NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.Gardes Found 35 matches. 2007CH46 Nucl.Instrum.Methods Phys.Res. A577, 353 (2007) M.Chabot, D.Gardes, M.Nectoux, G.Maynard, C.Deutsch Energy loss of Clq+ (52 MeV) through dilute H2 target: Evidence of non-linear term and non-Coulombian potential contribution
doi: 10.1016/j.nima.2007.02.029
1997BO05 Z.Phys. A357, 7 (1997) B.Borderie, M.F.Rivet, P.Box, M.Dakowski, C.Cabot, Y.El Masri, F.Hanappe, D.Gardes, D.Jouan, G.Mamane, X.Tarrago, H.Utsunomiya Energy Relaxation Time in Heavy Ion Collisions between 27 and 44 MeV/u NUCLEAR REACTIONS Ag(40Ar, X), E=27, 44 MeV/nucleon; measured (fragment)(fragment)-coin, excitation energy sharing; deduced energy relaxation time. Landau-Vlasov simulations.
doi: 10.1007/s002180050206
1991BO15 Z.Phys. A338, 369 (1991) B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, D.Gardes, F.Hanappe, D.Jouan, M.Montoya Excitation Energy Partition in Deeply Inelastic Collisions between 40Ar and Ag at 27 MeV Per Nucleon NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment particle evaporation; deduced excitation energy partition features.
doi: 10.1007/BF01288204
1991JO12 Z.Phys. A340, 63 (1991) D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille Dynamics and Thermalization in Violent Collisions between 40Ar and Ag at 27 MeV/nucleon NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1007/BF01284482
1990JA07 Nucl.Phys. A511, 195 (1990) D.Jacquet, G.F.Peaslee, J.M.Alexander, B.Borderie, E.Duek, J.Galin, D.Gardes, C.Gregoire, D.Guerreau, H.Fuchs, M.Lefort, M.F.Rivet, X.Tarrago Production and Deexcitation of Hot Nuclei in Collisions of 27 MeV/Nucleon 40Ar with 238U NUCLEAR REACTIONS 238U(40Ar, F), (40Ar, X), E=1080 MeV; measured (fragment)(fragment)-, (light charged particle)(fragment)-coin following fission. Landau-Vlasov calculations.
doi: 10.1016/0375-9474(90)90032-H
1988BO13 Phys.Lett. 205B, 26 (1988) B.Borderie, M.Montoya, M.F.Rivet, D.Jouan, C.Cabot, H.Fuchs, D.Gardes, H.Gauvin, D.Jacquet, F.Monnet, F.Hanappe Deeply Inelastic Collisions as a Source of Intermediate Mass Fragments at E/A = 27 MeV NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment σ(θ1, θ2); deduced reaction mechanism.
doi: 10.1016/0370-2693(88)90393-0
1988RI06 Z.Phys. A330, 301 (1988) M.F.Rivet, R.Alami, B.Borderie, H.Fuchs, D.Gardes, H.Gauvin Fusion-Fission of Heavy Systems. Influence of the Entrance Channel Mass Asymmetry NUCLEAR REACTIONS 209Bi(40Ar, F), E=202, 238 MeV; 187Re(56Fe, F), E=294, 307, 326 MeV; measured fission σ, fragment mass distribution widths; deduced entrance channel role in fission.
1986RI06 Phys.Rev. C34, 1282 (1986) M.F.Rivet, B.Borderie, H.Gauvin, D.Gardes, C.Cabot, F.Hanappe, J.Peter Deexcitation of Nuclei Formed near the Instability Temperature NUCLEAR REACTIONS 165Ho, Ag(40Ar, X), E=1090 MeV; measured fragment σ(θ), mass distribution, velocity spectra, (fragment)(fragment)(θ); deduced reaction mechanism. Natural targets, TOF telescope, parallel plate avalanche counter.
doi: 10.1103/PhysRevC.34.1282
1985JA14 Nucl.Phys. A445, 140 (1985) D.Jacquet, J.Galin, M.F.Rivet, R.Bimbot, B.Borderie, D.Gardes, B.Gatty, D.Guerreau, L.Kowalski, M.Lefort, X.Tarrago Fission following Carbon Interactions on Gold and Uranium between 30 and 84 MeV/u NUCLEAR REACTIONS 197Au, 238U(12C, F), E=30, 60, 84 MeV/nucleon; measured binary fission fragment mass spectra; deduced fusion mechanism. 209At, 250Cf deduced excitation energy.
