NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Girard Found 23 matches. 1995BL01 Nucl.Phys. A582, 296 (1995) J.Blons, D.Goutte, A.Lepretre, R.Letourneau, R.Lucas, V.Meot, D.Paya, X.H.Phan, J.Girard, G.Barreau, T.P.Doan, G.Pedemey, Ph.Dessagne, Ch.Miehe A New Isomeric State in 65Ni NUCLEAR REACTIONS 64Ni(18O, 17O), E=72 MeV; measured Eγ, pγ-coin. 65Ni deduced levels, T1/2.
doi: 10.1016/0375-9474(94)00448-V
1988DU01 Phys.Lett. 200B, 17 (1988) P.Dupieux, J.P.Alard, J.Augerat, R.Babinet, N.Bastid, F.Brochard, P.Charmensat, N.de Marco, H.Fanet, Z.Fodor, L.Fraysse, J.Girard, P.Gorodetzky, J.Gosset, C.Laspalles, M.C.Lemaire, D.L'Hote, B.Lucas, J.Marroncle, G.Montarou, M.J.Parizet, J.Poitou, D.Qassoud, C.Racca, A.Rahmani, W.Schimmerling, O.Valette Proton-Proton Correlations at Small Relative Momentum in Neon-Nucleus Collisions at E/A = 400 and 800 MeV NUCLEAR REACTIONS C, Na, F, Nb, Pb(20Ne, X), E=400, 800 MeV/nucleon; measured proton-proton correlation functions; deduced emitting region sizes, target mass density vs incident energy.
doi: 10.1016/0370-2693(88)91101-X
1987LH01 Phys.Lett. 198B, 139 (1987) D.L'Hote, J.P.Alard, J.Augerat, R.Babinet, F.Brochard, Z.Fodor, L.Fraysse, J.Girard, P.Gorodetzky, J.Gosset, C.Laspalles, M.C.Lemaire, B.Lucas, G.Montarou, M.J.Parizet, J.Poitou, C.Racca, W.Schimmerling, J.C.Tamain, Y.Terrien, J.Valerio, J.Cugnon, J.Vandermeulen Exclusive Measurements of Mean Pion Multiplicities in 4He-Nucleus Reactions from 200 to 800 MeV/Nucleon NUCLEAR REACTIONS C, Cu, Pb(α, π+), (α, π-), E=200, 600, 800 MeV/nucleon; C, Pb(α, π+), (α, π-), E=400 MeV/nucleon; measured mean pion multiplicities. Cylindrical drift chamber.
doi: 10.1016/0370-2693(87)91484-5
1986MI25 Nucl.Phys. A459, 594 (1986) B.Million, V.Bellini, L.Bimbot, M.Bolore, X.Charlot, J.Girard, J.M.Hisleur, J.C.Jourdain, J.Julien, A.Palmeri, G.S.Pappalardo, F.Reide, G.Sanouillet, N.Willis Inclusive (3He, π±) Reactions at 283 MeV NUCLEAR REACTIONS 12C, 27Al, 89Y, Pb(3He, π+), (3He, π-), E=283 MeV; measured σ(E(π), θ); deduced σ(θ), σ.
doi: 10.1016/0375-9474(86)90162-4
1984BE35 Nucl.Phys. A423, 511 (1984) V.Bernard, J.Girard, J.Julien, R.Legrain, J.Poitou, A.Oskarsson, L.Carlen, H.-A.Gustafsson, B.Jakobsson, P.Kristiansson, B.Noren, I.Otterlund, H.Ryde, T.Johansson, G.Tibell, R.Bertholet, C.Guet, M.Maurel, H.Nifenecker, P.Perrin, F.Schussler, M.Buenerd, D.Lebrun, P.Martin, G.Lovhoiden, J.P.Bondorf, O.-B.Nielsen, A.Palmeri Production of Charged Pions in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 7Li, 12C, 208Pb(12C, π+), E=60, 75, 85 MeV/nucleon; measured production σ(θ), σ(θ, E(π)); deduced (π-/π+) ratio.
doi: 10.1016/0375-9474(84)90038-1
1981BO15 Z.Phys. A299, 263 (1981) B.Borderie, M.Berlanger, D.Gardes, F.Hanappe, L.Nowicki, J.Peter, B.Tamain, S.Agarwal, J.Girard, C.Gregoire, J.Matuszek, C.Ngo A Possible Mechanism in Heavy Ion Induced Reactions: 'Fast fission process' NUCLEAR REACTIONS, Fission 165Ho(40Ar, F), E=180, 200, 230, 243, 280, 315, 340, 391 MeV; 181Ta(24Mg, F), E=270, 335, 340 MeV; Re(20Ne, F), E=124, 206 MeV; measured σ(fusion), L(critical), fragment mass vs compound nucleus excitation, angular momentum; deduced fast fission process.
