Studies of the resonance structure in $D^{0} \to K^\mp Ï^\pm Ï^\pm Ï^\mp$ decays
arXiv:1712.08609 · doi:10.1140/epjc/s10052-018-5758-4
Abstract
Amplitude models are constructed to describe the resonance structure of ${D^{0}\to K^{-}Ï^{+}Ï^{+}Ï^{-}}$ and ${D^{0} \to K^{+}Ï^{-}Ï^{-}Ï^{+}}$ decays using $pp$ collision data collected at centre-of-mass energies of 7 and 8 TeV with the LHCb experiment, corresponding to an integrated luminosity of $3.0\mathrm{fb}^{-1}$. The largest contributions to both decay amplitudes are found to come from axial resonances, with decay modes $D^{0} \to a_1(1260)^{+} K^{-}$ and $D^{0} \to K_1(1270/1400)^{+} Ï^{-}$ being prominent in ${D^{0}\to K^{-}Ï^{+}Ï^{+}Ï^{-}}$ and $D^{0}\to K^{+}Ï^{-}Ï^{-}Ï^{+}$, respectively. Precise measurements of the lineshape parameters and couplings of the $a_1(1260)^{+}$, $K_1(1270)^{-}$ and $K(1460)^{-}$ resonances are made, and a quasi model-independent study of the $K(1460)^{-}$ resonance is performed. The coherence factor of the decays is calculated from the amplitude models to be $R_{K3Ï} = 0.459\pm 0.010\,(\mathrm{stat}) \pm 0.012\,(\mathrm{syst}) \pm 0.020\,(\mathrm{model})$, which is consistent with direct measurements. These models will be useful in future measurements of the unitary-triangle angle $γ$ and studies of charm mixing and $C\!P$ violation.
All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2017-040.html