doi: 10.1016/0375-9474(85)90365-3
1984BI02 Nucl.Phys. A413, 489 (1984) R.Bimbot, D.Gardes, L.De Reilhac, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador Influence of the Potential Energy Surface on the Cross Sections for Deeply Inelastic Transfer Reactions Induced by Heavy Ions NUCLEAR REACTIONS, ICPND 148Sm(40Ca, X), E=193, 211, 236, 266 MeV; 144,150Sm, 142,144,146Nd(40Ca, X), E=211, 236 MeV; 154Sm(40Ca, X), E=236 MeV; 144Sm(40Ar, X), E=211, 245 MeV; measured production σ for 151,150Dy, 149Tb; deduced transfer reaction potential energy surface dependence, reaction mechanism.
doi: 10.1016/0375-9474(84)90423-8
1984BO17 Z.Phys. A316, 243 (1984) B.Borderie, M.F.Rivet, C.Cabot, D.Fabris, D.Gardes, H.Gauvin, F.Hanappe, J.Peter Heavy Products from Violent Collisions in the 40Ar + (nat)Ag System at 27 MeV/u NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured heavy evaporation residue σ(θ), velocity spectra vs mass; deduced reaction mechanism.
doi: 10.1007/BF01412271
1984BO35 Z.Phys. A318, 315 (1984) B.Borderie, M.F.Rivet, C.Cabot, D.Fabris, D.Gardes, H.Gauvin, F.Hanappe, J.Peter Light Fragments Produced in 40Ar + (nat)Ag Reactions at 27 MeV/u NUCLEAR REACTIONS Ag(40Ar, X), E=1.095 GeV; measured σ(fragment θ, E), fragment mass, energy distributions for Z=4-12; deduced light particle emission mechanism.
doi: 10.1007/BF01418089
1984JA16 Phys.Rev.Lett. 53, 2226 (1984) D.Jacquet, E.Duek, J.M.Alexander, B.Borderie, J.Galin, D.Gardes, D.Guerreau, M.Lefort, F.Monnet, M.F.Rivet, X.Tarrago Reaching the Capacity of a Composite Nucleus for Energy and Spin Containment NUCLEAR REACTIONS 238U(40Ar, αF), E=1080 MeV; measured fission (fragment)(fragment)(α)(θ); deduced reaction mechanism.
doi: 10.1103/PhysRevLett.53.2226
1984ZH04 Nucl.Phys. A422, 447 (1984) Z.Zheng, B.Borderie, D.Gardes, H.Gauvin, F.Hanappe, J.Peter, M.F.Rivet, B.Tamain, A.Zaric Further Experimental Evidence for Fast Fission NUCLEAR REACTIONS 238U, 209Bi(40Ar, X), (40Ar, F), E ≈ 175-350 MeV; 197Au(40Ar, X), (40Ar, F), E=150-350 MeV; measured (fragment)(fragment)-coin, fission type fragment mass energy distributions; deduced fusion σ(E), fast fission evidence.
doi: 10.1016/0375-9474(84)90526-8
1983BO14 Nucl.Phys. A402, 57 (1983) B.Borderie, M.F.Rivet, I.Forest, J.Galin, D.Guerreau, R.Bimbot, D.Gardes, B.Gatty, M.Lefort, H.Oeschler, S.Song, B.Tamain, X.Tarrago Emission of Light Charged Particles and Associated Heavy Partners in Reactions Induced on Ni by C Projectiles at 30, 60 and 84 MeV/u NUCLEAR REACTIONS Ni(12C, pX), (12C, dX), (12C, tX), (12C, 3HeX), (12C, αX), E=30, 60, 84 MeV/nucleon; measured(fragment)(fragment)-coin, σ(Ep), σ(Ed), σ(Et), σ(E3He), σ(α); deduced reaction mechanism.