doi: 10.1007/BF01443944
1981MA03 Nucl.Instrum.Methods 180, 141 (1981) G.Mariolopoulos, J.P.Bocquet, R.Brissot, H.Nifenecker, Ch.Ristori, A.Pequet, J.Girard A New Experimental Method to Measure the Charge Distributions of Fission Products RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(X-ray)-coin, fragment charge distribution; deduced yields for Rb, Sr, Y, Zr, Nb, Mo, Tc, Ru, Rh, Pd, Ag. ΔE-E telescope, X-ray detector.
doi: 10.1016/0029-554X(81)90021-5
1980AG06 Z.Phys. A296, 287 (1980) S.Agarwal, J.Galin, B.Gatty, D.Guerreau, M.Lefort, X.Tarrago, R.Babinet, J.Girard The Influence of the Entrance Channel Mass Asymmetry on the Reaction Mechanism: Investigated on the 16O+92Mo and 52Cr+56Fe Systems NUCLEAR REACTIONS, Fission 92Mo(16O, X), (16O, F), E=187 MeV; 56Fe(52Cr, X), (52Cr, F), E=264 MeV; measured evaporation residue σ(θ), σ(fragment θ, Z); deduced reaction mechanism, entrance channel mass asymmetry effects on fission.
doi: 10.1007/BF01438522
1980BA15 Z.Phys. A295, 153 (1980) R.Babinet, B.Cauvin, J.Girard, J.M.Alexander, T.H.Chiang, J.Galin, B.Gatty, D.Guerreau, X.Tarrago Light Particle Emission in Deeply Inelastic Collisions of 280 MeV 40Ar + 58Ni: Thermal Equilibrium and Angular Momentum Transfer NUCLEAR REACTIONS 58Ni(40Ar, αX), (40Ar, pX), E=280 MeV; measured αX(θ), pX(θ), in-plane, out-of-plane, σ(fragment θ, Eα, θα), σ(fragment θ, Ep, θp); deduced reaction mechanism.
doi: 10.1007/BF01413073
1980GU09 Z.Phys. A295, 105 (1980) D.Guerreau, J.Galin, B.Gatty, X.Tarrago, J.Girard, R.Lucas, C.Ngo Seven New Neutron Rich Nuclides Observed in Deep Inelastic Collisions Of 340 MeV 40Ar on 238U NUCLEAR REACTIONS 238U(40Ar, X), E=340 MeV; measured σ for 54Ti, 56V, 58,59Cr, 61Mn, 63,64Fe. deep-inelastic collisions.
1979AU03 Z.Phys. A289, 255 (1979) P.Auger, T.H.Chiang, J.Galin, B.Gatty, D.Guerreau, E.Nolte, J.Pouthas, X.Tarrago, J.Girard Observation of New Nuclides 37Si, 40P, 41S, 42S Produced in Deeply Inelastic Reactions Induced by 40Ar on 238U NUCLEAR REACTIONS 238U(Ar, X), E=263 MeV; measured fractional-charge parameter versus A; deduced evidence for 37Si, 30P, 41,42S. Tof measurements.
doi: 10.1007/BF01415785
1979BI02 Nucl.Phys. A318, 215 (1979) R.Bimbot, M.F.Rivet, J.Girard, R.Lucas, J.Poitou Complete Fusion and Transfer Reactions Induced by 273 MeV 40Ar on 159Tb NUCLEAR REACTIONS 159Tb(40Ar, X), E=273 MeV; measured projected ranges, σ(E(recoil), Z, θ), Z=45-80, off line X-ray spectrometry. Compared calculated distributions for transfer products.
doi: 10.1016/0375-9474(79)90480-9
1979CH27 Phys.Rev. C20, 1408 (1979) T.H.Chiang, D.Guerreau, P.Auger, J.Galin, B.Gatty, X.Tarrago, J.Girard Isotopic Distributions in Deep Inelastic Reactions Induced by Heavy Ions and the Relaxation of the Neutron Excess Degree of Freedom NUCLEAR REACTIONS 197Au(40Ar, X), E=217 MeV; 232Th(40Ar, X), E=295 MeV; 197Au(63Cu, X), E=445 MeV; 238U(40Ar, X), E=263 MeV; 238U(32S, X), E=241 MeV; measured σ(A, Z). Classical model of deep-inelastic collisions.
doi: 10.1103/PhysRevC.20.1408
1979LU06 Nucl.Phys. A321, 501 (1979) Evaporation Residue Excitation Functions from Fusion of 63Cu with 65Cu NUCLEAR REACTIONS 65Cu(63Cu, X), E not given; measured σ for evaporation residues for excitation energy=55-105 MeV, mass distributions; deduced fission barrier parameters.
