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NSR database version of May 23, 2024.

Search: Author = Y.Llabador

Found 16 matches.

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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

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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