doi: 10.1016/0375-9474(83)90562-6
1983SO07 Phys.Lett. 130B, 14 (1983) S.Song, M.F.Rivet, R.Bimbot, B.Borderie, I.Forest, J.Galin, D.Gardes, B.Gatty, M.Lefort, H.Oeschler, B.Tamain, X.Tarrago Evidence for the Formation of Highly Excited Compound-Like Nuclei (T≈5 MeV) in Collisions of 720 MeV C Projectiles with 238U, 232Th and 197Au Targets NUCLEAR REACTIONS 232Th(12C, pF), (12C, αF), E=720 MeV; measured fission fragment(p)-, (fragment)(α)-coin. 197Au, 238U(12C, F), E=720 MeV; measured fission (fragment)(fragment)(light particle)-coin; deduced reaction mechanism.
doi: 10.1016/0370-2693(83)91053-5
1982GA15 Phys.Rev.Lett. 48, 1787 (1982) J.Galin, H.Oeschler, S.Song, B.Borderie, M.F.Rivet, I.Forest, R.Bimbot, D.Gardes, B.Gatty, H.Guillemot, M.Lefort, B.Tamain, X.Tarrago Evidence for a Limitation of the Linear Momentum Transfer in 12C-Induced Reactions between 30 and 84 MeV/u NUCLEAR REACTIONS, Fission U, Au, Ni(12C, F), E=30-84 MeV/nucleon; measured σ(θ1, θ2) for fragment pair; deduced linear momentum transfer limitation. Surface barrier detectors.
doi: 10.1103/PhysRevLett.48.1787
1982RI01 Nucl.Phys. A379, 173 (1982) M.F.Rivet, R.Bimbot, D.Gardes, A.Fleury, F.Hubert, Y.Llabador Cross Sections for Deeply Inelastic Transfer Reactions induced by Heavy Ions in Rare-Earth Targets NUCLEAR REACTIONS 142,143,144,145,146Nd, 144,147,148,149,150Sm, 151,153Eu, 155Gd(Ar, X), E=275, 245 MeV; 139La, 140,142Ce, 141Pr, 148,150Nd, 154,156,157,158,160Gd, 159Tb, 152,154Sm(Ar, X), E=275 MeV; 142,143,144,145,146Nd, 144,147,148,149,150,152Sm(Cr, X), E=332 MeV; 142,144,146,148Nd, 148,149,150,152,154Sm(Fe, X), E=356 MeV; 140,142Ce, 142,144,146,148Nd, 144,148,149,150,152Sm, 151,153Eu, 154,156,158Gd(Cu, X), E=401 MeV; measured cumulative yields, production σ for 149,150,151Dy. Enriched targets, activation technique.
doi: 10.1016/0375-9474(82)90562-0
1982RI06 Z.Phys. A307, 365 (1982) M.F.Rivet, B.Gatty, H.Guillemot, B.Borderie, R.Bimbot, I.Forest, J.Galin, D.Gardes, D.Guerreau, M.Lefort, X.Tarrago, B.Tamain, L.Novicki Correlations between Fission Fragments and Light Charged-Particles in the Reaction 20Ne + 197Au at 13 MeV/Nucleon NUCLEAR REACTIONS 197Au(20Ne, pF), (20Ne, dF), (20Ne, tF), (20Ne, αF), E=265 MeV; measured fission fragment(light particle)-coin, σ(θp, Ep, fragment θ), σ(θα, Eα, fragment θ); deduced fission σ(total), fusion L(critical), reaction mechanism. 217Ac deduced fission characteristics, particle multiplicities. Rotating liquid drop model.
doi: 10.1007/BF01421298
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
1980BO27 Z.Phys. A298, 235 (1980) B.Borderie, R.Bimbot, C.Cabot, D.Gardes, L.Nowicki, B.Tamain, C.Gregoire, C.Ngo, M.Berlanger, F.Hanappe Limitation to the Fusion Cross Section for the System Mg + Cu at High Energy NUCLEAR REACTIONS Cu(24Mg, X), E=161-341 MeV; measured σ(θ) for evaporation residue, σ(fusion, E); deduced critical angular momentum. Sharp cutoff model.
doi: 10.1007/BF01418662
1980DU02 Z.Phys. A294, 107 (1980) J.P.Dufour, A.Fleury, F.Hubert, Y.Llabador, M.B.Mauhourat, R.Bimbot, D.Gardes New Isotope 184Pb RADIOACTIVITY 184Pb; measured Eα. NUCLEAR REACTIONS 147,148Sm(40Ca, xn), E=190-250 MeV; measured α yield vs E, αα(t); deduced evidence for 184Pb.
