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hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorFARGET, F.
dc.contributor.authorCAAMANO, M.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorDELAUNE, O.
dc.contributor.authorB. TARASOV, O.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorDERKX, X.
hal.structure.identifierAval du cycle et Energie Nucléaire [ACEN]
dc.contributor.authorSCHMIDT, K.-H.
dc.contributor.authorM. AMTHOR, A.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorAUDOUIN, L.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorBACRI, C.-O.
hal.structure.identifierAval du cycle et Energie Nucléaire [ACEN]
dc.contributor.authorBARREAU, G.
hal.structure.identifierLaboratoire de physique corpusculaire de Caen [LPCC]
dc.contributor.authorBASTIN, B.
dc.contributor.authorBAZIN, Dominique
hal.structure.identifierNoyaux exotiques [NEX]
dc.contributor.authorBLANK, Bertram
dc.contributor.authorBENLLIURE, J.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorCACERES, L.
dc.contributor.authorCASAREJOS, E.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorCHBIHI, A.
dc.contributor.authorFERNANDEZ-DOMINGUEZ, B.
hal.structure.identifierDAM Île-de-France [DAM/DIF]
dc.contributor.authorGAUDEFROY, L.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorGOLABEK, C.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorGRÉVY, S.
hal.structure.identifierAval du cycle et Energie Nucléaire [ACEN]
dc.contributor.authorJURADO, B.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorKAMALOU, O.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorLEMASSON, A.
dc.contributor.authorLUKYANOV, S.
dc.contributor.authorMITTIG, W.
dc.contributor.authorJ. MORRISSEY, D.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorNAVIN, A.
dc.contributor.authorPEREIRA, J.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorPERROT, L.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorREJMUND, M.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorROGER, T.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorSAINT-LAURENT, M.G.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorSAVAJOLS, H.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorSCHMITT, C.
dc.contributor.authorSHERILL, B.M.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorSTODEL, C.
hal.structure.identifierDAM Île-de-France [DAM/DIF]
dc.contributor.authorTAIEB, J.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorTHOMAS, J.C.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorVILLARI, A.C.C.
dc.date.issued2013
dc.date.conference2012-06-01
dc.description.abstractEnDuring the fission process, the atomic nucleus deforms and elongates up to the two fragments inception and their final separation at the scission deformation. The evolution of the nucleus energy with deformation defines a potential energy landscape in the multidimensional deformation space. It is determined by the macroscopic properties of the nucleus, and is also strongly influenced by the single-particle structure of the nucleus, which modifies the macroscopic energy minima. The fission fragment distribution is a direct consequence of the deformation path the nucleus has encountered, and therefore is the most genuine experimental observation of the potential energy landscape of the deforming nucleus. Very asymmetric fusion-fission reactions at energy close to the Coulomb barrier, produce well-defined conditions of the compound nucleus formation, where processes such as quasi-fission, pre-equilibrium emission and incomplete fusion are negligible. In the same time, the excitation energy is sufficient to reduce significantly structural effects, and mostly the macroscopic part of the potential is responsible for the formation of the fission fragments. We use inverse kinematics combined with a spectrometer to select and identify the fission fragments produced in 238U+12C at a bombarding energy close to and well-above the Coulomb barrier. For the first time, the isotopic yields are measured over the complete atomic-number distribution, between Z=30 and Z=63. In the experimental set-up, it is also possible to identify transfer-induced reactions, which lead to low-energy fission
dc.language.isoen
dc.title.enIsotopic fission fragment distributions as a deep probe to fusion-fission dynamics
dc.typeCommunication dans un congrès
dc.identifier.doi10.1088/1742-6596/420/1/012119
dc.subject.halPhysique [physics]/Physique Nucléaire Expérimentale [nucl-ex]
dc.identifier.arxiv1209.0816
bordeaux.page012119
bordeaux.volume420
bordeaux.countryUS
bordeaux.conference.citySan Antonio
bordeaux.peerReviewedoui
hal.identifierin2p3-00703163
hal.version1
hal.invitednon
hal.proceedingsoui
hal.conference.end2012-06-01
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//in2p3-00703163v1
bordeaux.COinSctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.date=2013&rft.volume=420&rft.spage=012119&rft.epage=012119&rft.au=FARGET,%20F.&CAAMANO,%20M.&DELAUNE,%20O.&B.%20TARASOV,%20O.&DERKX,%20X.&rft.genre=unknown


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