asymmetry for all three processes: (K\^+ \^-) = -0.04 0.16,   [A]{}(K\^+ \^0) = -0.29 0.23,   [A]{}(K\_S \^+) = 0.18 0.24.

Conclusions
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The coupling of $\pp$ and $\ppp$ to charmed particle pairs can lead to S–D-wave mixing, the distortion of the relative branching ratios of the $\ppp$ to $\gamma + \chi_c$ final states, and the suppression of some decay modes of $\pp$ and their appearance instead in products of the $\ppp$. If $\ppp$ to $\gamma + \chi_{c2}$ is observed at a branching ratio level exceeding a couple of parts in $10^4$, this will be evidence for S–D-wave mixing, while the branching ratio for $\ppp$ to $\gamma + \chi_{c0}$ is expected to be a percent, give or take a factor of 2. A similar branching ratio is expected for [*hadronic*]{} charmless decays of $\ppp$. This picture provides a rationale for large observed $\bar b \to \bar s$ penguin amplitudes in $B$ meson decays, and would be further supported by the observation of large direct CP-violating asymmetries in the decays $B^+ \to \pi^0 K^+$ and $B^0 \to K^+ \pi^-$.

Acknowledgments {#acknowledgments .unnumbered}
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I thank San Fu Tuan for asking questions which led to this investigation and for useful comments, and Thorsten 