$\bf{
691 \pm5}$
|
OUR FIT
|
$\bf{
691 \pm5}$
|
OUR AVERAGE
|
$689.9$ $\pm2.9$ $\pm5.1$ |
10K |
1 |
|
LHCB |
$698$ $\pm5$ $\pm12$ |
2.6k |
2 |
|
CDF |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
$714.3$ $\pm6.4$ $\pm5.1$ |
10K |
3 |
|
LHCB |
1
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{0}}}{\mathit m}_{{{\mathit B}^{+}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{-}}}$ = $550.4$ $\pm2.9$ $\pm5.1$ MeV which we adjust by the ${{\mathit \pi}^{-}}$ mass. The masses inside the square brackets were measured for each candidate event. The result assumes $\mathit P$ = ($-1){}^{J}$ and uses two relativistic Breit-Wigner functions in the fit for mass difference.
|
2
AALTONEN 2014I reports ${\mathit m}_{{{\mathit B}_{{J}}{(5970)}^{0}}}$ $−$ ${\mathit m}_{{{\mathit B}^{+}}}$ $−$ ${\mathit m}_{{{\mathit \pi}^{-}}}$ = $558$ $\pm5$ $\pm12$ MeV which we adjusted by the ${{\mathit \pi}^{-}}$ mass.
|
3
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{0}}}{\mathit m}_{{{\mathit B}^{+}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{-}}}$ = $575$ $\pm6$ $\pm5$ MeV which we adjust by the ${{\mathit \pi}^{-}}$ mass. The masses inside the square brackets were measured for each candidate event. The result assumes $\mathit P$ = ($-1){}^{J}$ and uses three relativistic Breit-Wigner functions in the fit for mass difference.
|