| $\bf{
1.430 \pm0.006}$
|
OUR EVALUATION
$~~$(Produced by HFLAV)
|
| $\bf{
1.452 \pm0.016}$
|
OUR AVERAGE
|
| $1.445$ $\pm0.016$ $\pm0.008$ |
1, 2 |
|
LHCB |
| $1.479$ $\pm0.034$ $\pm0.011$ |
1 |
|
LHCB |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $1.40$ $\pm0.02$ |
3 |
|
CMS |
| $1.379$ $\pm0.026$ $\pm0.017$ |
4 |
|
LHCB |
| $1.407$ $\pm0.016$ $\pm0.007$ |
5 |
|
LHCB |
| $1.440$ $\pm0.096$ $\pm0.009$ |
5 |
|
LHCB |
| $1.455$ $\pm0.046$ $\pm0.006$ |
5 |
|
LHCB |
|
6 |
|
CDF |
| $1.437$ ${}^{+0.054}_{-0.047}$ |
7, 8 |
|
CDF |
| $1.24$ ${}^{+0.14}_{-0.11}$ ${}^{+0.01}_{-0.02}$ |
8 |
|
D0 |
| $1.05$ ${}^{+0.16}_{-0.13}$ $\pm0.02$ |
8 |
|
CDF |
| $1.27$ $\pm0.33$ $\pm0.08$ |
9 |
|
ALEP |
|
1
Uses ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \eta}}$ decays.
|
|
2
AAIJ 2023P reports a ${{\mathit \tau}_{{{L}}}}$ value combined with AAIJ 2016AL result as ${{\mathit \tau}_{{{L}}}}$ = $1.452$ $\pm0.014$ $\pm0.007$ ps.
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|
3
Measured using results in SIRUNYAN 2018BY for the heavy ${{\mathit B}_{{{s}}}^{0}}$ lifetime obtained from ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays and the average effective ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}$ lifetime, and magnitude squared of the $\mathit CP$-odd amplitude $\vert A_{\perp}\vert ^2$ = $0.250$ $\pm0.006$. The uncertainty includes all statistical and systematic contributions.
|
|
4
Measured using ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{{s}}}^{-}}{{\mathit D}_{{{s}}}^{+}}$. The effective lifetime is translated into a decay width of $\Gamma _{L}$ = $0.725$ $\pm0.014$ $\pm0.009$ ps${}^{-1}$.
|
|
5
Measured using ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ decays. There may still be CPV in the decay.
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|
6
Uses the time-dependent angular analysis of ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}$ decays and assuming $\mathit CP$-violating angle ${{\mathit \beta}_{{{s}}}}$( ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}$) = 0.02.
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|
7
Obtained from $\Delta \Gamma _{s}$ and $\Gamma _{s}$ fit with a correlation of 0.6.
|
|
8
Measured using the time-dependent angular analysis of ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}$ decays.
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|
9
Uses ${{\mathit \phi}}{{\mathit \phi}}$ correlations from ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{{s}}}^{(*)+}}{{\mathit D}_{{{s}}}^{(*)-}}$.
|