\begin{document}$ V\rightarrow K^{+}K^{-} (V=\phi, \rho, \omega) $\end{document} resonance, which generates a strong phase associated with vector meson resonances, leading to significant CP asymmetry in the interference region. The \begin{document}$ \phi \rightarrow K^{+}K^{-} $\end{document}, \begin{document}$ \rho \rightarrow K^{+}K^{-} $\end{document}, and \begin{document}$ \omega \rightarrow K^{+}K^{-} $\end{document} resonances arise from the mixing of the vector mesons ϕ, ρ, and ω. We calculate the CP asymmetry from the decay mode of \begin{document}$ B \rightarrow KK\pi(K) $\end{document}. Meanwhile, the localized CP asymmetries are presented and a detailed analysis is performed. The CP asymmetry from the decay mode of \begin{document}$ {B}^{-}\rightarrow \phi\pi^{-}\rightarrow K^{+}K^{-}\pi^{-} $\end{document} is also presented in our framework, which is highly consisted with that of the LHC experiment. The introduced CP asymmetry can provide a favorable theoretical support for experimental exploration in the future."> <i>CP</i> asymmetry from the resonance effect of the <i>B</i> meson decay process with <i>π</i> and <i>K</i> final states -
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