NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = L.Lessard Found 21 matches. 1988CH30 Z.Phys. A330, 377 (1988) A.Champagne, G.Beaudoin, L.A.Hamel, H.Jeremie, L.Lessard Measurement of the Beta Spectrum of the 0- (120 keV) State of 16N RADIOACTIVITY 16N(β-) [from 15N(d, p), E=2 MeV]; measured β-spectrum.
1985HA22 Z.Phys. A321, 439 (1985) L.A.Hamel, L.Lessard, H.Jeremie, J.Chauvin New Measurement of the Beta Decay Rate of the 16N(0-) - 16O(0+) Transition RADIOACTIVITY 16N(β-) [from 15N(d, p), E=2 MeV]; measured Eβ, Iβ, Eγ, Iγ; deduced g(p)/g(A), β-decay rate.
doi: 10.1007/BF01411977
1985PA20 Phys.Rev. C32, 916 (1985) Proton-Induced Fission of 232Th and Ir: Exciton model calculations NUCLEAR REACTIONS, ICPND 232Th(p, 6n), E ≈ 35-100 MeV; 232Th(p, 7n), E ≈ 45-90 MeV; calculated σ(E). 232Th(p, F)128Cs/130Cs/132Cs/134Cs/136Cs/138Cs/140Cs/142Cs/144Cs/146Cs, E=97 MeV; 232Th(p, F)85Rb/86Rb/87Rb/88Rb/89Rb/90Rb/91Rb/92Rb/93Rb/94Rb/95Rb/96Rb/97Rb, E=29, 59, 75, 97 MeV; calculated residual production σ following fission. Ir(p, F), E=40-160 MeV; calculated fission σ(E).
doi: 10.1103/PhysRevC.32.916
1984FO10 Phys.Rev. C30, 79 (1984) J.L.Foster, Jr., S.E.Darden, M.C.Rozak, J.A.Ross, J.P.Martin, L.Lessard, S.Gales, G.Noury, J.M.Pearson, P.Depommier, M.C.Hermida, M.Ruiz 130Te(p(pol), p1) and 130Te(p, p1(pol)) Reactions on Analog Resonances NUCLEAR REACTIONS 130Te(polarized p, p), (polarized p, p'), E(cm)=10.1-10.7 MeV; measured σ(θ) vs E, analyzing power vs θ, E, polarization vs θ; deduced optical model parameters. 131I deduced IAR, J, π, configuaration. Coupled-channels analysis.
doi: 10.1103/PhysRevC.30.79
1984HA56 Nucl.Instrum.Methods 228, 9 (1984) L.A.Hamel, J.Chauvin, L.Lessard, H.Jeremie A Recirculating Gas Target for the Measurement of Very Short-Lived Beta-Decays RADIOACTIVITY 16N(β-) [from 15N(d, p)]; measured β-spectra. 16O level deduced branching ratio (λβ/λγ). Recirculating gas target.
doi: 10.1016/0168-9002(84)90003-2
1982JE04 Can.J.Phys. 60, 1616 (1982); Erratum Can.J.Phys. 61, 656 (1983) H.Jeremie, L.Lessard, S.Gujrathi, B.Zeitnitz The N - P Final State Interaction in the 2H(d, np)2H Reaction at 12 MeV NUCLEAR REACTIONS 2H(d, np), E=12 MeV; measured σ(θd, θp, Ep); deduced quasifree scattering, final state interaction superposition.
doi: 10.1139/p82-217
1982PA11 Phys.Rev. C25, 2534 (1982) B.P.Pathak, L.Lessard, L.Nikkinen, J.K.P.Lee Proton-Induced Fission of Iridium NUCLEAR REACTIONS, ICPND 191,193Ir(p, F)84Rb/85Rb/86Rb/87Rb/88Rb/89Rb/90Rb/91Rb/92Rb, E=68, 85, 100 MeV; measured fission σ, independent yields of residuals; deduced neutron multiplicities.
