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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