NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = Y.Llabador Found 16 matches. 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
1984CA31 Nucl.Phys. A427, 173 (1984) C.Cabot, H.Gauvin, Y.Le Beyec, H.Delagrange, J.P.Dufour, Y.Llabador, A.Fleury, J.M.Alexander Measurements of Evaporation Residues and Fission for 40Ar + 110Pd NUCLEAR REACTIONS 110Pd(40Ar, X), (40Ar, F), E=164-262 MeV; measured fission fragment σ(θ), evaporation residue σ(θ), fusion σ; deduced evaporation residue, fission spin zones. Different theoretical models.
doi: 10.1016/0375-9474(84)90144-1
1984DE39 Nucl.Phys. A429, 173 (1984) H.Delagrange, A.Benachou, F.Hubert, Y.Llabador, B.Heusch, J.P.Coffin, P.Engelstein, P.Fintz, G.Guillaume Statistical Decay of 193Au, 194Hg and 198Hg Compound Nuclei NUCLEAR REACTIONS, ICPND 181Ta(12C, F), E=60-110 MeV; 182W(12C, F), E=70-130 MeV; 186W(12C, F), E=80-100 MeV; measured fission σ(E). 181Ta(12C, X), E=105 MeV; measured σ(fragment θ, E), σ(fragment θ, mass). 182W(12C, X), E=98.7 MeV; measured evaporation residue σ(θ). 181Ta, 182,186W(12C, α), E=80, 98.7 MeV; measured σ; deduced fission mechanism, fusion σ. Statistical decay.
doi: 10.1016/0375-9474(84)90154-4
1982DU02 Phys.Lett. 109B, 265 (1982) J.P.Dufour, H.Delagrange, R.Del Moral, A.Fleury, F.Hubert, Y.Llabador, M.B.Mauhourat Production of α Emitters in Interactions of 86 MeV/u 12C on Targets of Mass 166-186 NUCLEAR REACTIONS 182,186W, 176Yb, 169Tm, 181Ta(12C, X), E=1 GeV; measured σ(fragment θ), recoil ranges; deduced production σ for 151Dy, 152Ho, 153Er, 155Yb, 156Lu, 157Hf. Activation technique. Intranuclear casade mechanism.
doi: 10.1016/0370-2693(82)90432-4
1982DU15 Nucl.Phys. A387, 157c (1982) J.P.Dufour, H.Delagrange, R.Del Moral, A.Fleury, F.Hubert, Y.Llabador, M.B.Mauhourat, K.H.Schmidt, A.Lleres Cross Sections and Dynamical Properties of α Emitters Produced in Interactions of 12C at 86 MeV/n on Medium and Heavy Targets NUCLEAR REACTIONS Dy, Ho, Er, Tm, Yb, Ta, Pt, Au, Pb(12C, X)156Lu/155Yb/154Tm/154mTm/151Dy/153Er/152Ho/152mHo, E=1 GeV; measured production σ(E) for residuals. Activation technique, on-line electrostatic collection. Intranuclear cascade, abrasion-ablation model.
doi: 10.1016/0375-9474(82)90198-1
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
1980CA27 J.Phys.(Paris), Colloq.C-10, 234 (1980) C.Cabot, H.Gauvin, Y.Le Beyec, H.Delagrange, J.P.Dufour, A.Fleury, Y.Llabador, J.M.Alexander Evaporation Residue and Fission Cross-Sections for the System: 40Ar + 110Pd NUCLEAR REACTIONS, Fission 110Pd(40Ar, xn), (40Ar, xnp), (40Ar, xnα), (40Ar, X), (40Ar, F), E=140-260 MeV; 130Te(40Ar, X), (40Ar, F), (40Ar, xn), (40Ar, xnp), E=164.5-226 MeV; measured σ(evaporation residue), σ(fission), σ(fusion) vs E. 150Gd deduced fission characteristics. Statistical model.
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
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
1975SC11 Rev.Phys.Appl. 10, 121 (1975) J.P.Schunck, J.M.Friedt, Y.Llabador Spectroscopie Mossbauer de 57Fe et 119Sn par Detection des Electrons de Conversion et Auger; Application a des Etudes de Surface NUCLEAR REACTIONS 57Fe, 119Sn(γ, γ'); measured ce-, Mossbauer-spectrum.
doi: 10.1051/rphysap:01975001003012100
1974LL01 J.Inorg.Nucl.Chem. 36, 2453 (1974) Mossbauer Emission Spectroscopy of 119Sb-Labelled Antimony(III) Oxide, Suphate and Helides NUCLEAR REACTIONS 119Sn(γ, γ); measured Mossbauer effect. 119Sn levels deduced quadrupole splitting.
doi: 10.1016/0022-1902(74)80452-5
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