${{\boldsymbol B}_{{s2}}^{*}{(5840)}^{0}}$ MASS INSPIRE search

VALUE (MeV) DOCUMENT ID TECN  COMMENT
$\bf{ 5839.86 \pm0.12}$ OUR FIT
$\bf{ 5839.92 \pm0.14}$ OUR AVERAGE
$5839.86$ $\pm0.09$ $\pm0.17$
SIRUNYAN
2018DF
CMS ${{\mathit p}}{{\mathit p}}$ at 8 TeV
$5839.99$ $\pm0.05$ $\pm0.20$
AAIJ
2013O
LHCB ${{\mathit p}}{{\mathit p}}$ at 7 TeV
$5839.6$ $\pm1.1$ $\pm0.7$ 1
ABAZOV
2008E
D0 ${{\mathit p}}{{\overline{\mathit p}}}$ at 1.96 TeV
• • • We do not use the following data for averages, fits, limits, etc. • • •
$5839.7$ $\pm0.7$ 2
AALTONEN
2008K
CDF Repl. by AALTONEN 2014I
1  Observed in ${{\mathit B}_{{s2}}^{*0}}$ $\rightarrow$ ${{\mathit B}^{+}}{{\mathit K}^{-}}$ . Measured production rate of ${{\mathit B}_{{s2}}^{*0}}$ relative to ${{\mathit B}^{+}}$ to be ($1.15$ $\pm0.23$ $\pm0.13)\%$.
2  Uses two-body decays into ${{\mathit K}^{-}}$ and ${{\mathit B}^{+}}$ mesons reconstructed as ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{+}}$ , ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ or ${{\mathit B}^{+}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}$ , ${{\overline{\mathit D}}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ .
  References:
SIRUNYAN 2018DF
EPJ C78 939 Studies of ${\mathrm {B}} ^{*{\mathrm {s}}2}(5840)^0 $ and ${\mathrm {B}} _{{\mathrm {s}}1}(5830)^0 $ mesons including the observation of the ${\mathrm {B}} ^{*{\mathrm {s}}2}(5840)^0 \rightarrow {\mathrm {B}} ^0 \mathrm {K} ^0_{\mathrm {S}} $ decay in proton-proton collisions at $\sqrt{s}=8\,\text {TeV} $
AAIJ 2013O
PRL 110 151803 First Observation of the Decay ${{\mathit B}_{{s2}}^{*}{(5840)}^{0}}$ $\rightarrow$ ${{\mathit B}^{*+}}{{\mathit K}^{-}}$ and Studies of Excited ${{\mathit B}_{{s}}^{0}}$ Mesons
AALTONEN 2008K
PRL 100 082001 Observation of Orbitally Excited ${{\mathit B}_{{s}}}$ Mesons
ABAZOV 2008E
PRL 100 082002 Observation and Properties of the Orbitally Excited ${{\mathit B}^{*}_{{s2}}}$ Meson