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Amplitude models are applied to studies of resonance structure in $D^0to K^0_S K^- pi^+$ and $D^0to K^0_S K^+ pi^-$ decays using $pp$ collision data corresponding to an integrated luminosity of $3.0,mathrm{fb}^{-1}$ collected by the LHCb experiment. Relative magnitude and phase information is determined, and coherence factors and related observables are computed for both the whole phase space and a restricted region of $100,mathrm{MeV/}c^2$ around the $K^{*}(892)^{pm}$ resonance. Two formulations for the $Kpi$ $S$-wave are used, both of which give a good description of the data. The ratio of branching fractions $mathcal{B}(D^0to K^0_S K^+ pi^-)/mathcal{B}(D^0to K^0_S K^- pi^+)$ is measured to be $0.655pm0.004,(textrm{stat})pm0.006,(textrm{syst})$ over the full phase space and $0.370pm0.003, (textrm{stat})pm0.012,(textrm{syst})$ in the restricted region. A search for $CP$ violation is performed using the amplitude models and no significant effect is found. Predictions from $SU(3)$ flavor symmetry for $K^{*}(892)K$ amplitudes of different charges are compared with the amplitude model results.
Amplitude models are constructed to describe the resonance structure of ${D^{0}to K^{-}pi^{+}pi^{+}pi^{-}}$ and ${D^{0} to K^{+}pi^{-}pi^{-}pi^{+}}$ decays using $pp$ collision data collected at centre-of-mass energies of 7 and 8 TeV with the LHCb ex
We report on measurements of the time-dependent CP violating observables in $B^0_srightarrow D^{mp}_s K^{pm}$ decays using a dataset corresponding to 1.0 fb$^{-1}$ of pp collisions recorded with the LHCb detector. We find the CP violating observables
A first study of CP violation in the decay modes $B^pmto [K^0_{rm S} K^pm pi^mp]_D h^pm$ and $B^pmto [K^0_{rm S} K^mp pi^pm]_D h^pm$, where $h$ labels a $K$ or $pi$ meson and $D$ labels a $D^0$ or $overline{D}^0$ meson, is performed. The analysis use
An analysis of the decays of $B^mp rightarrow D K^mp$ and $B^mp rightarrow D pi^mp $ is presented in which the $D$ meson is reconstructed in the three-body final states $K^mp pi^pm pi^0$, $pi^+ pi^- pi^0$ and $K^+ K^- pi^0$. Using data from LHCb corr