Abstract
We have done a study of the $B^- \to K^- \pi^0 X(3872)$ reaction by means of a triangle mechanism via the chain of reactions: $B^- \to K^- D^{*0}\bar D^{*0}$; $D^{*0} \to \pi^0 D^0$; $D^0\bar D^{*0}\to X(3872)$. We show that this mechanism generates a triangle singularity in the $\pi^0 X(3872)$ invariant mass for a very narrow window of the $X(3872)$ mass, around the present measured values, and show that the peak positions and the shape of the mass distributions are sensitive to the $X(3872)$ mass, such that a measurement of the reaction can serve to improve on the present values of this mass. In particular, we point out that the $X(3872)$ mass relative to the $D^0\bar D^{*0}$ threshold may be extracted from the asymmetry of the $\pi^0X$ line shape.
Highlights
Triangle singularities (TSs) in physical processes, introduced in the 1960s [1,2] and searched for in some reactions without much success [3,4], have undergone a spectacular revival in recent years
We show that this mechanism generates a triangle singularity in the π0Xð3872Þ invariant mass for a very narrow window of the Xð3872Þ mass, around the present measured values, and show that the peak positions and the shape of the mass distributions are sensitive to the Xð3872Þ mass, such that a measurement of the reaction can serve to improve on the present values of this mass
The lines are normalized with the maximum of the δX 1⁄4 0 keV case again
Summary
Triangle singularities (TSs) in physical processes, introduced in the 1960s [1,2] and searched for in some reactions without much success [3,4], have undergone a spectacular revival in recent years. [7,8,9] that the peak corresponded to the πf0ð980Þ decay mode of the a1ð1260Þ due to a TS Another example was the explanation due to a TS [10,11,12,13,14] of the spectacular enhancement of the isospin forbidden ηð1405Þ decay into π0f0ð980Þ compared to π0a0ð980Þ [15]. It is shown there that some reactions involving TSs, which are in the vicinity of the physical region, serve to enhance the production of hadronic molecules. This would be the case of the Xð4260Þ → γXð3872Þ proposed in.
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