NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = P.Richard Found 34 matches. 1986HA02 Phys.Rev. A33, 914 (1986) J.Hall, P.Richard, P.L.Pepmiller, D.C.Gregory, P.D.Miller, C.D.Moak, C.M.Jones, G.D.Alton, L.B.Bridwell, C.J.Sofield Energy Systematics of Single and Double K-Shell-Vacancy Production in Titanium Bombarded by Chlorine Ions NUCLEAR REACTIONS Ti(37Cl, X), E=6.88 MeV/nucleon; measured E K(X-ray), I K(X-ray); deduced single, double K-shell vacancy production σ.
doi: 10.1103/PhysRevA.33.914
1975JA02 Phys.Rev. A11, 505 (1975) K.A.Jamison, C.W.Woods, R.L.Kauffman, P.Richard Kα Satellite X Rays in Al, Sc, and Ti Following Bromine-Ion Bombardment ATOMIC PHYSICS Al, Sc, Ti(Br, Br), E=31 MeV; measured I(K, L X-rays).
doi: 10.1103/PhysRevA.11.505
1974EL04 Z.Phys. 269, 89 (1974) D.O.Elliott, F.F.Hopkins, G.W.Phillips, P.Richard Low Lying Levels in 124Sb NUCLEAR REACTIONS 124Sn(p, nγ), E=6 MeV; measured γγ-coin, σ(Eγ). 124Sb deduced levels, J, π.
doi: 10.1007/BF01669048
1973HO22 Phys.Rev. C8, 380 (1973) F.F.Hopkins, J.R.White, C.F.Moore, P.Richard Gamma Cascades in 252Cf Spontaneous Fission Fragments RADIOACTIVITY, Fission 252Cf; measured Eγ, Iγ, γγ-coin. 105Mo, 109,111Ru, 146La deduced levels.
doi: 10.1103/PhysRevC.8.380
1973HO37 Phys.Rev. C8, 1721 (1973) F.Hopkins, J.S.Eck, D.O.Elliott, P.Richard, J.R.White Particle Emission from High Excitation in the 40Ca System NUCLEAR REACTIONS 24Mg(16O, Xγ), E=30-40 MeV; 28Si(12C, Xγ), E=24-26 MeV; measured Eγ, γγ-coin, σ. 40Ca deduced transitions.
doi: 10.1103/PhysRevC.8.1721
1972EL01 Phys.Rev. C5, 202 (1972) D.O.Elliott, G.W.Phillips, F.F.Hopkins, P.Richard Low-Lying States in 122Sb from the 122Sn(p, n) Reaction NUCLEAR REACTIONS 122Sn(p, n), E=6.5, 6.0 MeV; measured Eγ, γγ-coin. 121Sb(d, p), E=13 MeV; measured σ(Ep). 122Sb deduced levels, γ-branching. Ge(Li) detectors.
doi: 10.1103/PhysRevC.5.202
1972HO08 Phys.Rev. C5, 1015 (1972) F.F.Hopkins, J.R.White, G.W.Phillips, C.F.Moore, P.Richard Further Measurements of Gamma Transitions in Spontaneous-Fission Fragments of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured Xγ-coin. 100,102,104Zr, 146,147,148Ce, 141,142,143,144,146La, 102,104,106Mo, 139,142,144,146Ba, 105,106,108,110Tc, 138,139,142Cs, 106,109,111Ru, 137,138,142Xe, 109,111Pd, 137Te, 108,109,112,113Rh, 132,134,136I, 114Pd, 132,134Te, 98Y, 95,98Sr, 143,145,147,153Pr, 147,151,154Nd, 94Rb, 149,154Pm, 91Kr, 156Sm, 156,158Eu; measured Eγ; deduced transitions. Ge(Li) detectors.
