| $\bf{
1.516 \pm0.006}$
|
OUR EVALUATION
$~~$(Produced by HFLAV)
|
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $1.518$ $\pm0.041$ $\pm0.027$ |
|
1 |
|
CDF |
| $1.398$ $\pm0.044$ ${}^{+0.028}_{-0.025}$ |
|
2 |
|
D0 |
| $1.42$ ${}^{+0.14}_{-0.13}$ $\pm0.03$ |
|
3 |
|
DLPH |
| $1.53$ ${}^{+0.16}_{-0.15}$ $\pm0.07$ |
|
4 |
|
DLPH |
| $1.36$ $\pm0.09$ ${}^{+0.06}_{-0.05}$ |
|
5 |
|
CDF |
| $1.72$ ${}^{+0.20}_{-0.19}$ ${}^{+0.18}_{-0.17}$ |
|
6 |
|
OPAL |
| $1.50$ ${}^{+0.16}_{-0.15}$ $\pm0.04$ |
|
5 |
|
OPAL |
| $1.47$ $\pm0.14$ $\pm0.08$ |
|
4 |
|
ALEP |
| $1.51$ $\pm0.11$ |
|
7 |
|
ALEP |
| $1.56$ ${}^{+0.29}_{-0.26}$ ${}^{+0.08}_{-0.07}$ |
|
5 |
|
DLPH |
| $1.65$ ${}^{+0.34}_{-0.31}$ $\pm0.12$ |
|
4 |
|
DLPH |
| $1.76$ $\pm0.20$ ${}^{+0.15}_{-0.10}$ |
|
8 |
|
DLPH |
| $1.60$ $\pm0.26$ ${}^{+0.13}_{-0.15}$ |
|
9 |
|
DLPH |
| $1.67$ $\pm0.14$ |
|
10 |
|
DLPH |
| $1.61$ ${}^{+0.30}_{-0.29}$ ${}^{+0.18}_{-0.16}$ |
90 |
4 |
|
ALEP |
| $1.54$ ${}^{+0.14}_{-0.13}$ $\pm0.04$ |
|
5 |
|
ALEP |
| $1.42$ ${}^{+0.27}_{-0.23}$ $\pm0.11$ |
76 |
5 |
|
CDF |
| $1.74$ ${}^{+1.08}_{-0.69}$ $\pm0.07$ |
8 |
11 |
|
CDF |
| $1.54$ ${}^{+0.25}_{-0.21}$ $\pm0.06$ |
79 |
5 |
|
OPAL |
| $1.59$ ${}^{+0.17}_{-0.15}$ $\pm0.03$ |
134 |
5 |
|
ALEP |
| $0.96$ $\pm0.37$ |
41 |
12 |
|
DLPH |
| $1.92$ ${}^{+0.45}_{-0.35}$ $\pm0.04$ |
31 |
5 |
|
ALEP |
| $1.13$ ${}^{+0.35}_{-0.26}$ $\pm0.09$ |
22 |
5 |
|
OPAL |
|
1
AALTONEN 2011AP combines the fully reconstrcuted ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{{s}}}^{-}}{{\mathit \pi}^{+}}$ decays and partially reconstructed ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{{s}}}}{{\mathit X}}$ decays.
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|
2
Measured using ${{\mathit D}_{{{s}}}}{{\mathit \mu}^{+}}$ vertices.
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|
3
Uses ${{\mathit D}_{{{s}}}^{-}}{{\mathit \ell}^{+}}$, and ${{\mathit \phi}}{{\mathit \ell}^{+}}$ vertices.
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|
4
Measured using ${{\mathit D}_{{{s}}}}$ hadron vertices.
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|
5
Measured using ${{\mathit D}_{{{s}}}^{-}}{{\mathit \ell}^{+}}$ vertices.
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|
6
ACKERSTAFF 1998F use fully reconstructed ${{\mathit D}_{{{s}}}^{-}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{-}}$ and ${{\mathit D}_{{{s}}}^{-}}$ $\rightarrow$ ${{\mathit K}^{*0}}{{\mathit K}^{-}}$ in the inclusive ${{\mathit B}_{{{s}}}^{0}}$ decay.
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|
7
Combined results from ${{\mathit D}_{{{s}}}^{-}}{{\mathit \ell}^{+}}$ and ${{\mathit D}_{{{s}}}}$ hadron.
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|
8
Measured using ${{\mathit \phi}}{{\mathit \ell}}$ vertices.
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|
9
Measured using inclusive ${{\mathit D}_{{{s}}}}$ vertices.
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|
10
Combined result for the four ABREU 1996F methods.
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|
11
Exclusive reconstruction of ${{\mathit B}_{{{s}}}}$ $\rightarrow$ ${{\mathit \psi}}{{\mathit \phi}}$.
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|
12
ABREU 1994E uses the flight-distance distribution of ${{\mathit D}_{{{s}}}}$ vertices, ${{\mathit \phi}}$-lepton vertices, and ${{\mathit D}_{{{s}}}}{{\mathit \mu}}$ vertices.
|