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LHCb observes the $B^+_c \to D^0 K^+$ decay with $R_{D^0 K} = f_c/f_u \times{\cal B}(B^+_c \to D^0 K^+)=(9.3^{+2.8}_{-2.5} \pm 0.6)\times 10^{-7}$. Thecorresponding branching ratio (BR) of the decay can be estimated as ${\calB}(B^+_c \to D^0 K^+) \approx (10.01 \pm 3.40)\times 10^{-5}$; however, thetheoretical estimates vary from $\sim 10^{-7}$ to $\sim 5\times 10^{-5}$. Wephenomenologically investigate the $B^+_c \to (D^0 K^+, D^0 \pi^+)$ decaysthrough the analysis of $B\to KK$, $B^+_u\to D^+ K^0$, and $B_d \to D^-_s K^+$.With the form factor of $f^{B_c D}_0\approx 0.2$, it is found that thetree-annihilation contribution dominates the $B^+_c \to D^0 K^+$ decay, andwhen ${\cal B}(B^+_u \to D^+ K^0) \approx (1-3.1) \times 10^{-7}$ is required,we obtain ${\cal B}(B^+_c \to D^0 K^+)\approx (4.4- 9) \times 10^{-5}$, and themagnitude of CP asymmetry is lower than approximately $10\%$. Although the$B^+_c \to D^0 \pi^+$ decay is dominated by the tree-transition effect, thetree-annihilation also makes an important contribution, where its effect couldbe around $70\%$ of the tree-transition. It is found that when ${\cal B}(B^+_c\to D^0 K^+)\approx (4.4- 9) \times 10^{-5}$ is taken, the BR and CP asymmetryfor $B^+_c \to D^0 \pi^+$ with the common values of parameters can be ${\calB}(B^+_c \to D^0 \pi^+)\approx (4.9-8)\times 10^{-6}$ and of the order of one,respectively. Moreover, we conclude ${\cal B}(B^+_c \to D^+ K^0)\approx {\calB}(B^+_c \to D^0 K^+)$, and the BRs for $B^+_c \to K^+ \bar K^0$ and $B^+_c \toJ/\Psi \pi^+$ are $(6.99 \pm 1.34) \times 10^{-7}$ and $(7.7 \pm 1.1)\times10^{-4}$, respectively.

Study of $B^\pm_c \to (D^0 K^\pm, D^0 \pi^\pm)$ decays