NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Jeremie Found 20 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
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
1983PE04 Z.Phys. A310, 317 (1983) C.A.Peridier, J.L.Matthews, M.J.Leitch, H.Jeremie, M.Irshad, B.L.Roberts The 3He(γ, 2p)n Reaction for Eγ = 80 - 170 MeV NUCLEAR REACTIONS 3He(γ, p), E=80-170 MeV bremsstrahlung; measured σ(θ1, θ2) vs E; deduced strong proton-proton final state interaction. Kinematically complete experiment.
doi: 10.1007/BF01419518
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
1981DE31 Phys.Rev.Lett. 47, 1118 (1981) W.Del Bianco, L.Federici, G.Giordano, G.Matone, G.Pasquariello, P.Picozza, R.Caloi, L.Casano, M.P.De Pascale, L.Ingrosso, M.Mattioli, E.Poldi, C.Schaerf, P.Pelfer, D.Prosperi, S.Frullani, B.Girolami, H.Jeremie Neutron Asymmetry Measurements in the Deuteron Photodisintegration between 10 and 70 MeV NUCLEAR REACTIONS 2H(polarized γ, n), E=9.9-69 MeV; measured neutron asymmetry vs E; deduced meson exchange contributions. Monochromatic linearly polarized beam.
doi: 10.1103/PhysRevLett.47.1118
1980DE25 Nucl.Phys. A343, 121 (1980) W.Del Bianco, H.Jeremie, M.Irshad, G.Kajrys Deuteron Photodisintegration by 20.3 MeV Lineraly Polarized γ-Rays NUCLEAR REACTIONS 2H(γ, n), E=20.3 MeV; measured σ(θn, φn). Enriched target, linearly polarized beam.
doi: 10.1016/0375-9474(80)90644-2
1978JE01 Nucl.Phys. A312, 43 (1978) H.Jeremie, L.Lemay, M.Irshad, G.Kennedy The 9Be(p, pn)8Be (g.s.) Reaction between 10 and 24 MeV NUCLEAR REACTIONS 9Be(p, pn), E=10-24 MeV; measured σ(Ep, θ(p), θ(n)) in kinematically complete geometry; deduced reaction mechanism. 9Be deduced level. Natural target.
doi: 10.1016/0375-9474(78)90574-2
1977JE01 Can.J.Phys. 55, 261 (1977) Asymmetric Excitation of the Isobaric Doublet 9Be-9B Through the 9Be(p, pn)8Be(gs) Reaction NUCLEAR REACTIONS 9Be(p, pn), E=12.7 MeV; measured σ(Ep, θ), En.
1975JE04 Can.J.Phys. 53, 2639 (1975) Neutron Spectra from the 3H(7Li, 2n)2α Reaction NUCLEAR REACTIONS 3H(7Li, 2n), E=15, 23 MeV; measured nn-coin, time difference modes; deduced reaction mechanism.
1974LA02 Nucl.Phys. A218, 559 (1974) The 3H(t, α)2n Reaction at 40 keV NUCLEAR REACTIONS 3H(t, α), E=40 keV; measured σ(Eα, En, θ(α)=129°, θ(n)=47°); deduced final-state interactions.
doi: 10.1016/0375-9474(74)90041-4
1973JE02 Phys.Lett. 44B, 68 (1973) The Neutron-Neutron Scattering Length from a Complete Experiment on the 3H(d, 2n)3He Reaction at 8.45 MeV NUCLEAR REACTIONS 3H(d, 2n), E=9 MeV; measured σ(En), nn(t); deduced nn-scattering length.
doi: 10.1016/0370-2693(73)90304-3
1972JE05 Phys.Lett. 40B, 311 (1972) Cross-Section for Ejection of Deuterons from 6Li by Electrons NUCLEAR REACTIONS 6Li(e, e'd), E not given; calculated σ(θ). Born approximation.
doi: 10.1016/0370-2693(72)90807-6
1971JE03 Can.J.Phys. 49, 2085 (1971) Neutron-8Be Final-State Interaction in the Breakup of 9Be NUCLEAR REACTIONS 9Be(p, p'); E=5 MeV; measured nothing; analyzed available data; deduced n-8Be final-state interaction. 9Be deduced level.
doi: 10.1139/p71-254
1970PO05 Can.J.Phys. 48, 1414 (1970) Final-State Interaction in the 3H(t, α)2n Reaction at 90 keV NUCLEAR REACTIONS 3H(t, α) E=90 keV; measured σ(Eα, En); deduced n-n scattering length.
doi: 10.1139/p70-174
1969JE02 Nucl.Phys. A132, 571 (1969) The Reaction 2H(p, 2p)n between 5 and 10 MeV NUCLEAR REACTIONS 2H(p, 2p)n, E=5 to 10 MeV; measured σ(E;Ep1, θ(1), θ(2)); deduced n-p scattering length. Enriched target.
doi: 10.1016/0375-9474(69)90719-2
1967JE01 Nucl.Phys. A105, 689(1967) H.Jeremie, P.Martin, A.Calamand Three-Body Break-up in the Reaction 7Li(d, n)αα NUCLEAR REACTIONS 7Li(d, n)αα, E=180 keV; measured σ(Eα, θ nα). Natural target.
doi: 10.1016/0375-9474(67)90545-3
1963JE05 Nucl.Phys. 47, 225 (1963) Contribution a l'Etude de la Reaction (n, 2n) NUCLEAR STRUCTURE 2H, 9Be, 209Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90867-8
1961JE01 Compt.Rend. 252, 403 (1961) NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
1960HE10 J.Phys.Radium 21, 380 (1960) M.Heyman, H.Jeremie, J.Kahane, R.Sene Inelastic Scattering of Neutrons at 14 MeV by Excitation of the 9.6-MeV. Level of Carbon NUCLEAR STRUCTURE 13C, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:01960002105038000
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