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dc.contributor.authorCALINESCU, S.
dc.contributor.authorCACERES, L.
hal.structure.identifierNoyaux exotiques [NEX]
dc.contributor.authorGRÉVY, S.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorSORLIN, O.
dc.contributor.authorSOHLER, D.
dc.contributor.authorSTANOIU, M.
dc.contributor.authorNEGOITA, F.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorCLÉMENT, E.
dc.contributor.authorASTABATYAN, R.
dc.contributor.authorBORCEA, C.
dc.contributor.authorBORCEA, R.
dc.contributor.authorBOWRY, M.
dc.contributor.authorCATFORD, W.
dc.contributor.authorDOMBRADI, Z.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorFRANCHOO, S.
dc.contributor.authorGARCIA, R.
dc.contributor.authorGILLIBERT, R.
dc.contributor.authorGUERIN, H.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorTHOMAS, J.C.
dc.contributor.authorKUTI, I.
dc.contributor.authorLUKYANOV, S.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorLEPAILLEUR, A.
dc.contributor.authorMASLOV, V.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorMORFOUACE, P.
dc.contributor.authorMRAZEK, J.
dc.contributor.authorNIIKURA, M.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorPERROT, L.
dc.contributor.authorPODOLYAK, Z.
dc.contributor.authorPETRONEA, C.
dc.contributor.authorPENIONZHKEVICH, Y.
hal.structure.identifierGrand Accélérateur National d'Ions Lourds [GANIL]
dc.contributor.authorROGER, T.
dc.contributor.authorROTARU, F.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorSTEFAN, I.
dc.contributor.authorVAJTA, Z.
dc.contributor.authorWILSON, E.
dc.date.issued2014
dc.date.conference2013-09-01
dc.description.abstractEnThe preliminary value of the reduced transition probability B(E2; 0+ ! 2+1 ) in 46Ar has been determined using the Coulomb excitation technique at intermediate energy. The 46Ar was produced in the fragmentation of a 48Ca beam at GANIL. The -rays following the Coulomb excitation of the 2+1 were emitted in-flight and detected by the 64 BaF2 detectors of the Château de Cristal array. The relatively low B(E2) value of 46Ar reported in this article supports the semi-magic character of this nucleus due to the persistence of the N = 28 shell closure at Z = 18.
dc.language.isoen
dc.title.enStudy of the neutron-rich isotope $^{46}$Ar through intermediate energy Coulomb excitation
dc.typeCommunication dans un congrès
dc.identifier.doi10.5506/APhysPolB.45.199
dc.subject.halPhysique [physics]/Physique Nucléaire Expérimentale [nucl-ex]
bordeaux.page199
bordeaux.volume45
bordeaux.countryPL
bordeaux.conference.cityPiaski
bordeaux.peerReviewedoui
hal.identifierin2p3-00954485
hal.version1
hal.invitednon
hal.proceedingsoui
hal.conference.end2013-09-07
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//in2p3-00954485v1
bordeaux.COinSctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.date=2014&rft.volume=45&rft.spage=199&rft.epage=199&rft.au=CALINESCU,%20S.&CACERES,%20L.&GR%C3%89VY,%20S.&SORLIN,%20O.&SOHLER,%20D.&rft.genre=unknown


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