${\cal B}(B_s^0 \to K^*(892)^0 \bar{K}^*(892)^0)$

ExperimentMeasurement [10-5]$\Delta\chi^2$ReferenceComments
Average$1.10 \pm0.20$8.14$p=0.52$ (ndf=9)
PDG$1.11 \pm0.27$pdgLive
LHCb$1.12 \pm0.22 \pm0.15$ using ${\cal B}(B^0 \to \phi(1020) K^*(892)^0)$0.01 JHEP 07,166 (2015)Multiple systematic uncertainties are added in quadrature.
LHCb${\cal B}(B^0 \to K^*(892)^0 \bar{K}^*(892)^0) / {\cal B}(B_s^0 \to K^*(892)^0 \bar{K}^*(892)^0)$0.00 JHEP 07,032 (2019)Multiple systematic uncertainties are added in quadrature.
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^0 \to K^*(892)^0 \bar{K}^*(892)^0)$90.2$8.3 \pm1.6 \times 10^{-7}$
fit${\cal B}(B^0 \to \phi(1020) K^*(892)^0)$23.4$1.011 \pm0.048 \times 10^{-5}$
fit${\cal B}(B_s^0 \to \phi(1020) \mu^+ \mu^-)$-22.1$8.65\,^{+0.66}_{-0.64} \times 10^{-7}$
fit${\cal B}(B_s^0 \to \phi(1020) \phi(1020))$9.1$1.87\,^{+0.15}_{-0.14} \times 10^{-5}$
fit${\cal B}(B_s^0 \to f_2^{\prime}(1525) \mu^+ \mu^-)$-4.8$1.66\,^{+0.26}_{-0.24} \times 10^{-7}$
fit${\cal B}(B^0 \to \rho^0(770) \rho^0(770))$3.9$9.6 \pm1.5 \times 10^{-7}$
fit${\cal B}(B_s^0 \to \phi(1020) \bar{K}^*(892)^0)$3.9$1.14 \pm0.29 \times 10^{-6}$
external${\cal B}(B_s^0 \to J/\psi \phi(1020))$-23.0$1.074\,^{+0.074}_{-0.073} \times 10^{-3}$0.01
Parameters of interest whose average is determined from individual measurements are called fit parameters. Parameters that are needed by the fit (in particular daughter branching fraction) and whose average is not determined here, but taken from somewhere else (usually PDG) are called external parameters.