doi: 10.1103/PhysRevC.25.2534
1980NI08 Phys.Rev. C22, 617 (1980) L.Nikkinen, B.P.Pathak, L.Lessard, I.S.Grant Independent Yields of Rb, In, Cs Isotopes in the Proton-Induced Fission of 232Th NUCLEAR REACTIONS 232Th(p, F), E=29, 59, 75, 97 MeV; measured independent σ(E) for 116,117,118,119,120,121,122,123,124,125,96,97Rb, 131,132,133,134,135,136,137,138,139,140,141,142,143,144Cs; deduced total neutron number per fission event.
doi: 10.1103/PhysRevC.22.617
1978CH25 J.Phys.(London) G4, 1501 (1978) H.C.Cheung, H.Huang, B.N.Subba Rao, L.Lessard, J.K.P.Lee Decay of 120In RADIOACTIVITY 120,120mIn [from 238U(p, F), separated isotope]; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 120Sn deduced levels, J, π.
doi: 10.1088/0305-4616/4/9/020
1977CH24 J.Inorg.Nucl.Chem. 39, 1915 (1977) K.C.Chan, B.P.Pathak, L.Nikkinen, L.Lessard, I.S.Grant Independent Yields of Indium and Gallium in the Proton Induced Fission Of Natural Uranium NUCLEAR REACTIONS 238U(p, F), E=30-98.6 MeV; measured σ(E, A, Z).
doi: 10.1016/0022-1902(77)80516-2
1977HU03 Z.Phys. A282, 285 (1977) H.Huang, B.P.Pathak, R.Iafigliola, L.Lessard, J.K.P.Lee Decay of 90m, g-Rb RADIOACTIVITY 90,90mRb [from 238U(p, F)]; measured Eγ, Iγ, γγ-coin, I(ce), Eβ, T1/2, βγ-coin; deduced log ft, Q, β-branching. 90Sr deduced levels. 90Rb transition deduced B(λ).
doi: 10.1007/BF01414896
1977PA10 Phys.Rev. C15, 1577 (1977) B.P.Pathak, L.Lessard, L.Nikkinen Decay of the 66-keV Level in 127Cs RADIOACTIVITY 127Ba; measured γγ(t), K X-ray; deduced ICC. 127Cs transition deduced λ, hindrance factor, T1/2.
doi: 10.1103/PhysRevC.15.1577
1976PA11 Phys.Rev. C14, 1573 (1976) B.P.Pathak, L.Lessard, L.Nikkinen, I.L.Preiss Decays of 126Ba and 126Cs RADIOACTIVITY 126Ba, 126Cs [from 115In(16O, 5n), 121Sb(11B, 6n), 133Cs(p, 8n)]; measured Eγ, Iγ, I(ce), βγ-, xrayγ-, γγ-coin; deduced log ft, ICC, EC/β+ ratio, Q. 126Ba; measured T1/2. 126Cs, 126Xe deduced levels, J, π, B(E2).
doi: 10.1103/PhysRevC.14.1573
1976RE07 Phys.Lett. 62B, 33 (1976) W.Reisdorf, M.de Saint-Simon, L.Lessard, L.Remsberg, C.Thibault, E.Roeckl, R.Klapisch, I.V.Kuznetsov, Y.T.Oganessian, Y.E.Penionshkevitch Low Neutron Multiplicity in the Symmetric Fission Reaction 158Gd(22Ne, Rb)Rb NUCLEAR REACTIONS 158Gd(22Ne, F), E=127, 141, 166 MeV; measured isotopic Rb distribution, neutron multiplicity.
doi: 10.1016/0370-2693(76)90040-X
1976RE11 Phys.Rev. C14, 2189 (1976) W.Residorf, M.de Saint-Simon, L.Remsberg, L.Lessard, C.Thibault, E.Roeckl, R.Klapisch Analysis of Isotopic Yield Distributions in 11B- and 22Ne-Induced Fission of 238U NUCLEAR REACTIONS 238U(11B, F), E=85 MeV; 238U(22Ne, F), E=132, 165 MeV; calculated σ(A, Z), Z=37, Z=55, first moments, variances. Statistical model.