doi: 10.1007/BF01473127
1980GA13 Phys.Rev. C21, 2447 (1980) D.Gardes, R.Bimbot, J.Maison, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador Angular Distributions and Ranges of Heavy Products from Quasi-Elastic Transfer Reactions Induced by Heavy Ions in 209Bi NUCLEAR REACTIONS 209Bi(14N, X), E=74, 99 MeV; 209Bi(16O, X), E=85, 102 MeV; 209Bi(19F, X), E=95, 110 MeV; 209Bi(40Ar, X), E=203, 212, 275 MeV; 209Bi(40Ca, X), E=217 MeV; 197Au(16O, X), E=112 MeV; Tl(40Ar, X), E=242 MeV; measured production σ(θ), ranges for 210Po, 211At, 211Rn, 198,200Tl, 204Bi; deduced reaction mechanism.
doi: 10.1103/PhysRevC.21.2447
1980RI03 Z.Phys. A296, 201 (1980) M.F.Rivet, R.Bimbot, D.Gardes, G.Mouchaty, A.Fleury, F.Hubert, Y.Llabador Deeply Inelastic Transfer Reactions Induced by Heavy Ions in Rare-Earth Targets NUCLEAR REACTIONS 141Pr(40Ar, xnyp), E=278 MeV; 142,145Nd(40Ar, xnyp), E=276 MeV; 144,149Sm, 151Eu(40Ar, xnyp), E=275 MeV; 144Nd(52Cr, xnyp), E=331 MeV; 148Sm(52Cr, xnyp), E=332 MeV; 144Nd(56Fe, xnyp), E=364 MeV; 148Sm(56Fe, xnyp), E=289, 366 MeV; 144Nd(63Cu, xnyp), E=421 MeV; 148Sm(63Cu, xnyp), E=330, 421 MeV; measured production σ(θ, fragment E) for 150,151Dy, 149Tb; deduced damping level in deep inelastic transfer reactions.
doi: 10.1007/BF01415834
1979BI01 Z.Phys. A290, 157 (1979) R.Bimbot, D.Gardes, J.Cugnon, R.da Silveira Simple Formulae for Heavy Ion Subcoulomb Transfer Probabilities. Application to One and Two-Proton Transfers in Bismuth NUCLEAR REACTIONS 209Bi(14N, 13C), (14N, 12B), E=50-70 MeV; 209Bi(16O, 15N), (16O, 14C), E=70-80 MeV; 209Bi(19F, 18O), (19F, 17N), E=70-90 MeV; 209Bi(40Ar, 39Cl), (40Ar, 38S), E=150-170 MeV; 209Bi(40Ca, 39K), (40Ca, 38Ar), E=150-180 MeV; 209Bi(57Fe, 55Mn), (56Fe, 54Cr), E=200-230 MeV; 209Bi(63Cu, 62Ni), (63Cu, 61Co), E=220-250 MeV; calculated σ(E). DWBA approach.
doi: 10.1007/BF01408110
1979LL01 Z.Phys. A289, 173 (1979) Y.Llabador, F.Hubert, A.Fleury, D.Gardes, M.F.Rivet, R.Bimbot Angular Distribution Analysis for Quasi-Elastic Transfer Reactions Induced in 209Bi Targets with Heavy Ions NUCLEAR REACTIONS 209Bi(14N, 13C), (14N, 12B), E=74, 99 MeV; measured σ(θ). 209Bi(16O, 14C), E=83, 102 MeV; 209Bi(19F, 17N), E=95, 110 MeV; 209Bi(40Ar, 38S), E=203, 212, 275 MeV; 209Bi(40Ca, 38Ar), E=217 MeV; measured σ(θ). DWBA analysis of quasielastic transfer.
doi: 10.1007/BF01435935
1979RI05 Z.Phys. A290, 57 (1979) M.F.Rivet, R.Bimbot, D.Gardes, A.Fleury, F.Hubert, Y.Llabador Production of 149gTb in Deep Inelastic Transfer Reactions: An Approach to the Angular Momentum of Fragments NUCLEAR REACTIONS 142,145Nd, 144,148Sm, 154Gd(Ar, X), E=160-280 MeV; 144Nd, 148Sm, 151Eu, 154Gd(Cu, X), E=280-420 MeV; measured σ(E). 149Tb deduced production σ in deep-inelastic transfer reactions.
