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dc.contributor.authorSilva, Daniel Tavares dapt_BR
dc.contributor.authorRoschildt, Nathanpt_BR
dc.contributor.authorHadjimichef, Dimiterpt_BR
dc.contributor.authorRodrigues, Hercules Borgespt_BR
dc.date.accessioned2016-01-31T02:03:55Zpt_BR
dc.date.issued2015pt_BR
dc.identifier.issn1742-6588pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/132591pt_BR
dc.description.abstractThe goal of this work is to establish a comparison between the very well studied 3P0 model and a bound-state corrected version, the C3P0 model, obtained from applying the Fock- Tani transformation to the 3P0 model, in the context of the charmed-strange meson sector (DSJ meson). In particular, we shall calculate the decay amplitudes and decay rates of the Ds1(2460)+ ! D + s 0 and Ds1(2536)+ ! D (2010)+K0, showing the differences between the two models.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofJournal of physics : conference series. Bristol. Vol. 630 (2015), 012038, 5 p.pt_BR
dc.rightsOpen Accessen
dc.subjectFormalismo de Fock-Tanipt_BR
dc.subjectMesonspt_BR
dc.titleDifferences between the 3P0 and C3P0 model in the charming strange sectorpt_BR
dc.title.alternativeDifferences between the 3P0 and C3P0 model in the charming strange sector en
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000982352pt_BR
dc.type.originEstrangeiropt_BR


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