doi: 10.1103/PhysRevC.14.2189
1976SA24 Phys.Rev. C14, 2185 (1976) M.de Saint-Simon, L.Lessard, W.Reisdorf, L.Remsberg, C.Thibault, E.Roeckl, R.Klapisch, I.V.Kuznetsov, Y.T.Oganesian, Y.E.Penionshkevitch On-Line Mass-Spectrometric Measurement of Rubidium and Cesium Isotopic Distributions in 11B- and 22Ne-Induced Fission of 238U NUCLEAR REACTIONS 238U(11B, F), E=85 MeV; 238U(22Ne, F), E=132, 162 MeV; measured Rb, Cs isotopic distributions, σ(A, Z), Z=37, 55; deduced first moment of distributions.
doi: 10.1103/PhysRevC.14.2185
1975TH08 Phys.Rev. C12, 644 (1975) C.Thibault, R.Klapisch, C.Rigaud, A.M.Poskanzer, R.Prieels, L.Lessard, W.Reisdorf Direct Measurement of the Masses of 11Li and 26-32Na with an on-Line Mass Spectrometer RADIOACTIVITY 11Li; measured neutron binding energy, delayed neutron branching ratio, T1/2; deduced log ft. ATOMIC MASSES 11Li, 26,27,28,29,30,31,32Na; measured mass excesses.
doi: 10.1103/PhysRevC.12.644
1974BI01 Phys.Rev. C9, 741 (1974) L.Bimbot, L.Lessard, S.Santhanam, R.Martin, O.Dietzsch, D.Spalding, K.Schechet, J.L.Foster, Jr. 142Nd(p, p') Reaction on Analog Resonances NUCLEAR REACTIONS 142Nd(p, p'), E=9.5-11 MeV on analog resonances; measured σ(θ). 142Nd deduced levels, J, π, S. Enriched targets, Breit-Wigner analysis, resolution 5-15 keV, θ=20-170°.
doi: 10.1103/PhysRevC.9.741
1973GA01 Nucl.Phys. A202, 535 (1973) S.Gales, L.Lessard, J.L.Foster, Jr. The 144Nd(d, p) and 144Nd(d, t) Reactions and Isobaric Analog Resonances In 144Nd(p, p0) and 144Nd(p, p') NUCLEAR REACTIONS 144Nd(d, p), (d, t), Ed=12.6 MeV; measured Q, σ(E, θ). 145Nd, 143Nd deduced levels, (J), π, L. 144Nd(p, p0), 144Nd(p, p'), Ep=9.3-12 MeV; measured σ(E). 145Pm deduced isobaric analog resonances level-width, J, π.
doi: 10.1016/0375-9474(73)90641-6
1973MA31 Nucl.Phys. A210, 221 (1973) R.Martin, L.Bimbot, S.Gales, L.Lessard, D.Spalding, W.G.Weitkamp, O.Dietzsch, J.L.Foster, Jr. The 144Sm(p, p') Reaction on Analog Resonances NUCLEAR REACTIONS 144Sm(p, p'), E=9.3-11 MeV; measured σ(E, θ). 144Sm deduced levels, J, π, S.
doi: 10.1016/0375-9474(73)90299-6
1972LE17 Phys.Rev. C6, 517 (1972) L.Lessard, S.Gales, J.L.Foster, Jr. 142Ce(d, p) and 142Ce(d, t) Reactions and Isobaric Analog Resonances in 142Ce(p, p0) and 142Ce(p, p1) NUCLEAR REACTIONS 142Ce(d, p), (d, t), E=12.6 MeV; measured Q, σ(θ). 142Ce(p, p), (p, p'), E=9.5-12 MeV; measured σ(E). 143Ce deduced levels, J, π, L(n), S. 143Pr deduced isobaric analog resonance, level-width, J, π. 143Ce, 143Pr deduced Coulomb displacement energy.
doi: 10.1103/PhysRevC.6.517
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