${{\mathit B}_{{{J}}}^{*}{(5732)}}$ MASS INSPIRE search

M151M
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 5698 \pm8}$ OUR AVERAGE  Error includes scale factor of 1.2.
$5710$ $\pm20$ 1
AFFOLDER
2001F
 CDF ${{\mathit p}}{{\overline{\mathit p}}}$ at 1.8 TeV
$5695$ ${}^{+17}_{-19}$ 2
BARATE
1998L
 ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}$
$5704$ $\pm4$ $\pm10$ 1944 3
BUSKULIC
1996D
 ALEP ${\it{}E}^{\it{}ee}_{\rm{}cm}$= $88 - 94$ GeV
$5732$ $\pm5$ $\pm20$ 2157
ABREU
1995B
 DLPH ${\it{}E}^{\it{}ee}_{\rm{}cm}$= $88 - 94$ GeV
$5681$ $\pm11$ 1738
AKERS
1995E
 OPAL ${\it{}E}^{\it{}ee}_{\rm{}cm}$= $88 - 94$ GeV
• • • We do not use the following data for averages, fits, limits, etc. • • •
$5713$ $\pm2$ 4
ACCIARRI
1999N
 L3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}$
1  AFFOLDER 2001F uses the reconstructed ${{\mathit B}}~$meson through semileptonic decay channels. The fraction of light ${{\mathit B}}~$mesons that are produced at $\mathit L$=1 ${{\mathit B}^{{**}}}$ states is measured to be $0.28$ $\pm0.06$ $\pm0.03$.
2  BARATE 1998L uses fully reconstructed ${{\mathit B}}$ mesons to search for ${{\mathit B}}{}^{**}$ production in the ${{\mathit B}}{{\mathit \pi}^{\pm}}$ system. In the framework of heavy quark symmetry (HQS), they also measured the mass of ${{\mathit B}_{{{2}}}^{*}}$ to be $5739$ ${}^{+8}_{-11}{}^{+6}_{-4}$ MeV/$\mathit c{}^{2}$ and the relative production rate of B( ${{\mathit b}}$ $\rightarrow$ ${{\mathit B}_{{{2}}}^{*}}$ $\rightarrow$ ${{\mathit B}}{}^{(*)}$ ${{\mathit \pi}}$)/B( ${{\mathit b}}$ $\rightarrow$ ${{\mathit B}}$ $_{{{\mathit u}},{{\mathit d}}}$) = ($31$ $\pm9$ ${}^{+6}_{-5})\%$.
3  Using ${\mathit m}_{\mathrm {{{\mathit B}} {{\mathit \pi}}}}−{\mathit m}_{{{\mathit B}}}$ = $424$ $\pm4$ $\pm10$ MeV.
4  ACCIARRI 1999N uses inclusive reconstructed ${{\mathit B}}$ mesons to search for ${{\mathit B}}{}^{**}$ production in the ${{\mathit B}}{}^{(*)}{{\mathit \pi}^{\pm}}$ system. In the framework of HQET, they measured the mass of ${{\mathit B}^{*}_{\mathrm 1}}$ and ${{\mathit B}^{*}_{\mathrm 2}}$ to be $5670$ $\pm10$ $\pm13~$MeV and $5768$ $\pm5$ $\pm6$ with the B( ${{\mathit b}}$ $\rightarrow$ ${{\mathit B}}{}^{**}$)= ($32$ $\pm3$ $\pm6$) $ \times 10^{-2}$. They also reported the evidence for the existence of an excited ${{\mathit B}}$-meson state or mixture of states in the region $5.9 - 6.0$ GeV.
  References:
AFFOLDER 2001F
PR D64 072002 Observation of Orbitally Excited ${{\mathit B}}$ Mesons in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$= 1.8 TeV
ACCIARRI 1999N
PL B465 323 Measurement of the Spectroscopy of Orbitally Excited ${{\mathit B}}$ Mesons at LEP
BARATE 1998L
PL B425 215 Resonant Structure and Flavour Tagging in the ${{\mathit B}}$ ${{\mathit \pi}^{\pm}}$ System using Fully Reconstructed ${{\mathit B}}$ Decays
BUSKULIC 1996D
ZPHY C69 393 Production of Excited Beauty States in ${{\mathit Z}}$ Decays
ABREU 1995B
PL B345 598 Observation of Orbitally Excited ${{\mathit B}}$ Mesons
AKERS 1995E
ZPHY C66 19 Observations of ${{\mathit \pi}}$ $−$ ${{\mathit B}}$ Charge Flavor Correlations and Resonant ${{\mathit B}}$ ${{\mathit \pi}}$ and ${{\mathit B}}$ ${{\mathit K}}$ Production