NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Babinet Found 18 matches. 1994CO15 Nucl.Phys. A579, 369 (1994) C.Comptour, J.Augerat, J.Berthot, P.Bertin, K.Bouyakhlef, H.Fonvieille, G.Audit, R.Babinet, G.Fournier, J.Gosset, M.C.Lemaire, D.L'Hote, B.Mayer, J.Poitou, B.Saghai, F.Brochard, J.M.Durand, Z.Fodor, J.Yonnet A Study of the pp → ppπ0 Reaction at 800 MeV Beam Energy Using the DIOGENE Detector at Saturne NUCLEAR REACTIONS 1H(polarized p, pπ0), E=800 MeV; measured total σ, σ(E(π)), analyzing power; deduced Δ contribution dominance.
doi: 10.1016/0375-9474(94)90913-X
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
1987NG01 Nucl.Phys. A464, 717 (1987) Nguyen Van Sen, Ye Yanlin, J.Arvieux, G.Gaillard, B.Bonin, A.Boudard, G.Bruge, J.C.Lugol, T.Hasegawa, F.Soga, L.E.Antonuk, J.M.Cameron, S.T.Lam, G.C.Neilson, G.Roy, D.M.Sheppard, R.Babinet Elastic Scattering of Polarized Deuterons from 16O at 200, 400 and 700 MeV NUCLEAR REACTIONS 16O(polarized d, d), E=200, 400, 700 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters, total reaction σ. Glauber model. Energy-loss spectrometer, water target.
doi: 10.1016/0375-9474(87)90372-1
1985NG01 Phys.Lett. 156B, 185 (1985) Nguyen Van Sen, J.Arvieux, Ye Yanlin, G.Gaillard, B.Bonin, A.Boudard, G.Bruce, J.C.Lugol, R.Babinet, T.Hasegawa, F.Soga, J.M.Cameron, G.C.Neilson, D.M.Sheppard Elastic Scattering of Polarized Deuterons from 40Ca and 58Ni at Intermediate Energies NUCLEAR REACTIONS 58Ni(polarized d, d), E=200, 400, 700 MeV; 40Ca(polarized d, d), E=700 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters, reaction σ(E) for 58Ni.
doi: 10.1016/0370-2693(85)91506-0
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
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
1978CA09 Nucl.Phys. A301, 511 (1978) B.Cauvin, R.C.Jared, P.Russon, R.P.Schmitt, R.Babinet, L.G.Moretto Binary Aspects and Particle Multiplicities of the Fragments from (nat)Ag + 340 MeV 40Ar Deep Inelastic Collisions NUCLEAR REACTIONS Ag(40Ar, X), E=340 MeV; measured binary events 10 ≤ Z ≤ 32; deduced masses of fragments before evaporation, mass loss due to evaporation.
doi: 10.1016/0375-9474(78)90065-9
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
1977SC06 Nucl.Phys. A279, 141 (1977) R.P.Schmitt, P.Russo, R.Babinet, R.Jared, L.G.Moretto Nuclear Relaxation Phenomena, Diffusion and Orbiting in the Reaction 107,109Ag + 84,86Kr at 7.2 MeV/Nucleon NUCLEAR REACTIONS 107,109Ag(84Kr, X), (86Kr, X), E=606, 620 MeV; measured σ(E, θ, Z), Z=9-50.
doi: 10.1016/0375-9474(77)90426-2
1976BA08 Nucl.Phys. A258, 172 (1976) R.Babinet, L.G.Moretto, J.Galin, R.Jared, J.Moulton, S.G.Thompson Diffusion Processes in the Relaxed Cross Section for the Reaction 107,109Ag + 20Ne NUCLEAR REACTIONS 107,109Ag(20Ne, X), E=175, 252 MeV; measured σ(E, Z, θ), Z ≤ 32.
doi: 10.1016/0375-9474(76)90538-8
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
1976MO05 Nucl.Phys. A259, 173 (1976) L.G.Moretto, J.Galin, R.Babinet, Z.Fraenkel, R.Schmitt, R.Jared, S.G.Thompson Potential Energy Effects and Diffusion in the Relaxed Components of the Reaction 197Au + 40Ar at 288 and 340 MeV Bombarding Energies NUCLEAR REACTIONS 197Au(40Ar, X), E=288, 340 MeV; measured σ(E(fragment Z), θ), Z ≤ 32.
doi: 10.1016/0375-9474(76)90502-9
1975GA21 Nucl.Phys. A255, 472 (1975) J.Galin, L.G.Moretto, R.Babinet, R.Schmitt, R.Jared, S.G.Thompson Evidence of Incomplete Relaxation in the Reaction Ag+40Ar at 288 and 340 MeV Bombarding Energies NUCLEAR REACTIONS 107,109Ag(40Ar, X), E=288, 340 MeV; measured σ(E(fragment mass), θ), Z ≤ 30.
doi: 10.1016/0375-9474(75)90694-6
1975MO25 Phys.Lett. 58B, 31 (1975) L.G.Moretto, R.P.Babinet, J.Galin, S.G.Thompson Experimental Evidence of a Diffusion Process Associated with the Mass Asymmetry Degree of Freedom in Heavy Ion Reactions NUCLEAR REACTIONS 107,109Ag(14N, X), E=160 MeV; 107,109Ag(20Ne, X), E=252 MeV; 107,109Ag(40Ar, X), E=228 MeV; measured σ(fragment mass, θ).
doi: 10.1016/0370-2693(75)90719-4
1970QU05 Nucl.Phys. A156, 365 (1970) Nilsson's Hamiltonian in the Asymptotic Basis NUCLEAR STRUCTURE 25Al, 169Tm; calculated total energy vs deformation.
doi: 10.1016/0375-9474(70)90148-X
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