Abstract

Direct CP violation in the hadronic charm decays provides a good testing ground for the Kobayashi-Maskawa mechanism in the Standard Model. Any significant deviations from the expectation would be indirect evidence of physics beyond the Standard Model. In view of improved measurements from LHCb and BESIII experiments, we re-analyze the Cabibbo-favored $D \to P\!P$ and $V\!P$ decays in the topological diagram approach. By assuming certain SU(3)-breaking effects in the tree-type amplitudes, we make predictions for both branching fractions and CP asymmetries of the singly Cabibbo-suppressed decay modes. While the color-allowed and -suppressed amplitudes are preferred to scale by the factor dictated by factorization in the $P\!P$ modes, no such scaling is required in the $V\!P$ modes. The $W$-exchange amplitudes are found to change by 10\% to 50\% and depend on whether $d\overline{d}$ or $s\overline{s}$ pair directly emerges from $W$-exchange. The predictions of branching fractions are generally improved after these SU(3) symmetry breaking effects are taken into account. We show in detail how the tree-type, QCD-penguin, and weak penguin-annihilation diagrams contribute and modify CP asymmetry predictions. Future measurements of sufficiently many direct CP asymmetries will be very useful in removing a discrete ambiguity in the strong phases as well as discriminating among different theory approaches. In particular, we predict $a_{CP}(K^+K^-)-a_{CP}(\pi^+\pi^-) = (-1.14 \pm 0.26) \times 10^{-3}$ or $(-1.25 \pm 0.25) \times 10^{-3}$, consistent with the latest data, and $a_{CP}(K^+K^{*-})-a_{CP}(\pi^+\rho^-) = (-1.52 \pm 0.43) \times 10^{-3}$, an attractive and measurable observable in the near future. Moreover, we observe that such CP asymmetry differences are dominated by long-distance penguin-exchange through final-state rescattering.

Highlights

  • Since ΔadCiPr in the Standard Model (SM) is naively expected to be at most of order 1 × 10−3, many new physics models [2,3,4,5,6,7,8,9,10,11,12,13,14,15] had been proposed to explain the measurement of large ΔACP, it was argued in [16,17,18,19,20,21,22,23] that large CP asymmetries in singly Cabibbo-suppressed (SCS) D decays were allowed in the SM due to some nonperturbative effects or unexpected strong dynamics and the measured ΔadCiPr could be accommodated or marginally achieved

  • In 2012, we have studied direct CP violation in charmed meson decays based on the topological diagram approach for tree amplitudes and QCD factorization for penguin amplitudes [36,37]

  • We have shown that ΔadCiPr arises mainly from long-distance weak penguin annihilation

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Summary

INTRODUCTION

Based on 0.62 fb−1 of 2011 data, in 2012 the LHCb collaboration has reported a result of a nonzero value for the difference between the time-integrated CP asymmetries of the decays D0 → KþK− and D0 → πþπ− [1]: ΔACP ≡ aCPðKþK−Þ − aCPðπþπ−Þ. In 2012, we have studied direct CP violation in charmed meson decays based on the topological diagram approach for tree amplitudes and QCD factorization for penguin amplitudes [36,37]. In our previous study of the long-distance contribution to PE, we did not consider the uncertainties connected with final-state rescattering [37] This will be improved in this work. Analyses of topological graphs can provide valuable information on final-state interactions

Topological amplitudes
Penguin amplitudes in QCD factorization
Tree-level CP violation
Penguin-induced CP violation
Ãcs V udðAV
Direct CP violation
DISCUSSIONS AND CONCLUSIONS

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