Speaker
Description
The presence of New Physics contribution to loop diagram-induced $b \to s \bar{s} s$ transitions can lead to a noticeable direct $CP$ violation in $B^+ \to K^+ K^+ K^-$ if not only the weak but also the strong phase of the New Physics are different from the Standard Model phase. We show that by using a resonance in the $K^+ K^-$ system from the tree diagram $b \to c \bar{c} s$, for example $\chi_{c0}(1P)$, we can significantly expand the possibilities of the method for NP searching in this final state. Due to the changing strong phase near the resonance pole, automatic scanning occurs over all possible values of the difference between the strong phases of the Standard Model and NP. In addition, the strongly changing resonance amplitude allows for the enhancement of the $CP$ violation effect in separate areas of the phase volume, due to the fact that the amplitudes of the SM and NP will be comparable.
