NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.R.Dodge Found 26 matches. 1999BE79 Nucl.Phys. (Supplement) A654, 837c (1999) B.L.Berman, C.Cetina, P.L.Cole, W.R.Dodge, G.Feldman, J.C.Sanabria, N.Kolb, R.E.Pywell, J.Vogt, V.Nedorezov, A.Sudov, G.Ya.Kezerashvili Photofission of Actinide and Pre-Actinide Nuclei in the Quasideuteron and Delta Energy Regions NUCLEAR REACTIONS Pb, 197Au(γ, F), E=122-222 MeV; measured fission σ. 232Th, 233,235,238U, 237Np(γ, F), E=64-264 MeV; measured fission σ; deduced relative fissilities. Tagged photon beams.
doi: 10.1016/S0375-9474(00)88557-7
1998ST17 Phys.Rev. D58, 032003 (1998) L.M.Stuart, P.E.Bosted, L.Andivahis, A.Lung, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.H.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao Measurements of the Δ(1232) Transition Form Factor and the Ratio σn/σp from Inelastic Electron-Proton and Electron-Deuteron Scattering NUCLEAR REACTIONS 1,2H(e, e'), E=9.8 GeV; measured σ(E', θ); deduced transition form factors, Δ production σ(n)/σ(p).
doi: 10.1103/PhysRevD.58.032003
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
1993SA03 Phys.Rev. C47, 459 (1993) A.J.Sarty, K.G.R.Doss, G.Feldman, E.L.Hallin, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, H.R.Weller, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, C.C.Chang Measurement of the Reaction 3He(γ, pp)n and Its Relation to Three-Body Forces NUCLEAR REACTIONS 3He(γ, 2p), E=90-250 MeV bremsstrahlung; measured σ(θn, θp) vs neutron momentum; deduced two-pion-exchange, three-body absorption mechanisms role.
doi: 10.1103/PhysRevC.47.459
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
1991BO21 Nucl.Phys. A527, 339c (1991) P.E.Bosted, L.Clogher, A.Lung, L.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.G.Petratos, G.A.Peterson, S.E.Rock, S.H.Rokni, W.K.Sakumoto, K.Swartz, Z.N.Szalata, L.H.Tao New Measurements of the Electric and Magnetic Elastic Form Factors of the Proton and Neutron at High Momentum Transfers NUCLEAR REACTIONS 1H(e, e'), E=1.4-10 GeV; measured electron spectra. 1H deduced magnetic form factor.
doi: 10.1016/0375-9474(91)90123-N
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
1990HA09 Phys.Rev. C41, 1619 (1990) K.Hansen, J.-O.Adler, K.I.Blomqvist, D.Nilsson, A.Sandell, B.Schroder, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, J.R.Calarco, J.P.Connelly, F.W.Hersman, W.Kim, M.Leuschner Electrofission in the Quasifree and Delta Regions NUCLEAR REACTIONS 233,238U(e, e'F), E=720-830 MeV; measured σ(E, θ), fission probability; deduced mean nuclear excitation energy. Parallel plate avalanche detector.
doi: 10.1103/PhysRevC.41.1619
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
1987OC01 Phys.Rev. C35, 1063 (1987) J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn, J.H.Koch, N.Ohtsuka Electromagnetic Excitation of the Delta Resonance in Nuclei NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'X), E=537, 730 MeV; measured inclusive σ(E(e'), θ(e')); deduced quasifree peak positions, widths, average separation energies. Dispersion matched energy loss spectrometer. Model calculations.
doi: 10.1103/PhysRevC.35.1063
1986DO05 Phys.Rev. C33, 1251 (1986) Siegert's Theorem and Nuclear Electrodisintegration NUCLEAR REACTIONS 90Zr(e, e'p), E=17-104 MeV; measured σ(E) across IAS; deduced transverse Coulomb interference term sign, magnitude. 90Zr deduced ΓγΓp0/Γ vs E.
doi: 10.1103/PhysRevC.33.1251
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
1984OC01 Phys.Rev.Lett. 53, 1627 (1984) J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn Electron Scattering in the Excitation Region of the Delta Resonance on Nuclei with A = 1 to 16 NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'), E=730 MeV; measured σ vs energy loss; deduced (σ/A) in the quasifree, isobar resonance regions.
doi: 10.1103/PhysRevLett.53.1627
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
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
1974CH13 Phys.Rev. C9, 1300 (1974) C.C.Chang, W.R.Dodge, J.J.Murphy, II 3He(γ, d)1H Cross Section from 10 to 21 MeV NUCLEAR REACTIONS 3He(e, d), Eγ=10-21 MeV; measured σ(Eγ, 90°).
doi: 10.1103/PhysRevC.9.1300
1972DO03 Phys.Rev.Lett. 28, 839 (1972) Ratio of the 4He(γ, p) and 4He(γ, n) Cross Sections NUCLEAR REACTIONS 4He(γ, n), (γ, p), E=30-52 MeV; measured σ(E).
doi: 10.1103/PhysRevLett.28.839
1972SK05 Phys.Rev. C6, 43 (1972) 4He(e, d)e'2H Angular-Distribution and Cross-Section Measurements between 36 and 50 MeV NUCLEAR REACTIONS 4He(e, d), E=36-50 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.6.43
1961DO08 Thesis, Stanford University (1961); HEPL-246 (1961); Nuclear Sci.Abstr. 16, 750, Abstr.5921 (1962) NUCLEAR STRUCTURE 27Al, 19F, Ar, Ne, C, B, O; measured not abstracted; deduced nuclear properties.
1960DO04 Contrib.Karlsruhe Photonuclear Conf., Karlsruhe, Germany, Paper A7 (1960) Photoprotons from Oxygen, Fluorine and Neon NUCLEAR STRUCTURE 19F, 20Ne, 16O; measured not abstracted; deduced nuclear properties.
1958BA30 Bull.Am.Phys.Soc. 3, No.3, 173, E7 (1958) W.C.Barber, W.R.Dodge, V.J.Van Huyse Protons from the Photo- and Electrodisintegration of C12 and Al27
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