doi: 10.1103/PhysRevC.5.1015
1972MA16 Phys.Rev. C5, 1390 (1972) D.L.Matthews, F.F.Hopkins, P.Richard, G.W.Phillips, C.F.Moore States in 93Mo to 5 MeV by 92Mo(d, pγ)93Mo Coincidence Measurements NUCLEAR REACTIONS 92Mo(d, pγ), E=6 MeV; measured σ(Ep, Eγ), Iγ, pγ-coin 93Mo deduced levels, γ-branching. Ge(Li), Si(Li) detectors.
doi: 10.1103/PhysRevC.5.1390
1972PH02 Phys.Rev. C5, 297 (1972) G.W.Phillips, P.Richard, D.O.Elliott, F.F.Hopkins, A.C.Porter Structure of Mass 15: The 14N(p, γ)15O and 14N(p, p'γ) Reactions NUCLEAR REACTIONS 14N(p, γ), 14N(p, p'γ), E=3.75-5.22 MeV; measured σ(E;Eγ). 15O deduced resonances, level-width, γ-branching. Ge(Li) detector.
doi: 10.1103/PhysRevC.5.297
1971HO11 Z.Phys. 243, 446 (1971) F.F.Hopkins, W.J.Courtney, W.R.Coker, C.F.Moore, P.Richard 208Pb(p, α)205Tl Reaction at 16.475 MeV NUCLEAR REACTIONS 208Pb(p, α), E=16.475 MeV; measured σ(Eα, θ). 205Tl deduced levels, J, π.
doi: 10.1007/BF01396619
1971HO29 Phys.Rev. C4, 1927 (1971) F.F.Hopkins, G.W.Phillips, J.R.White, C.F.Moore, P.Richard Low-Energy Transitions from the Deexcitation of Spontaneous Fission Fragments of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured Xγ-coin. 150Pr, 101Y, 99Y, 148,150Ce, 149Ce, 102Zr, 100Zr, 145,146,147La, 103Nb, 104Nb, 106Mo, 142,144,145Ba, 140Cs, 108Tc, 138,141,142Cs, 109Tc, 105Tc, 110Ru, 108Ru, 111Ru, 116Rh, 136I, 112Rh, 137I; measured Eγ; deduced transitions. RADIOACTIVITY, Fission 252Cf(SF); measured Xγ-coin. 150Pr, 101Y, 99Y, 148,150Ce, 149Ce, 102Zr, 100Zr, 145,146,147La, 103Nb, 104Nb, 106Mo, 142,144,145Ba, 140Cs, 108Tc, 138,141,142Cs, 109Tc, 105Tc, 110Ru, 108Ru, 111Ru, 116Rh, 136I, 112Rh, 137I deduced transitions.
doi: 10.1103/PhysRevC.4.1927
1971RI11 Nucl.Phys. A174, 273 (1971) Fine Structure in Isobaric Analogue Resonances NUCLEAR REACTIONS 90Zr(p, p), 92Mo(p, p), E=5.1-6.1 MeV; measured σ(E). 91Nb, 93Tc deduced isobaric analog resonances, level-width.
doi: 10.1016/0375-9474(71)90662-2
1971ST29 Phys.Rev. C4, 1948 (1971) R.St-Laurent, G.W.Phillips, P.Richard, C.F.Moore Internal-Conversion Cascades in Fission Products RADIOACTIVITY, Fission 252Cf; measured XX-coin, I(X-ray).
doi: 10.1103/PhysRevC.4.1948
1970KU13 Phys.Rev. C2, 1491 (1970) J.G.Kulleck, P.Richard, D.Burch, C.F.Moore, W.R.Wharton, P.von Brentano Particle-Hole States in 208Pb with the Configuration (d5/2, j-1) NUCLEAR REACTIONS 208Pb(p, p'), E=16.5 MeV; measured σ(Ep', θ). 208Pb deduced levels, J, π, level-width.
