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

ExperimentMeasurement [10-5]$\Delta\chi^2$ReferenceComments
Average$4.97 \pm0.18$1.50$p=0.96$ (ndf=6)The PDG average is a result of a fit including input from other measurements.
Treatment of charmonium intermediate components differs between the results.
PDG$4.97 \pm0.18$pdgLive
BaBar$5.015 \pm0.147 \pm0.176$0.04 Phys.Rev.D 80,112001 (2009)Result extracted from Dalitz-plot analysis of $B^0 \to K_S^0 \pi^+ \pi^-$ decays.
Multiple systematic uncertainties are added in quadrature.
Belle$4.75 \pm0.24 \pm0.37$0.25 Phys.Rev.D 75,012006 (2007)Result extracted from Dalitz-plot analysis of $B^0 \to K_S^0 \pi^+ \pi^-$ decays.
CLEO$5.00\,^{+1.00}_{-0.90} \pm0.70$0.00 Phys.Rev.Lett. 89,251801 (2002)
LHCb${\cal B}(\Lambda_b^0 \to p \bar{K}^0 \pi^-) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.00 JHEP 04,087 (2014)Multiple systematic uncertainties are added in quadrature.
LHCb${\cal B}(\Lambda_b^0 \to p K^0 K^-) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$JHEP 04,087 (2014)
LHCb$\frac{f_{\Xi^{0}_{b}}}{f_d}{\cal{B}}(\Xi^{0}_{b} \to p \bar{K}^0 \pi^{-}) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$JHEP 04,087 (2014)
LHCb$\frac{f_{\Xi^{0}_{b}}}{f_{d}}{\cal{B}}(\Xi^{0}_{b} \to p \bar{K}^0 K^{-}) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$JHEP 04,087 (2014)
LHCb${\cal B}(B^0 \to K^*(892)^0 \bar{K}^0 \mathrm{+c.c.}) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$JHEP 01,012 (2016)
LHCb${\cal B}(B^0 \to K^0 K^+ \pi^- \mathrm{+c.c.}) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.44 JHEP 11,027 (2017)Regions corresponding to $D$, $\Lambda_c^+$ and charmonium resonances are vetoed in this analysis.
LHCb${\cal B}(B^0 \to K^0 K^+ K^-) / {\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.
LHCb${\cal B}(B_s^0 \to K^0 \pi^+ \pi^-) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.00 JHEP 11,027 (2017)Regions corresponding to $D$, $\Lambda_c^+$ and charmonium resonances are vetoed in this analysis.
LHCb${\cal B}(B_s^0 \to K^0 K^+ \pi^- \mathrm{+c.c.}) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.00 JHEP 11,027 (2017)Regions corresponding to $D$, $\Lambda_c^+$ and charmonium resonances are vetoed in this analysis.
LHCb${\cal B}(B_s^0 \to K^0 K^+ K^-) / {\cal B}(B^0 \to K^0 \pi^+ \pi^-)$0.00 JHEP 11,027 (2017)Regions corresponding to $D$, $\Lambda_c^+$ and charmonium resonances are vetoed in this analysis.
Input values that appear in red are not included in the PDG average.

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

SourceParameterCorrelation [%]Value$\Delta\chi^2$
fit${\cal B}(B_s^0 \to K^0 K^+ \pi^- \mathrm{+c.c.})$34.3$8.45 \pm0.87 \times 10^{-5}$
fit${\cal B}(B^0 \to K^0 K^+ K^-)$25.5$2.68 \pm0.10 \times 10^{-5}$
fit${\cal B}(B^0 \to K^0 K^+ \pi^- \mathrm{+c.c.})$16.8$6.69 \pm0.51 \times 10^{-6}$
fit${\cal B}(B_s^0 \to K^0 \pi^+ \pi^-)$15.7$9.5 \pm2.1 \times 10^{-6}$
fit${\cal B}(\Lambda_b^0 \to p \bar{K}^0 \pi^-)$10.7$1.24 \pm0.42 \times 10^{-5}$
fit${\cal B}(B_s^0 \to K^0 K^+ K^-)$7.0$1.29 \pm0.66 \times 10^{-6}$
nuisance$\frac{f_s}{f_d}$-0.1$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.