doi: 10.1016/0375-9474(79)90141-6
1978BA14 Nucl.Phys. A296, 160 (1978) R.Babinet, B.Cauvin, J.Girard, H.Nifenecker, B.Gatty, D.Guerreau, M.Lefort, X.Tarrago Coincidence Study of the Deep Inelastic Collisions in the 40Ar + 58Ni System at 280 MeV NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; measured masses, kinetic energies, charge 6 ≤ Z ≤ 21; deduced mass evaporated by the light fragment.
doi: 10.1016/0375-9474(78)90419-0
1977AG04 Nucl.Phys. A293, 230 (1977) S.Agarwal, J.Galin, B.Gatty, D.Guerreau, M.Lefort, X.Tarrago, R.Babinet, B.Cauvin, J.Girard, H.Nifenecker Evidence for a Short Lifetime and a Long Lifetime Regime in the Deep Inelastic Collisions between 40Ca and 64Ni at 182 MeV NUCLEAR REACTIONS 64Ni(40Ca, X), E=182 MeV; measured σ(E, Z, θ), Z=6-27. Enriched target.
doi: 10.1016/0375-9474(77)90489-4
1977GA19 Z.Phys. A283, 173 (1977) J.Galin, B.Gatty, D.Guerreau, M.Lefort, X.Tarrago, S.Agarwal, R.Babinet, B.Cauvin, J.Girard, H.Nifenecker Fusion and Deep Inelastic Collisions Studied on the Ar + Au System II. Charge and Mass Analysis at 217 MeV Bombarding Energy NUCLEAR REACTIONS 197Au(40Ar, X), E=217 MeV; measured σ(A, Z, θ).
doi: 10.1007/BF01418709
1976GA25 Z.Phys. A278, 347 (1976) J.Galin, B.Gatty, D.Guerreau, M.Lefort, X.Tarrago, R.Babinet, B.Cauvin, J.Girard, H.Nifenecker The Transition between Quasi Elastic and Completely Damped Collisions Studied in the 40Ar (280 MeV) + 58Ni Reaction NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; measured σ(Z, θ).
doi: 10.1007/BF01437748
1975GA09 Z.Phys. A273, 65 (1975) B.Gatty, D.Guerreau, M.Lefort, J.Pouthas, X.Tarrago, J.Galin, B.Cauvin, J.Girard, H.Nifenecker Evidence for the Temporary Existence of a 'Composite' System in Deep Inelastic Nuclear Interactions NUCLEAR REACTIONS 58,64Ni(40Ar, X), (40Ca, X), E=280 MeV; measured σ(fragment mass).
doi: 10.1007/BF01435759
1975GA20 Nucl.Phys. A253, 511 (1975) B.Gatty, D.Guerreau, M.Lefort, X.Tarrago, J.Galin, B.Cauvin, J.Girard, H.Nifenecker Deep Inelastic Collisions in the Interaction of 280 MeV 40Ar with 58Ni NUCLEAR REACTIONS 58Ni(40Ar, X), X from B to Ca with isotope identification, E=280 MeV; measured σ(E(fragment mass), θ). Enriched target.
doi: 10.1016/0375-9474(75)90495-9
1974GA34 J.Phys.(Paris), Suppl.Lett. 35, L-117 (1974) B.Gatty, D.Guerreau, M.Lefort, J.Pouthas, X.Tarrago, J.Galin, B.Cauvin, J.Girard, H.Nifenecker Mass and Charge Identification of the Light Products of the Reaction 40Ar + (nat)Ni NUCLEAR REACTIONS Ni(40Ar, X), E=280 MeV; measured σ(E, E(fragment mass)) for Z < 21.
doi: 10.1051/jphyslet:01974003509011700
1970RI03 Nucl.Phys. A143, 130 (1970) Proprietes Statistiques des Parametres des Niveaux de 104Rh NUCLEAR REACTIONS 103Rh(n, X), (n, n), E < 4 keV; measured σ(nT), σ(nn). 104Rh deduced resonance parameters, J, L, average values.
doi: 10.1016/0375-9474(70)90686-X
1968IR02 Compt.Rend. 267B, 1358 (1968) J.-L.Irigaray, G.-Y.Petit, R.Samama, P.Carlos, J.Girard, G.Perrin Intensites et Energies des Raies γ dans la Reaction Rb(n, γ)Rb NUCLEAR REACTIONS 85Rb(n, γ), E=0.058 eV; measured Eγ, Iγ; deduced Q. 86Rb deduced levels, J, π. Ge(Li) detector, natural target.
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