of $\rho^f_A$ and $\phi^f_A$ for $A^{f}_k$. In fact, the symmetry breaking effects have been considered in pervious QCDF study on two-body hadronic $B$ decays [@Cheng1; @Cheng2; @Cheng3; @Beneke2; @chang1], but with parameters of $\rho^f_A$ $=$ $\rho^i_A$ and $\phi^f_A$ $=$ $\phi^i_A$. So, it is essential to systematically reevaluate factorizable and nonfactorizable annihilation contributions and preform a global fit on the annihilation parameters with the current available experimental data. In this paper, we will pay much attention to $B_{u,d}$ ${\to}$ $KK$, ${\pi}K$, ${\pi}{\pi}$ decays and the aforementioned ${\pi}K$, ${\pi}{\pi}$ puzzles with a distinction between ($\rho^f_A$, $\phi^f_A$) and ($\rho^i_A$, $\phi^i_A$), i.e., $X_A^i$ $\neq$ $X_A^f$.

As aforesaid [@Cheng1; @pipipuz], the nonfactorizable spectator scattering amplitudes contribute to a large complex $C^{\prime}$, which is important to resolve the ${\pi}K$, ${\pi}{\pi}$ puzzles. From the building block Eq.(\[hardblock\]), it can be easily seen that $B$ meson wave functions $\Phi_{B}(\xi)$ appear in the spectator scattering amplitudes. Therefore, the symmetry breaking effects should also be considered for the quantity $X_H$ that is introduced to parameterize the endpoint singularity in the twist-3 level spectator scattering corrections. Similar to $X_A^i$, the quantity $X_H$ is related to the topologies that gluon emit from the initial $B$ meson. So, for simplicity, the approximation $X_H$ 