| Experiment | Measurement [10-5] | $\Delta\chi^2$ | Reference | Comments |
| Average | $1.011 \pm0.048$ | 8.14 | $p=0.52$ (ndf=9) | |
| PDG | $1.004 \pm0.052$ | | pdgLive | |
| BaBar | $0.97 \pm0.05 \pm0.05$ | 0.33 |
Phys.Rev.D 78,092008 (2008) | |
| Belle | $1.04 \pm0.05 \pm0.06$ | 0.14 |
Phys.Rev.D 88,072004 (2013) | |
| Belle II | $1.10 \pm0.21 \pm0.11$ | 0.14 |
arXiv:2008.03873 | |
| CLEO | $1.15\,^{+0.45}_{-0.37}\,^{+0.18}_{-0.17}$ | 0.10 |
Phys.Rev.Lett. 86,3718 (2001) | |
| LHCb | ${\cal B}(B_s^0 \to \phi(1020) \bar{K}^*(892)^0) / {\cal B}(B^0 \to \phi(1020) K^*(892)^0)$ | 0.00 |
JHEP 11,092 (2013) | Multiple systematic uncertainties are added in quadrature.
|
| LHCb | ${\cal B}(B_s^0 \to K^*(892)^0 \bar{K}^*(892)^0) / {\cal B}(B^0 \to \phi(1020) K^*(892)^0)$ | 0.01 |
JHEP 07,166 (2015) | Multiple systematic uncertainties are added in quadrature.
|
| LHCb | ${\cal B}(B_s^0 \to \phi(1020) \phi(1020)) / {\cal B}(B^0 \to \phi(1020) K^*(892)^0)$ | 0.01 |
JHEP 10,053 (2015) | Multiple systematic uncertainties are added in quadrature.
|
| LHCb | ${\cal B}(B^0 \to \rho^0(770) \rho^0(770)) / {\cal B}(B^0 \to \phi(1020) K^*(892)^0)$ | 0.00 |
Phys.Lett.B 747,468 (2015) | |
Input values that appear in red are not included in the PDG average.
Parameters of interest whose average is determined from individual measurements are called