NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = P.J.Ryan Found 9 matches. 1988HO11 Phys.Rev. C38, 1547 (1988) A.Hotta, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, P.J.Ryan, R.P.Singhal, D.Halderson Electroexcitation of 4He in the Near Continuum NUCLEAR REACTIONS 4He(e, e'), E=130, 200 MeV; measured σ(E(e'), θ(e')). Shell model in continuum interpretation.
doi: 10.1103/PhysRevC.38.1547
1986PA20 Phys.Rev. C34, 2354 (1986) B.Parker, R.S.Hicks, A.Hotta, R.L.Huffman, G.A.Peterson, M.A.Plum, P.J.Ryan, R.P.Singhal Transverse Quasielastic Electron Scattering from the Deuteron NUCLEAR REACTIONS 2H(e, e'), E=220, 270, 320 MeV; measured σ(E(e'), θ); deduced isobar configuration role.
doi: 10.1103/PhysRevC.34.2354
1986RY02 Nucl.Phys. A457, 1 (1986) Photodisintegration of 29,30Si to Excited Residual States NUCLEAR REACTIONS 29Si(γ, n), (γ, p); 30Si(γ, n), (γ, p), (γ, 2n), (γ, np), (γ, α), E=26 MeV bremsstrahlung; measured Eγ, Iγ. 29,28Si, 26Mg, 29,28Al levels deduced σ. 29,30Si deduced GDR, 1p-1h character. Enriched targets.
doi: 10.1016/0375-9474(86)90516-6
1984HO13 Phys.Rev. C30, 87 (1984) A.Hotta, P.J.Ryan, H.Ogino, B.Parker, G.A.Peterson, R.P.Singhal Quasielastic Electron Scattering from 56Fe at 180° NUCLEAR REACTIONS 56Fe(e, e'), E=155-555 MeV; measured σ(θ) vs energy loss, transverse response function; deduced effective mass ratio. Relativistic Fermi gas model.
doi: 10.1103/PhysRevC.30.87
1984RY01 Phys.Rev. C29, 655 (1984) P.J.Ryan, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson Transverse Quasielastic Electron Scattering from 12C at 180° NUCLEAR REACTIONS 12C(e, e'), E=150.6 MeV; measured σ(θ, E(e')), transverse quasielastic scattering. 12C deduced resonances. RPA theory comparison.
doi: 10.1103/PhysRevC.29.655
1983RY03 Phys.Rev. C21, 2575 (1983) P.J.Ryan, R.S.Hicks, A.Hotta, J.Dubach, G.A.Peterson, D.V.Webb Electroexcitation of Even-Parity States in 27Al NUCLEAR REACTIONS 27Al(e, e'), E=60-340 MeV; measured σ(E, θ), σ(E(e')). 27Al deduced levels, tentative J, π, form factors, effective charges.
doi: 10.1103/PhysRevC.27.2515
1983RY07 Nucl.Phys. A411, 105 (1983) P.J.Ryan, M.N.Thompson, K.Shoda, T.Tanaka The Photodisintegration of 24Mg NUCLEAR REACTIONS 24Mg(γ, p), (γ, n), E=28 MeV bremsstrahlung; measured proton yield vs Ep, Eγ, Iγ, σ(θp); deduced σ(γ, p)/σ(γ, n). 23Na, 23Mg levels deduced energy integrated population σ. 24Mg(γ, α), E=12-26 MeV bremsstrahlung; measured σ(θ). 24Mg deduced GDR decay characteristics, isospin purity, configuration. Magnetic spectrometer, enriched target.
doi: 10.1016/0375-9474(83)90510-9
1982RY02 Nucl.Phys. A389, 29 (1982) P.J.P.Ryan, M.N.Thompson, K.Shoda, M.Hirooka The Angular Distribution of Photoprotons from 27Al NUCLEAR REACTIONS 27Al(e, p), E=16.8-25.6 MeV; measured σ(E, θ); deduced σ(γ, p) vs θ. 27Al deduced GDR configurations, E2 decay characteristics.
doi: 10.1016/0375-9474(82)90288-3
1981RY03 Nucl.Phys. A371, 318 (1981) P.J.P.Ryan, M.N.Thompson, K.Shoda, T.Tanaka The Photoproton Decay of 27Al NUCLEAR REACTIONS 27Al(e, p), E=14.8-27.6 MeV; measured σ(Ep), σ(θ). 26Mg levels deduced population probability, photoproduction mechanism. Magnetic spectrometer, isotopically pure target.
doi: 10.1016/0375-9474(81)90070-1
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