Predictions for the Bˉ0→Kˉ∗0X(YZ)\bar B^0 \to \bar K^{*0} X (YZ) and Bˉs0→ϕX(YZ)\bar B^0_s \to ϕX (YZ) with X(4160),Y(3940),Z(3930)X(4160), Y(3940), Z(3930)

preprint2015arXivOpen access

Abstract

We investigate the decay of Bˉ0→Kˉ∗0R\bar B^0 \to \bar K^{*0} R and Bˉs0→ϕR\bar B^0_s \to ϕR with RR being the X(4160)X(4160), Y(3940)Y(3940), Z(3930)Z(3930) resonances. Under the assumption that these states are dynamically generated from the vector-vector interaction, as has been concluded from several theoretical studies, we use a reaction mechanism of quark production at the elementary level, followed by hadronization of one final qqˉq \bar q pair into two vectors and posterior final state interaction of this pair of vector mesons to produce the resonances. With this procedure we are able to predict five ratios for these decays, which are closely linked to the dynamical nature of these states, and also predict the order of magnitude of the branching ratios which we find of the order of 10−410^{-4}, well within the present measurable range. In order to further test the dynamical nature of these resonances we study the Bˉs0→ϕD∗Dˉ∗\bar B^0_s \to ϕD^* \bar D^* and Bˉs0→ϕDs∗Dˉs∗\bar B^0_s \to ϕD_s^* \bar D_s^* decays close to the D∗Dˉ∗D^* \bar D^* and Ds∗Dˉs∗D_s^* \bar D_s^* thresholds and make predictions for the ratio of the mass distributions in these decays and the Bˉs0→ϕR\bar B^0_s \to ϕR decay widths. The measurement of these decays rates can help unravel the nature of these resonances.

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