TThe LHCb collaboration has recently reported evidence for non-zero CP asymmetries in decays into $\pi^+ K^+ K^-,; \pi^+\pi^+\pi^-,; K^+ K^+ K^- K^+\pi^+\pi^-$. The branching ratios for these decays have also been measured with different values ranging from to $51\times 10^{-6}SU(3)B$ decays, in the case that the dominant amplitude is momentum independent it is expected that branching ratios and CP violating rate differences $\Delta_{CP} = \Gamma - \overline{\Gamma}Br(\pi^+\pi^+\pi^-) = 2Br(\pi^+ K^+ K^-)Br(K^+K^+K^-) = 2 Br(K^+\pi^+\pi^-)\Delta_{CP}(\pi^+\pi^+\pi^-) = 2\Delta_{CP}(\pi^+ K^+K^-) = - \Delta_{CP}(K^+K^+K^-) = -2\Delta_{CP}(K^+\pi^+\pi^-)$. The experimental data do not exhibit the expected pattern for the branching ratios. The rate differences for $B^+\to \pi^+\pi^+\pi^-B^+\to K^+ K^+ K^-\Delta S =0\Delta S=1$ well, but the other two do not, with the CP asymmetries having different signs than expected. In this work we study how to including momentum dependent and also breaking effects on these decays to explain experimental data. We find that only including lowest order derivative terms, in the limit, the decay patterns cannot be explained. Large breaking effects are needed to explain the data.

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