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hal.structure.identifierLaboratoire Matière sous Conditions Extrêmes [LMCE]
dc.contributor.authorCHATILLON, A.
hal.structure.identifierLaboratoire Matière sous Conditions Extrêmes [LMCE]
dc.contributor.authorTAÏEB, J.
dc.contributor.authorHEINZ, A.
dc.contributor.authorALVAREZ-POL, H.
hal.structure.identifierLaboratoire de Physique des 2 Infinis Irène Joliot-Curie [IJCLab]
dc.contributor.authorAUDOUIN, L.
dc.contributor.authorAYYAD, Y.
hal.structure.identifierLaboratoire Matière sous Conditions Extrêmes [LMCE]
dc.contributor.authorBÉLIER, G.
dc.contributor.authorBENLLIURE, J.
hal.structure.identifierDirection des Applications Militaires [DAM]
dc.contributor.authorBOUTOUX, G.
dc.contributor.authorCAAMAÑO, M.
dc.contributor.authorCASAREJOS, E.
dc.contributor.authorCORTINA-GIL, D.
hal.structure.identifierLaboratoire Matière sous Conditions Extrêmes [LMCE]
dc.contributor.authorEBRAN, A.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorFARGET, F.
dc.contributor.authorFERNÁNDEZ-DOMÍNGUEZ, B.
hal.structure.identifierDirection des Applications Militaires [DAM]
dc.contributor.authorGORBINET, T.
hal.structure.identifierDirection des Applications Militaires [DAM]
dc.contributor.authorGRENTE, L.
dc.contributor.authorJOHANSSON, H.T.
hal.structure.identifierLaboratoire de Physique des Deux Infinis Bordeaux [LP2I - Bordeaux]
dc.contributor.authorJURADO, B.
dc.contributor.authorKELIĆ-HEIL, A.
dc.contributor.authorKURZ, N.
hal.structure.identifierLaboratoire Matière sous Conditions Extrêmes [LMCE]
dc.contributor.authorLAURENT, B.
hal.structure.identifierDirection des Applications Militaires [DAM]
dc.contributor.authorMARTIN, J.-F.
dc.contributor.authorNOCIFORO, C.
dc.contributor.authorPARADELA, C.
hal.structure.identifierDirection des Applications Militaires [DAM]
dc.contributor.authorPELLEREAU, E.
dc.contributor.authorPIETRI, S.
dc.contributor.authorPROCHAZKA, A.
dc.contributor.authorRODRÍGUEZ-SÁNCHEZ, J.L.
dc.contributor.authorROSSI, D.
dc.contributor.authorSIMON, H.
hal.structure.identifierLaboratoire de Physique des 2 Infinis Irène Joliot-Curie [IJCLab]
dc.contributor.authorTASSAN-GOT, L.
dc.contributor.authorVARGAS, J.
dc.contributor.authorVOSS, B.
dc.contributor.authorWEICK, H.
dc.date.accessioned2022-09-15T12:35:00Z
dc.date.available2022-09-15T12:35:00Z
dc.date.issued2022
dc.identifier.issn2469-9985
dc.identifier.urihttps://oskar-bordeaux.fr/handle/20.500.12278/145323
dc.description.abstractEnMean values of the number of protons and neutrons of the primary fission fragments at scission are determinedfor the asymmetric fission of 16 fissioning isotopes, from 219Ac up to 238Np. Our results confirm that the mainasymmetric fission mode around the heavier uranium isotopes is indeed characterized by an average atomicnumber around  ZH  = 54 in the heavy fission fragments. However, they also unambiguously show a stabilizationeffect in the light fission fragments around  NL  = 52–54 in the neutron-deficient thorium and actinium isotopes.This is a clear signature that these deformed proton and neutron shell closures around 54 play a major role inthe nuclear fission process. The evolution along the thorium chain shows that the neutron shell appears to bedominant in the asymmetric fission of the lighter thorium isotopes, in contrast to the heavier thorium isotopesfor which the stabilization originates from the proton shell.
dc.language.isoen
dc.publisherAmerican Physical Society
dc.title.enInfluence of proton and neutron deformed shells on the asymmetric fission of thorium isotopes
dc.typeArticle de revue
dc.identifier.doi10.1103/physrevc.106.024618
dc.subject.halPhysique [physics]/Physique Nucléaire Expérimentale [nucl-ex]
bordeaux.journalPhysical Review C
bordeaux.page024618
bordeaux.volume106
bordeaux.hal.laboratoriesLaboratoire de Physique des Deux Infinis de Bordeaux (LP2I) - UMR 5797*
bordeaux.issue2
bordeaux.institutionUniversité de Bordeaux
bordeaux.institutionCNRS
bordeaux.peerReviewedoui
hal.identifierhal-03766443
hal.version1
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-03766443v1
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