${{\mathit B}^{0}}$ MASS

INSPIRE   PDGID:
S042M
The fit uses ${\mathit m}_{{{\mathit B}^{+}}}$, (${\mathit m}_{{{\mathit B}^{0}}}–{\mathit m}_{{{\mathit B}^{+}}}$), and ${\mathit m}_{{{\mathit B}^{0}}}$ to determine ${\mathit m}_{{{\mathit B}^{+}}}$, ${\mathit m}_{{{\mathit B}^{0}}}$, and the mass difference.
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 5279.72 \pm0.08}$ OUR FIT
$\bf{ 5279.63 \pm0.20}$ OUR AVERAGE
$5279.74$ $\pm0.30$ $\pm0.10$ 1
AAIJ
2019U
LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8, 13 TeV
$5279.6$ $\pm0.2$ $\pm1.0$ 2
AAD
2013U
ATLS ${{\mathit p}}{{\mathit p}}$ at 7 TeV
$5279.58$ $\pm0.15$ $\pm0.28$ 3
AAIJ
2012E
LHCB ${{\mathit p}}{{\mathit p}}$ at 7 TeV
$5279.63$ $\pm0.53$ $\pm0.33$ 4
ACOSTA
2006
CDF ${{\mathit p}}{{\overline{\mathit p}}}$ at 1.96 TeV
$5279.1$ $\pm0.7$ $\pm0.3$ 135 5
CSORNA
2000
CLE2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5281.3$ $\pm2.2$ $\pm1.4$ 51
ABE
1996B
CDF ${{\mathit p}}{{\overline{\mathit p}}}$ at 1.8 TeV
• • We do not use the following data for averages, fits, limits, etc. • •
$5279.2$ $\pm0.54$ $\pm2.0$ 340
ALAM
1994
CLE2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5278.0$ $\pm0.4$ $\pm2.0$
BORTOLETTO
1992
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5279.6$ $\pm0.7$ $\pm2.0$ 40 6
ALBRECHT
1990J
ARG ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5278.2$ $\pm1.0$ $\pm3.0$ 40
ALBRECHT
1987C
ARG ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5279.5$ $\pm1.6$ $\pm3.0$ 7 7
ALBRECHT
1987D
ARG ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$5280.6$ $\pm0.8$ $\pm2.0$
BEBEK
1987
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
1  Uses ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit p}}{{\overline{\mathit p}}}$ decays.
2  Measured with ${{\mathit B}_{{{d}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}({{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$) ${{\mathit K}_S^0}$ (${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$) decays.
3  Uses ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{0}}$ fully reconstructed decays.
4  Uses exclusively reconstructed final states containing a ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ decays.
5  CSORNA 2000 uses fully reconstructed 135 ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{}^{(')}$ ${{\mathit K}_S^0}$ events and invariant masses without beam constraint.
6  ALBRECHT 1990J assumes 10580 for ${{\mathit \Upsilon}{(4S)}}$ mass. Supersedes ALBRECHT 1987C and ALBRECHT 1987D.
7  Found using fully reconstructed decays with ${{\mathit J / \psi}}$. ALBRECHT 1987D assume ${\mathit m}_{{{\mathit \Upsilon}{(4S)}}}$ = 10577 MeV.
References