi: 10.1103/PhysRevLett.44.1040
1980WO04 Phys.Rev. C22, 1012 (1980) E.Wolynec, W.R.Dodge, R.G.Leicht, E.Hayward Electrodisintegration of 58Ni, 60Ni, and 62Ni NUCLEAR REACTIONS 58,60,62Ni(e, α), (e, p), E=16-100 MeV; measured σ(E, θp, Ep), σ(E, θα, Eα). 58,60,62Ni deduced integrated photoproduction σ. DWBA, virtual E1, E2 photons.
doi: 10.1103/PhysRevC.22.1012
1979WO01 Phys.Rev.Lett. 42, 27 (1979) E.Wolynec, W.R.Dodge, E.Hayward Decay Modes of Giant Resonances in 58Ni, 60Ni, and 62Ni NUCLEAR REACTIONS 58,60,62Ni(e, p), 58,60,62Ni(e, α), E=16-50 MeV; measured particle spectra, σ; deduced photodisintegration σ. 58,60,62Ni deduced resonance parameters for E1, E2 components.
doi: 10.1103/PhysRevLett.42.27
1978DO12 Phys.Rev. C18, 2435 (1978) W.R.Dodge, E.Hayward, G.Moscati, E.Wolynec Electrodisintegration of 238U NUCLEAR REACTIONS 238U(e, α), 238U(e, p), E=40 MeV; measured σ(Ep), σ(Eα); deduced ternary fission cross section.
doi: 10.1103/PhysRevC.18.2435
1978KL03 Phys.Rev. C17, 1531 (1978) Electrodisintegration of 12C NUCLEAR REACTIONS 12C(e, n), E=30 MeV; measured absolute σ(n).
doi: 10.1103/PhysRevC.17.1531
1974HA64 Phys.Rev. C10, 2652 (1974) E.Hayward, W.C.Barber, J.J.McCarthy Nuclear Scattering of Plane-Polarized Photons NUCLEAR REACTIONS Cd, In, Sn, Sb, Nd, Ta, W, Pt, Au, Hg, Pb, Bi, Th, U(polarized γ, γ), (polarized γ, γ'), E=15.1 MeV; measured σ.
doi: 10.1103/PhysRevC.10.2652
1973HA38 Phys.Rev. C8, 1065 (1973) E.Hayward, W.C.Barber, J.Sazama Nuclear Scattering of Plane-Polarized Photons NUCLEAR REACTIONS Cd, Sn, 181Ta, W, Pt, 197Au, 209Bi(polarized γ, γ'), E=20 MeV; measured σ.
doi: 10.1103/PhysRevC.8.1065
1972HA16 Phys.Rev. C5, 846 (1972) E.Hayward, B.F.Gibson, J.S.O'Connell Consequences of Isospin Sum Rules for Photonuclear Reactions NUCLEAR REACTIONS 3He, 13C, 26Mg, 48Ti, 52Cr, 64Zn, 58,60,62,64Ni, 74Ge, 90Zr, 108Pd, 112Cd, 120Sn, 208Pb(γ, X), E < 30 MeV; calculated bremsstrahlung-weighted σ.
doi: 10.1103/PhysRevC.5.846
1970HA28 Phys.Rev. C2, 761 (1970) E.Hayward, R.B.Schwartz, K.M.Murray Comments on 'Isospin of the B11 Giant Resonance' NUCLEAR REACTIONS 11B(γ, Xγ), E not given; measured nothing; reinterpreted data. 11B deduced nothing on T-splitting of giant resonance.
doi: 10.1103/PhysRevC.2.761
1965HA19 Nucl.Phys. 69, 241 (1965) Photoneutron Production by Li6, Li7, B10, B11 and O16 NUCLEAR REACTIONS 6Li, 7Li, 10B, 11B, 16O(γ, xn), Eγ approx 6-30 MeV; measured activation curve using bremsstrahlung, obtained σ(E) with Δ E = 0.5, 1.0 MeV.
doi: 10.1016/0029-5582(65)90049-0
1962FU08 Nuclear Phys. 30, 613 (1962) The Nuclear Photoeffect in Holmium and Erbium
doi: 10.1016/0029-5582(62)90081-0
1962FU18 Nuclear Phys. 33, 431 (1962) The Photodisintegration of Bismuth and the Lead Isotopes NUCLEAR STRUCTURE 209Bi, 208Pb, 206Pb, 207Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90536-9
1960FU08 Contrib.Karlsruhe Photonuclear Conf., Karlsruhe, Germany, Paper P9 (1960) The Absorption Cross Section O16 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1958FU63 Phys.Rev.Letters 1, 465 (1958) Elastic Scattering of Photons by Tantalum
doi: 10.1103/PhysRevLett.1.465
1957HA13 Phys.Rev. 106, 991 (1957) Photon Self-Absorption and Scattering by the 15.1-MeV Level in C12
doi: 10.1103/PhysRev.106.991
1949HA55 Phys.Rev. 75, 917 (1949) The Energy Spectrum of the Delayed Neutrons from O17 RADIOACTIVITY 17N(β-n); measured decay products, En, In; deduced neutron energy distribution, an excited state width in 17O.
doi: 10.1103/PhysRev.75.917
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