doi: 10.1103/PhysRevC.2.1491
1969EJ02 Nucl.Phys. A128, 388 (1969) H.Ejiri, P.Richard, S.Ferguson, R.Heffner, D.Perry The 140Ce(p, γ)141Pr Reaction Through Isobaric Analogue Resonances in 141Pr NUCLEAR REACTIONS 140Ce(p, γ), E=9.5-10.7 MeV; measured σ(E;θ). 141Pr deduced level-width matrix for isobaric analog state, the analogous beta matrix. Natural Ce.
doi: 10.1016/0375-9474(69)90412-6
1969RI08 Phys.Letters 29B, 649 (1969) P.Richard, F.Gabbard, A.C.Porter, F.F.Hopkins The 88Sr(p, γ)89Y Reaction Near the d5/2 Ground-State Analogue NUCLEAR REACTIONS 88Sr(p, γ), (p, n), E=4.9-5.2 MeV; measured σ(E;Eγ). 89Y deduced resonances, level-width. Enriched 88Sr target, Ge(Li) detector.
doi: 10.1016/0370-2693(69)90099-9
1969RI10 Phys.Rev. 183, 1007 (1969) P.Richard, P.Von Brentano, H.Wieman, W.Wharton, W.G.Weitkamp, W.W.McDonald, D.Spalding Low-Lying Levels of 208Pb with g9/2, i11/2, or j15/2 Neutron-Particle Configurations NUCLEAR REACTIONS 208Pb(p, p'), E = 14-18 MeV; measured σ(E;Ep', θ). 209Bi deduced resonances, level-width. 208Pb deduced levels, J, π, level-width. Detector - Si(Li).
doi: 10.1103/PhysRev.183.1007
1969WH05 Phys.Rev. 188, 1934 (1969) W.R.Wharton, W.J.Courtney, P.Richard Analog Resonances of 206Tl and 204Tl NUCLEAR REACTIONS 203,205Tl(p, p), (p, p'), E=13.5-18.6 MeV; measured σ(E). 204,206Pb deduced resonances, level-width, isobaric analogs.
doi: 10.1103/PhysRev.188.1934
1968BO16 Phys.Letters 27B, 5 (1968) J.P.Bondorf, P.Von Brentano, P.Richard Configurations of the Lowest 4- State in 208Pb NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90317-1
1968CU04 Phys.Rev. 173, 1108 (1968) Proton Decay of Analog States Formed in the (d, n) Reaction NUCLEAR REACTIONS 16O, 27Al, 64Ni, 68Zn, 89Y, 90,91,92,94Zr, 92,94,98Mo, 114,116,118,120Sn, 206Pb(d, np), E < 16 MeV; measured σ(E;Ep).
doi: 10.1103/PhysRev.173.1108
1968EJ02 Phys.Rev.Letters 21, 373(1968) H.Ejiri, P.Richard, S.Ferguson, F.Heffner, D.Perry Electric Dipole Transition from the 2f7/2 Isobaric Analog Resonance to the 2d5/2 Ground State in 141Pr NUCLEAR REACTIONS 140Ce(p, γ), E=9.75 MeV; measured σ(Eγ, θ). 141Pr analog resonance deduced γ-width, transition matrix elements. Natural target.
doi: 10.1103/PhysRevLett.21.373
1968HE02 Phys.Letters 26B, 150 (1968) R.Heffner, C.Ling, N.Cue, P.Richard Charge Exchange Effects in the (d, p) Reaction Leading to States in 93,95Zr, 93,95Mo and 141Ce NUCLEAR STRUCTURE 141Ce, 93Zr, 93Mo, 95Zr, 95Mo; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90512-1
1968RI11 Phys.Rev. 171, 1308 (1968) P.Richard, N.Stein, C.D.Kavaloski, J.S.Lilley Two-Neutron-Hole Configurations in Pb206 from Isobaric Analog Measurements NUCLEAR STRUCTURE 206Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.171.1308
1968VO02 Phys.Letters 26B, 666 (1968) P.Von Brentano, W.K.Dawson, C.F.Moore, P.Richard, W.Wharton, H.Wieman Determination of the Total Widths of the Single-Particle Analog Resonances in 209Bi
doi: 10.1016/0370-2693(68)90384-5
1968WH02 Phys.Rev. 176, 1424 (1968) W.R.Wharton, P.Von Brentano, W.K.Dawson, P.Richard Determination of Total Widths and Resonance Energies of the Single-Particle Analog Resonances in 209Bi NUCLEAR REACTIONS 208Bi(p, p'), E=14-18 MeV; measured σ(Ep). 209Bi deduced resonances, J, π, level-width, isobaric analog.
