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Measurement of the CKM angle $γ$ using $B^0 \rightarrow D K^{*0}$ with $D \rightarrow K^0_S π^+ π^-$ decays (1605.01082v4)

Published 3 May 2016 in hep-ex

Abstract: A model-dependent amplitude analysis of the decay $B0\rightarrow D(K0_S\pi+\pi-) K{*0}$ is performed using proton-proton collision data corresponding to an integrated luminosity of 3.0fb${-1}$, recorded at $\sqrt{s}=7$ and $8 TeV$ by the LHCb experiment. The CP violation observables $x_{\pm}$ and $y_{\pm}$, sensitive to the CKM angle $\gamma$, are measured to be \begin{eqnarray*} x_- &=& -0.15 \pm 0.14 \pm 0.03 \pm 0.01, y_- &=& 0.25 \pm 0.15 \pm 0.06 \pm 0.01, x_+ &=& 0.05 \pm 0.24 \pm 0.04 \pm 0.01, y_+ &=& -0.65{+0.24}_{-0.23} \pm 0.08 \pm 0.01, \end{eqnarray*} where the first uncertainties are statistical, the second systematic and the third arise from the uncertainty on the $D\rightarrow K0_S \pi+\pi-$ amplitude model. These are the most precise measurements of these observables. They correspond to $\gamma=(80{+21}_{-22}){\circ}$ and $r_{B0}=0.39\pm0.13$, where $r_{B0}$ is the magnitude of the ratio of the suppressed and favoured $B0\rightarrow D K+ \pi-$ decay amplitudes, in a $K\pi$ mass region of $\pm50 MeV$ around the $K*(892)0$ mass and for an absolute value of the cosine of the $K{*0}$ decay angle larger than $0.4$.

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