| $\bf{
5366.93 \pm0.10}$
|
OUR FIT
|
| $\bf{
5366.91 \pm0.11}$
|
OUR AVERAGE
|
| $5366.98$ $\pm0.07$ $\pm0.13$ |
|
1 |
|
LHCB |
| $5366.85$ $\pm0.19$ $\pm0.13$ |
|
2 |
|
LHCB |
| $5366.83$ $\pm0.25$ $\pm0.27$ |
|
3 |
|
LHCB |
| $5367.08$ $\pm0.38$ $\pm0.15$ |
128 |
4 |
|
LHCB |
| $5366.90$ $\pm0.28$ $\pm0.23$ |
|
5 |
|
LHCB |
| $5364.4$ $\pm1.3$ $\pm0.7$ |
|
|
|
BELL |
| $5366.01$ $\pm0.73$ $\pm0.33$ |
|
6 |
|
CDF |
| $5369.9$ $\pm2.3$ $\pm1.3$ |
32 |
7 |
|
CDF |
| $5374$ $\pm16$ $\pm2$ |
3 |
|
|
DLPH |
| $5359$ $\pm19$ $\pm7$ |
1 |
7 |
|
OPAL |
| $5368.6$ $\pm5.6$ $\pm1.5$ |
2 |
|
|
ALEP |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $5370$ $\pm1$ $\pm3$ |
|
|
|
BELL |
| $5370$ $\pm40$ |
6 |
8 |
|
OPAL |
| $5383.3$ $\pm4.5$ $\pm5.0$ |
14 |
|
|
CDF |
|
1
Uses ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ decays.
|
|
2
Uses ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit p}}{{\overline{\mathit p}}}$ decays.
|
|
3
Uses ${{\mathit B}_{{{s}}}}$ $\rightarrow$ ${{\mathit \chi}_{{{c1}}}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ mode.
|
|
4
Uses ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$, ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ decays, and observes $128$ $\pm13$ events of ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}{{\mathit \phi}}$.
|
|
5
Uses ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}$ fully reconstructed decays.
|
|
6
Uses exclusively reconstructed final states containing a ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ decays.
|
|
7
From the decay ${{\mathit B}_{{{s}}}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \phi}}$.
|
|
8
From the decay ${{\mathit B}_{{{s}}}}$ $\rightarrow$ ${{\mathit D}_{{{s}}}^{-}}{{\mathit \pi}^{+}}$.
|