Direct CP Violation in Cabibbo-Favored Charmed Meson Decays and ${\epsilon }^{\prime }/\epsilon$ in $SU(2{)}_L\times SU(2{)}_R\times U(1{)}_{B-L}$ Model

Abstract

Since the standard model contribution is virtually absent, any observation of direct CP violation in the Cabibbo-favored charmed meson decays would be evidence of new physics. In this paper, we conduct a quantitative study on direct CP violation in $D^0\to K^{-}{\pi }^{+}$, $D_s^{+}\to \eta {\pi }^{+}$ and $D_s^{+}\to {\eta }^{\prime }{\pi }^{+}$ decays in the $SU(2{)}_L\times SU(2{)}_R\times U(1{)}_{B-L}$ gauge extension of the standard model. In the model, direct CP violation arises mainly from the interference between the decay amplitude coming from the SM left-left current operators and that from the right-right current operators induced by $W_R^{+}$ gauge boson exchange. Interestingly, the strong phase between the two amplitudes is evaluable, since it stems from difference in QCD corrections to the left-left and right-right current operators, which is a short-distance QCD effect given by $\sim ({\alpha }_s(M_{W_L}^2)/4\pi )\log (M_{W_R}^2/M_{W_L}^2)$. We assess the maximal direct CP violation in the above decays in the $SU(2{)}_L\times SU(2{)}_R\times U(1{)}_{B-L}$ model. Additionally, we present a correlation between direct CP violation in these modes and one in $K\to \pi \pi$ decay parametrized by ${\epsilon }^{\prime }$, since $W_R^{+}$ gauge boson has a sizable impact on the latter.

arXiv comment18 pages, 2 tables and 3 figures; v3: Discussion on the effect of $SU(3)$ flavor symmetry breaking is added

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• Left-handed color-sextet diquark in the Kaon system
• BSM Hadronic Matrix Elements for ${\epsilon }^{\prime }/\epsilon$ and $K\to \pi \pi$ Decays in the Dual QCD Approach
• The direct CP violation in a general two Higgs doublet model
• Effect of the Pauli exclusion principle in the electric dipole moment of ${}^9$Be with $|\Delta S|=1$ interactions
• ${\epsilon }_K$ and ${\epsilon }^{\prime }/\epsilon$ in a diquark model
• Direct CP violation in $D^{+}\to K^0({\bar{K}}^0){\pi }^{+}$ decays as a probe for new physics