NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.R.Deininger Found 7 matches. 1995PE01 Phys.Rev. C51, 1014 (1995) M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, S.Raman Low-Multipolarity Magnetic Transitions in 40Ca Excited by 180° Electron Scattering NUCLEAR REACTIONS Ca, S(e, e'), E=28.4-56.5 MeV; measured σ(θ); deduced σ. 40Ca levels deduced B(λ). Model comparison.
doi: 10.1103/PhysRevC.51.1014
1994PE08 Phys.Rev. C49, 3000 (1994) M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, R.Lindgren, S.Raman Low-Multipolarity Magnetic Transitions in 30Si, 32S, and 34S Studied by 180° Electron Scattering NUCLEAR REACTIONS 30Si, 32,34S(e, e'), E=28.4-63.4 MeV; measured spectra, σ. 32,34S, 30Si deduced M1, M2 transition strength fragmentation features.
doi: 10.1103/PhysRevC.49.3000
1992CO03 Phys.Lett. 277B, 383 (1992) J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, S.Raman, J.R.Deininger, S.E.Williamson Magnetic Dipole Strength in 46Ca Observed with 180° Electron Scattering NUCLEAR REACTIONS 46Ca(e, e'), E=32.9-63.1 MeV; measured σ(E(e')), θ=180°; deduced σ(θ). 46Ca level deduced reduced transition rate, transition radius, B(λ).
doi: 10.1016/0370-2693(92)91798-E
1992CO07 Phys.Rev. C45, 2494 (1992) J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, J.R.Deininger, S.E.Williamson Low-Momentum-Tranfer 180° Electron Scattering from the 3.68 MeV (3/2)- and the 3.85 MeV (5/2)+ States in 13C NUCLEAR REACTIONS 13C(e, e'), E=28.5-56.5 MeV; measured σ(E(e')), σ(θ), transverse form factors. 13C levels deduced B(λ).
doi: 10.1103/PhysRevC.45.2494
1992OB01 Nucl.Instrum.Methods Phys.Res. A312, 531 (1992) J.T.O'Brien, D.I.Sober, L.W.Fagg, H.Crannell, M.Petraitis, J.P.Connelly, J.R.Deininger, S.E.Williamson Design and Testing of Apparatus for 180° Electron Scattering at Low Momentum-Transfer NUCLEAR REACTIONS 28Si, 13C(e, e), E=53 MeV; measured electron spectra, before, after focal plane corrections. Low momentum transfer, 180° electron scattering appartus design and testing.
doi: 10.1016/0168-9002(92)90201-E
1991MI02 Phys.Rev. C43, 1677 (1991) R.A.Miskimen, E.A.Ammons, J.D.T.Arruda-Neto, G.O.Bolme, L.S.Cardman, P.L.Cole, J.R.Deininger, S.M.Dolfini, A.J.Linzey, J.B.Mandeville, B.L.Miller, P.E.Mueller, C.N.Papanicolas, A.Serdarevic, S.E.Williamson Use of the (e, e'n) Reaction to Study the Giant Multipole Resonances in 116Sn NUCLEAR REACTIONS 116Sn(e, e'n), E=68.3, 68.4, 99.4 MeV; measured σ(θn, En). 116Sn deduced giant multipole resonance EWSR strengths. Open-shell, continuum RPA.
doi: 10.1103/PhysRevC.43.1677
1990MI03 Phys.Lett. 236B, 251 (1990) R.A.Miskimen, E.A.Ammons, J.D.T.Arruda-Neto, L.S.Cardman, P.L.Cole, J.R.Deininger, S.M.Dolfini, A.J.Linzey, J.B.Mandeville, B.L.Miller, P.E.Mueller, C.N.Papanicolas, A.Serdarevic, S.E.Williamson Coincidence Studies of the Giant Multipole Resonances in 116Sn Using the (e, e'n) Reaction NUCLEAR REACTIONS 116Sn(e, e'n), E ≤ 100 MeV; measured σ(θn) for fixed E, θ(e'). 116Sn deduced transition strengths in giant resonance region.
doi: 10.1016/0370-2693(90)90977-E
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