| $\bf{
571 \pm19}$
|
OUR FIT
|
| $571$ $\pm13$ $\pm14$ |
7k |
1 |
|
LHCB |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $595$ $\pm26$ $\pm14$ |
7k |
2 |
|
LHCB |
|
1
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{+}}}–{\mathit m}_{{{\mathit B}^{0}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $431$ $\pm13$ $\pm14$ 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
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{+}}}–{\mathit m}_{{{\mathit B}^{0}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $455$ $\pm26$ $\pm14$ 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.
|
|
