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NSR database version of April 27, 2024.

Search: Author = Y.Llabador

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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
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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 ^{142,143,144,145,146}Nd, ^{144,147,148,149,150}Sm, ^151,153Eu, ¹⁵⁵Gd(Ar, X), E=275, 245 MeV; ¹³⁹La, ^140,142Ce, ¹⁴¹Pr, ^148,150Nd, ^{154,156,157,158,160}Gd, ¹⁵⁹Tb, ^152,154Sm(Ar, X), E=275 MeV; ^{142,143,144,145,146}Nd, ^{144,147,148,149,150,152}Sm(Cr, X), E=332 MeV; ^{142,144,146,148}Nd, ^{148,149,150,152,154}Sm(Fe, X), E=356 MeV; ^140,142Ce, ^{142,144,146,148}Nd, ^{144,148,149,150,152}Sm, ^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 ^{207,208,209,210,211}At, 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)

Y.Llabador

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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