Coulomb Energy Differences in T=1 Mirror Rotational Bands in 50Fe and 50Cr

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dc.contributor.authorLenzi, S.M.
dc.contributor.authorMarginean, N.
dc.contributor.authorNapoli, D.R.
dc.contributor.authorUr, C.A.
dc.contributor.authorZuker, A.P.
dc.contributor.authorde Angelis, G.
dc.contributor.authorAlgora, A.
dc.contributor.authorAxiotis, M.
dc.contributor.authorBazzacco, D.
dc.contributor.authorBelcari, N.
dc.contributor.authorBentley, M.A.
dc.contributor.authorBizzetti, P.G.
dc.contributor.authorBizzetti-Sona, A.
dc.contributor.authorBrandolini, F.
dc.contributor.authorvon Brentano, P.
dc.contributor.authorBucurescu, D.
dc.contributor.authorCameron, J.A.
dc.contributor.authorChandler, C.
dc.contributor.authorDe Poli, M.
dc.contributor.authorDewald, A.
dc.contributor.authorEberth, H.
dc.contributor.authorFarnea, E.
dc.contributor.authorGadea, A.
dc.contributor.authorGarces-Narro, J.
dc.contributor.authorGelletly, W.
dc.contributor.authorGrawe, H.
dc.contributor.authorIsocrate, R.
dc.contributor.authorJoss, D.T.
dc.contributor.authorKalfas, C.A.
dc.contributor.authorKlug, T.
dc.contributor.authorLampman, T.
dc.contributor.authorLunardi, S.
dc.contributor.authorMartinez, T.
dc.contributor.authorMartinez-Pinedo, G.
dc.contributor.authorMenegazzo, R.
dc.contributor.authorNyberg, J.
dc.contributor.authorPodolyak, Zs.
dc.contributor.authorPoves, A.
dc.contributor.authorRibas, R.V.
dc.contributor.authorRossi Alvarez, C.
dc.contributor.authorRubio, B.
dc.contributor.authorSanchez-Solano, J.
dc.contributor.authorSpolaore, P.
dc.contributor.authorSteinhardt, T.
dc.contributor.authorThelen, O.
dc.contributor.authorTonev, D.
dc.contributor.authorVitturi, A.
dc.contributor.authorvon Oertzen, W.
dc.contributor.authorWeiszflog, M.
dc.date.accessioned2024-02-07T18:05:52Z
dc.date.available2024-02-07T18:05:52Z
dc.date.issued2001-08-28
dc.description.abstractGamma rays from the N=Z-2 nucleus 50Fe have been observed, establishing the rotational ground state band up to the state Jp=11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror 50Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations,incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model spacees_ES
dc.description.sponsorshipERBFMCT980110 E.U. TMRes_ES
dc.identifier.citation10.1103/PhysRevLett.87.122501es_ES
dc.identifier.issn0031-9007
dc.identifier.urihttps://hdl.handle.net/20.500.14855/2411
dc.language.isoenges_ES
dc.publisherThe American Physical Societyes_ES
dc.relation.ispartofseriesPhysical Review Letters;87
dc.rights.accessRightsopen accesses_ES
dc.subjectNuclear structurees_ES
dc.subjectCoulomb energy differenceses_ES
dc.subjectMirror nucleies_ES
dc.subjectShell modeles_ES
dc.titleCoulomb Energy Differences in T=1 Mirror Rotational Bands in 50Fe and 50Cres_ES
dc.typejournal articlees_ES

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