| $\bf{
685 \pm5}$
|
OUR FIT
|
| $\bf{
685 \pm5}$
|
OUR AVERAGE
|
| $685.3$ $\pm4.1$ $\pm2.5$ |
2K |
1 |
|
LHCB |
| $681$ $\pm5$ $\pm12$ |
1.4k |
2 |
|
CDF |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $686.8$ $\pm4.5$ $\pm2.5$ |
2K |
3 |
|
LHCB |
|
1
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{+}}}–{\mathit m}_{{{\mathit B}^{0}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $545.8$ $\pm4.1$ $\pm2.5$ 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 ${\mathit m}_{{{\mathit B}_{{J}}{(5970)}^{+}}}$ $−$ ${\mathit m}_{{{\mathit B}^{0}}}$ $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $541$ $\pm5$ $\pm12$ MeV which we adjusted by the ${{\mathit \pi}^{+}}$ mass.
|
|
3
AAIJ 2015AB reports [${\mathit m}_{{{\mathit B}_{{J}}^{+}}}–{\mathit m}_{{{\mathit B}^{0}}}$] $−$ ${\mathit m}_{{{\mathit \pi}^{+}}}$ = $547$ $\pm5$ $\pm3$ 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.
|
