${\cal B}(B^0 \to K^0 K^+ K^-)$

ExperimentMeasurement [10-5]$\Delta\chi^2$ReferenceComments
Average$2.68 \pm0.10$1.50$p=0.96$ (ndf=6)
PDG$2.68 \pm0.11$pdgLive
LHCb$2.729 \pm0.089 \pm0.190$ using ${\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.07 JHEP 11,027 (2017)Regions corresponding to $D$, $\Lambda_c^+$ and charmonium resonances are vetoed in this analysis.
BaBar$2.65 \pm0.09 \pm0.08$0.06 Phys.Rev.D 85,112010 (2012)Result extracted from Dalitz-plot analysis of $B^0 \to K_S^0 K^+ K^-$ decays.
All charmonium resonances are vetoed, except for $\chi_{c0}$. The analysis also reports ${\cal{B}}( B^{0} \to K^0 K^+ K^- ) = (25.4 \pm 0.9 \pm 0.8) \times 10^{-6}$ excluding $\chi_{c0}$.
Belle$2.83 \pm0.33 \pm0.40$0.08 Phys.Rev.D 69,012001 (2004)

Further parameters used in the fit and their correlation with the average

SourceParameterCorrelation [%]Value$\Delta\chi^2$
fit${\cal B}(B^0 \to K^0 \pi^+ \pi^-)$25.5$4.97 \pm0.18 \times 10^{-5}$
fit${\cal B}(B_s^0 \to K^0 K^+ \pi^- \mathrm{+c.c.})$8.8$8.45 \pm0.87 \times 10^{-5}$
fit${\cal B}(B^0 \to K^0 K^+ \pi^- \mathrm{+c.c.})$4.3$6.69 \pm0.51 \times 10^{-6}$
fit${\cal B}(B_s^0 \to K^0 \pi^+ \pi^-)$4.0$9.5 \pm2.1 \times 10^{-6}$
fit${\cal B}(\Lambda_b^0 \to p \bar{K}^0 \pi^-)$2.7$1.24 \pm0.42 \times 10^{-5}$
fit${\cal B}(B_s^0 \to K^0 K^+ K^-)$1.8$1.29 \pm0.66 \times 10^{-6}$
nuisance$\frac{f_s}{f_d}$-0.0$5 \pm1000 \times 10^{-3}$0.00
Parameters of interest whose average is determined from individual measurements are called fit parameters. Auxiliary fit parameters without direct physical meaning (in particular those to model correlated systematic uncertainties) are called nuisance parameters and constrained by a normally distributed likelihood function.