${\cal{B}}(B^+ \to K^+ K^- \pi^+)~\pi\pi \leftrightarrow KK~\rm{rescattering}$

ExperimentMeasurement [10-7]$\Delta\chi^2$ReferenceComments
Average$8.25\,^{+0.78}_{-0.75}$
PDG$8.53 \pm0.94$pdgLive
LHCb$8.25 \pm0.40 \pm0.65$ using ${\cal{B}}(B^+ \to K^+ K^- \pi^+)$0.00 Phys.Rev.Lett. 123,231802 (2019)LHCb uses a dedicated lineshape to take into account $\pi\pi \leftrightarrow KK$ rescattering, which is particularly significant in the region $1 < m_{KK} < 1.5~\text{GeV}/c^2$. See Ref.~\cite{Aaij:2019qps} for details.

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

SourceParameterCorrelation [%]Value$\Delta\chi^2$
fit${\cal B}(B^+ \to \phi(1020) \pi^+)$0.4$3.1\,^{+1.5}_{-1.4} \times 10^{-8}$
fit${\cal B}(B^+ \to \bar{K}^*(892)^0 K^+)$0.1$5.67\,^{+0.67}_{-0.64} \times 10^{-7}$
fit${\cal B}(B^+ \to \bar{K}_0^*(1430)^0 K^+)$0.1$3.7\,^{+1.3}_{-1.2} \times 10^{-7}$
fit${\cal B}(B^+ \to \rho(1450)^0 \pi^+) \times {\cal B}(\rho(1450)^0 \to K^+ K^-)$0.0$1.54 \pm0.11 \times 10^{-6}$
fit${\cal B}(B^+ \to K^+ K^- \pi^+ \mathrm{(NR)})$0.0$1.62\,^{+0.24}_{-0.23} \times 10^{-6}$
fit${\cal B}(B^+ \to f_2(1270) \pi^+) \times {\cal B}(f_2(1270) \to K^+ K^-)$0.0$3.77\,^{+0.58}_{-0.56} \times 10^{-7}$
fit${\cal B}(B^0 \to \pi^+ \pi^- \mu^+ \mu^-)$-0.0$2.06\,^{+0.54}_{-0.53} \times 10^{-8}$
fit${\cal B}(B_s^0 \to \pi^+ \pi^- \mu^+ \mu^-)$-0.0$8.4 \pm1.6 \times 10^{-8}$
fit${\cal B}(B^+ \to \pi^+ \mu^+ \mu^-)$-0.0$1.78 \pm0.23 \times 10^{-8}$
fit${\cal B}(\Lambda_b^0 \to p \pi^- \mu^+ \mu^-)$-0.0$6.9\,^{+2.7}_{-2.3} \times 10^{-8}$
fit${\cal{B}}( B^+ \to p \overline{\Lambda}(1520))$-0.0$3.05\,^{+0.84}_{-0.81} \times 10^{-7}$
fit${\cal{B}}(B^+ \to p \overline{p} K^+)$-0.0$1.062\,^{+0.057}_{-0.056} \times 10^{-5}$
fit${\cal{B}}( B^+ \to p \overline{p} K^+ ),~m_{p\overline{p}}<2.85~\rm{GeV/c^2}$-0.0$4.37\,^{+0.30}_{-0.29} \times 10^{-6}$
fit${\cal{B}}( B^+ \to p \overline{p} \pi^+ ),~m_{p\overline{p}}<2.85~\rm{GeV/c^2}$0.0$10.0 \pm1.1 \times 10^{-7}$
external${\cal{B}}(B^+ \to K^+ K^- \pi^+)$1.7$5.03 \pm0.25 \times 10^{-6}$0.00
external${\cal B}(\phi(1020) \to K^+ K^-)$-0.0$0.4920 \pm0.0050$0.00
external${\cal{B}}(K^*(1430) \to K \pi)$-0.0$0.930 \pm0.100$0.00
external${\cal B}(K^*(892)^0 \to K \pi)$-0.0$0.99754 \pm0.00021$0.00
external${\cal B}(B^0 \to J/\psi K^*(892)^0)$-0.0$1.270 \pm0.050 \times 10^{-3}$0.00
external${\cal B}(J/\psi \to \mu^+ \mu^-)$-0.0$5.961 \pm0.033 \times 10^{-2}$0.00
external${\cal B}(B^+ \to J/\psi K^+)$-0.0$1.020 \pm0.019 \times 10^{-3}$0.00
external${\cal B}(\Lambda_b^0 \to J/\psi p \pi^-)$-0.0$2.61\,^{+0.50}_{-0.40} \times 10^{-5}$0.00
external${\cal B}(J/\psi \to p \bar{p})$0.0$2.120 \pm0.029 \times 10^{-3}$0.00
external${\cal B}(\bar{\Lambda(1520)} \to K^+ p)$0.0$0.234 \pm0.016$0.00
external${\cal B}(B^+ \to J/\psi \pi^+)$0.0$3.920 \pm0.080 \times 10^{-5}$0.00
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.