Differences between the 3P0 and C3P0 model in the charming strange sector

dc.contributor.author	Silva, Daniel Tavares da	pt_BR
dc.contributor.author	Roschildt, Nathan	pt_BR
dc.contributor.author	Hadjimichef, Dimiter	pt_BR
dc.contributor.author	Rodrigues, Hercules Borges	pt_BR
dc.date.accessioned	2016-01-31T02:03:55Z	pt_BR
dc.date.issued	2015	pt_BR
dc.identifier.issn	1742-6588	pt_BR
dc.identifier.uri	http://hdl.handle.net/10183/132591	pt_BR
dc.description.abstract	The 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.mimetype	application/pdf	pt_BR
dc.language.iso	eng	pt_BR
dc.relation.ispartof	Journal of physics : conference series. Bristol. Vol. 630 (2015), 012038, 5 p.	pt_BR
dc.rights	Open Access	en
dc.subject	Formalismo de Fock-Tani	pt_BR
dc.subject	Mesons	pt_BR
dc.title	Differences between the 3P0 and C3P0 model in the charming strange sector	pt_BR
dc.title.alternative	Differences between the 3P0 and C3P0 model in the charming strange sector	en
dc.type	Artigo de periódico	pt_BR
dc.identifier.nrb	000982352	pt_BR
dc.type.origin	Estrangeiro	pt_BR

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