We extend the perturbative QCD formalism including the Glauber gluons, which has been shown to accommodate the measured and $B^0\to\rho^0 \rho^0B \to K \piK \bar K$ decays. It is observed that the convolution of the universal Glauber phase factors with the transverse-momentum-dependent kaon wave function reveals weaker (stronger) Glauber effects than in the pion ( meson) case as expected. Our predictions for the branching ratios and the direct CP asymmetries of the and modes at next-to-leading-order accuracy agree well with data. In particular, the predicted difference of the and direct CP asymmetries, $\Delta A_{K\pi}\equiv A_{\rm CP}^{\rm dir}(K^\pm \pi^0)[0.021 \pm 0.016] - A_{\rm CP}^{\rm dir}(K^\pm \pi^\mp)[-0.081 \pm 0.017] = 0.102 \pm 0.023$, is consistent with the measured within uncertainties, and the known puzzle is resolved. The above $B \to \pi \piK\piK \bar K$ studies confirm that the Glauber gluons associated with pseudo-Nambu-Goldstone bosons enhance the color-suppressed tree amplitude significantly, but have a small impact on other topological amplitudes.

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