OUR FIT uses ${\mathit m}_{{{\mathit B}^{+}}}$, ${\mathit m}_{{{\mathit B}_{{{1}^}}^{0}}}–{\mathit m}_{{{\mathit B}^{+}}}$, and mass differences below to determine ${\mathit m}_{{{\mathit B}_{{{2}}}^{*}{(5747)}^{0}}}$. The $-0.659$ correlation between statistical uncertainties of ${\mathit m}_{{{\mathit B}_{{{1}^}}^{0}}}–{\mathit m}_{{{\mathit B}^{+}}}$ and ${\mathit m}_{{{\mathit B}_{{{2}}}^{*0}}}–{\mathit m}_{{{\mathit B}_{{{1}}}^{0}}}$ measurements reported by ABAZOV 2007T is taken into account.