Abstract
A binned Dalitz plot analysis of the decays $B^0 \to D K^{\ast 0}$, with $D \to K_{S}^{0} \pi^{+} \pi^{-}$ and $K_{S}^{0} K^{+} K^{-}$, is performed to measure the observables $x_\pm$ and $y_\pm$, which are related to the CKM angle $\gamma$ and the hadronic parameters of the decays. The $D$ decay strong phase variation over the Dalitz plot is taken from measurements performed at the CLEO-c experiment, making the analysis independent of the $D$ decay model. With a sample of proton-proton collision data, corresponding to an integrated luminosity of $3.0\,\rm{fb}^{-1}$, collected by the LHCb experiment, the values of the $CP$ violation parameters are found to be $x_+ = 0.05 \pm 0.35 \pm 0.02$, $x_-=-0.31\pm 0.20 \pm 0.04$, $y_+=-0.81\pm 0.28\pm 0.06$ and $y_-=0.31\pm 0.21 \pm 0.05$, where the first uncertainties are statistical and the second systematic. These observables correspond to values $\gamma$ = $(71 \pm 20)^\circ$, $r_{B^0} = 0.56\pm 0.17$ and $\delta_{B^0} = (204\,^{+21}_{-20})^\circ$. The parameters $r_{B^0}$ and $\delta_{B^0}$ are the magnitude ratio and strong phase difference between the suppressed and favoured $B^0$ decay amplitudes, and have been measured in a region of $\pm 50$ MeV/$c^2$ around the $K^{\ast}(892)^{0}$ mass and with the magnitude of the cosine of the $K^{\ast}(892)^{0}$ helicity angle larger than 0.4.
Highlights
Overview of the analysisAc(p) are the moduli of the b → u and b → c amplitudes, and δc,u(p) represent the strong phases of the relevant decay amplitudes
K ∗0 d the flavour of the decaying B meson as B0 or B0
A binned Dalitz plot analysis of the decays B0 → DK∗0, with D → KS0π+π− and D → KS0K+K−, is performed to measure the observables x± and y±, which are related to the CKM angle γ and the hadronic parameters of the decays
Summary
Ac(p) are the moduli of the b → u and b → c amplitudes, and δc,u(p) represent the strong phases of the relevant decay amplitudes. The magnitude ratio between the suppressed and favoured amplitudes rB0, the coherence factor κ [28], and the effective strong phase difference δB0 depend on the region of the B0 Dalitz plot to be analysed. An analogous expression can be written for si which is the sine of the strong-phase difference weighted by the decay amplitude and averaged in the bin. For the present analysis the variant with the 2 × 2 binning is chosen, given the very low signal yields expected in this decay. The effect of different nuclear interactions within the detector material for K0 and K0 mesons is expected to be of a similar magnitude and is ignored [33]
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