Abstract
We analyze patterns from $CP$--violating new physics (NP) in hadronic and semileptonic rare charm $|\mathrm{\ensuremath{\Delta}}c|=|\mathrm{\ensuremath{\Delta}}u|=1$ transitions. Observation of direct $CP$ violation in hadronic decays, as in $\mathrm{\ensuremath{\Delta}}{A}_{CP}$, provides opportunities for $c\ensuremath{\rightarrow}u{\ensuremath{\ell}}^{+}{\ensuremath{\ell}}^{\ensuremath{-}}$, $\ensuremath{\ell}=e,\ensuremath{\mu}$ transitions, and vice versa. For the concrete case of flavorful, anomalyfree ${Z}^{\ensuremath{'}}$--models a NP--interpretation of $\mathrm{\ensuremath{\Delta}}{A}_{CP}$ suggests measurable $CP$ asymmetries in semileptonic decays such as $D\ensuremath{\rightarrow}\ensuremath{\pi}{\ensuremath{\ell}}^{+}{\ensuremath{\ell}}^{\ensuremath{-}}$ or $D\ensuremath{\rightarrow}\ensuremath{\pi}\ensuremath{\pi}{\ensuremath{\ell}}^{+}{\ensuremath{\ell}}^{\ensuremath{-}}$. Conversely, an observation of $CP$ violation in $c\ensuremath{\rightarrow}u{e}^{+}{e}^{\ensuremath{-}}$ or $c\ensuremath{\rightarrow}u{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ decays supports a NP--interpretation of $\mathrm{\ensuremath{\Delta}}{A}_{CP}$. Flavorful $U(1{)}^{\ensuremath{'}}$--extensions provide explicit U--spin and isospin breaking which can be probed in patterns of hadronic decays of charm mesons. We work out signatures for $CP$ asymmetries in ${D}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, ${D}^{0}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}}$ and ${D}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}{\ensuremath{\pi}}^{0}$, ${D}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{0}$ decays, which can be probed in the future at LHCb and Belle II and provide further informative cross checks.
Highlights
Suppressions of standard model (SM) amplitudes due to accidental symmetries provide useful directions for searches for new physics (NP)
We work out NP–effects in charm from anomalyfree Uð1Þ0–extensions of the SM with fermion charges Fψi that depend on the generation, i 1⁄4 1, 2, 3
Taking into account the running from MZ0 to mc, details of which are given in Appendix B, we find that ΔACP can be written as ΔANCPP 1⁄4 ANCPP ðKþK−Þ − ANCPP ðπþπ−Þ; ð35Þ
Summary
Suppressions of standard model (SM) amplitudes due to accidental symmetries provide useful directions for searches for new physics (NP). Among the salient features of jΔcj 1⁄4 jΔuj 1⁄4 1 transitions within the SM are a strong While this leaves room for NP, due to the sizable uncertainties of hadronic D–decays, Eqs. In this work we pursue a global analysis of CP asymmetries in rare hadronic and semileptonic charm decays. Links via dipole operators between hadronic and semileptonic CP asymmetries in D → πlþl− decays have been pointed out by Ref.
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