?
Search for CP violation in 𝐷+(𝑠)→ℎ+𝜋0 and 𝐷+(𝑠)→ℎ+𝜂 decays
Searches for CP violation in the two-body decays 𝐷+(𝑠)→ℎ+𝜋0D(s)+→h+π0 and 𝐷+(𝑠)→ℎ+𝜂D(s)+→h+η (where h+ denotes a π+ or K+ meson) are performed using pp collision data collected by the LHCb experiment corresponding to either 9 fb−1 or 6 fb−1 of integrated luminosity. The π0 and η mesons are reconstructed using the e+e−γ final state, which can proceed as three-body decays π0 → e+e−γ and η → e+e−γ, or via the two-body decays π0 → γγ and η → γγ followed by a photon conversion. The measurements are made relative to the control modes 𝐷+(𝑠)→𝐾0Sℎ+D(s)+→KS0h+ to cancel the production and detection asymmetries. The CP asymmetries are measured to be
𝐶𝑃(𝐷+→𝜋+𝜋0)=(−1.3±0.9±0.6)%,𝐶𝑃(𝐷+→𝐾+𝜋0)=(−3.2±4.7±2.1)%,𝐶𝑃(𝐷+→𝜋+𝜂)=(−0.2±0.8±0.4)%,𝐶𝑃(𝐷+→𝐾+𝜂)=(−6±10±4)%,𝐶𝑃(𝐷+𝑠→𝐾+𝜋0)=(−0.8±3.9±1.2)%,𝐶𝑃(𝐷+𝑠→𝜋+𝜂)=(0.8±0.7±0.5)%,𝐶𝑃(𝐷+𝑠→𝐾+𝜂)=(0.9±3.7±1.1)%,ACP(D+→π+π0)=(−1.3±0.9±0.6)%,ACP(D+→K+π0)=(−3.2±4.7±2.1)%,ACP(D+→π+η)=(−0.2±0.8±0.4)%,ACP(D+→K+η)=(−6±10±4)%,ACP(Ds+→K+π0)=(−0.8±3.9±1.2)%,ACP(Ds+→π+η)=(0.8±0.7±0.5)%,ACP(Ds+→K+η)=(0.9±3.7±1.1)%,
where the first uncertainties are statistical and the second systematic. These results are consistent with no CP violation and mostly constitute the most precise measurements of 𝐶𝑃ACP in these decay modes to date.