doi: 10.1103/PhysRev.176.1424
1967RI13 Phys.Letters 26B, 8 (1967) P.Richard, W.G.Weitkamp, W.Wharton, H.Wieman, P.Von Brentano The Proton Decay of the g9/2 Analogue Resonance in 209Bi NUCLEAR STRUCTURE 209Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90531-X
1966KA02 Phys.Rev.Lett. 16, 807 (1966) C.D.Kavaloski, J.S.Lilley, P.Richard, N.Stein Decay of Isobaric Analog States in the Lead Region NUCLEAR STRUCTURE 207Pb, 208Pb, 206Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.16.807
1966LO09 Phys.Rev. 149, 906 (1966) D.D.Long, P.Richard, C.F.Moore, J.D.Fox Coulomb Displacement Energies from Isobaric Analogue Resonances
doi: 10.1103/PhysRev.149.906
1966MO06 Phys.Rev. 141, 1166 (1966) C.F.Moore, P.Richard, C.E.Watson, D.Robson, J.D.Fox Isobaric Analogue States in Heavy Nuclei. I. Molybdenum Isotopes NUCLEAR STRUCTURE 93Tc, 101Tc, 95Tc, 96Tc, 97Tc, 98Tc, 99Tc; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.141.1166
1966RI06 Phys.Rev. 145, 971 (1966) P.Richard, C.F.Moore, J.A.Becker, J.D.Fox Isobaric Analogue States in Heavy Nuclei. III. Tin Isotopes NUCLEAR STRUCTURE 117Sb, 113Sb, 115Sb, 119Sb, 118Sb, 123Sb, 121Sb, 120Sb, 125Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.145.971
1965MO02 Bull.Am.Phys.Soc. 10, No.1, 52, DC10 (1965) C.F.Moore, C.E.Watson, P.Richard, D.Robson, J.D.Fox Analog Comparisons in Reactions on the Molybdenum Isotopes NUCLEAR STRUCTURE Mo; measured not abstracted; deduced nuclear properties.
1965RI01 Bull.Am.Phys.Soc. 10, No.1, 52, DC11 (1965) Fine Structure in Isobaric Analog of Mo93 and Zr91 NUCLEAR STRUCTURE 91Nb, 91Mo, 93Tc; measured not abstracted; deduced nuclear properties.
1965RO23 Phys.Lett. 18, 86 (1965) D.Robson, J.D.Fox, P.Richard, C.F.Moore Reactions Involving Simple Isobaric Analogue Resonances NUCLEAR REACTIONS 92Zr(p, p), E(cm) ≈ 5.8-6.2 MeV; measured σ(E). 92Zr(p, n), E ≈ 5.7-6.3 MeV; analyzed data. 93Zr deduced resonance, Γp, Γ0.
doi: 10.1016/0031-9163(65)90039-9
1963FO08 Conf.Compd.Nucl.States, Gatlinburg, Tenn., p.8, A11 (1963) J.D.Fox, F.Robson, C.F.Moore, P.Richard Prominent Compound Nuclear States in Zr90 Near the Neutron Binding Energy NUCLEAR STRUCTURE 89Y, 90Zr; measured not abstracted; deduced nuclear properties.
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