doi: 10.1007/BF01408480
1978GA17 Phys.Rev. C18, 1298 (1978) D.Gardes, R.Bimbot, J.Maison, L.de Reilhac, M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador Excitation Functions for Quasielastic Transfer Reactions Induced with Heavy Ions in Bismuth NUCLEAR REACTIONS 209Bi(12C, X), (14N, X), (16O, X), (19F, X), (20Ne, X), (40Ar, X), 209Bi(56Fe, X), (63Cu, X), E=4.5-10 MeV/nucleon; measured σ(E) for production of 207,208,209,210,211At, 211Rn.
doi: 10.1103/PhysRevC.18.1298
1977RI02 Nucl.Phys. A276, 157 (1977) M.F.Rivet, R.Bimbot, A.Fleury, D.Gardes, Y.Llabador Evolution from Deep Inelastic Transfer to Quasi-Fission NUCLEAR REACTIONS 148Sm(56Fe, X), E=300, 377 MeV; 148Sm(63Cu, X), E=342, 431 MeV; measured σ(E(recoil), θ) for production of 150,151Dy, 149gTb. Enriched targets.
doi: 10.1016/0375-9474(77)90164-6
1975BI11 Nucl.Phys. A248, 377 (1975) R.Bimbot, D.Gardes, R.L.Hahn, Y.De Moras, M.F.Rivet Recoil Study of Ar Induced Multinucleon Transfer Reactions. Capture of 1 to 9 Charges by Rare-Earth Targets NUCLEAR REACTIONS 139La, 140,142Ce, 141Pr, 144,147,148,149,150,152,154Sm, 151,153Eu, 154,155,156,157,158,160Gd, 159Tb(Ar, X), E=282 MeV; measured σ, σ(E(recoil), θ) for production of 151Dy, 150Dy, 149gTb. Enriched targets.
doi: 10.1016/0375-9474(75)90171-2
1975GA04 J.Phys.(Paris), Suppl.Lett. 36, L-59 (1975) D.Gardes, R.Bimbot, A.Fleury, F.Hubert, M.F.Rivet Influence of Energetics on the Thresholds of Heavy Ion Transfer Reactions NUCLEAR REACTIONS 209Bi(14N, 13C), (14N, 12B), (16O, 15N), (16O, 14C), E=50-110 MeV; calculated interaction potential.
doi: 10.1051/jphyslet:0197500360305900
1974BI11 Nucl.Phys. A228, 85 (1974) R.Bimbot, D.Gardes, R.L.Hahn, Y.de Moras, M.F.Rivet Recoil Study of Multinucleon Transfer Reactions: Capture of Six Charges by Nd Targets in Ar Induced Reactions NUCLEAR REACTIONS 142,143,144,145,146,148,150Nd(40Ar, X), E=257, 282 MeV; measured σ(E), σ(E(recoil), θ). Enriched targets.
doi: 10.1016/0375-9474(74)90447-3
1972BI10 Nucl.Phys. A189, 193 (1972) Recoil Study of Transfer Reactions: Evidence for α and 8Be Transfers in 12C Reactions with Heavy Nuclei (Au, Bi) NUCLEAR REACTIONS 197Au, 209Bi(12C, αxn); 197Au, 209Bi(12C, 8Bexn), E(12C)=60-90 MeV; measured σ(E), σ(θ), recoil ranges.
doi: 10.1016/0375-9474(72)90654-9
1971BI14 Phys.Rev. C4, 2180 (1971) Excitation Function and Recoil Ranges of 211At Produced Through 40Ar + 209Bi Transfer Reactions NUCLEAR REACTIONS 209Bi(40Ar, X), E=190-270 MeV; measured recoil ranges, σ(E) for 211At production.
doi: 10.1103/PhysRevC.4.2180
1971BI16 C.R.Acad.Sci., Ser.B, 273, 505 (1971) R.Bimbot, C.Deprun, D.Gardes, H.Gauvin, Y.Le Beyec, M.Lefort, J.Peter, B.Tamain Experiences Preliminaires sur les Reactions Nucleaires Induites par un Faisceau d'Ions Krypton de 450 a 500 MeV. Premiers Indices en Faveur de la Synthese de Noyaux Superlourds NUCLEAR REACTIONS 74Ge, 116Cd, Th, U(Kr, X), E=450-500 MeV; measured charged particle spectra. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2216. Back to query form |