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Search: Author = D.Gardes

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0113.

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1972BI10      Nucl.Phys. A189, 193 (1972)

R.Bimbot, D.Gardes, M.F.Rivet

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0126.

1971BI14      Phys.Rev. C4, 2180 (1971)

R.Bimbot, D.Gardes, M.F.Rivet

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0034.

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.

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