# ${{\boldsymbol D}^{0}}$ $\rightarrow$ ${{\boldsymbol K}^{-}}{{\boldsymbol \pi}^{-}}$2 ${{\boldsymbol \pi}^{+}}$ , $\boldsymbol R_{ {{\boldsymbol K}}3 {{\boldsymbol \pi}} }$ (y cos $\delta {}^{ {{\boldsymbol K}}3 {{\boldsymbol \pi}} }$ $−$ x sin$\delta {}^{ {{\boldsymbol K}}3 {{\boldsymbol \pi}} }$) INSPIRE search

VALUE ($10^{-3}$ TeV${}^{-1}$) EVTS DOCUMENT ID TECN  COMMENT
$-3.0$ $\pm0.7$ 42.5k 1
 2016 F
LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8 TeV
1  From a time-dependent analysis of ${{\mathit D}}$ mixing in ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ . This result uses external constraints on R$_{M}$= 1/2 (x${}^{2}$ + y${}^{2}$). Without such constraints, AAIJ 2016F measure $0.0003$ $\pm0.0018$, with a large correlation coefficient to R$_{M}$.
References:
 AAIJ 2016F
PRL 116 241801 First Observation of ${{\mathit D}^{0}}−{{\overline{\mathit D}}^{0}}$ Oscillations in ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ Decays and Measurement of the Associated Coherence Parameters