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

INSPIRE   PDGID:

M151M

VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT $\bf{ 5698 \pm8}$ OUR AVERAGE  Error includes scale factor of 1.2. $5710$ $\pm20$ 1 AFFOLDER 2001 F CDF ${{\mathit p}}{{\overline{\mathit p}}}$ at 1.8 TeV $5695$ ${}^{+17}_{-19}$ 2 BARATE 1998 L ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}$ $5704$ $\pm4$ $\pm10$ 1944 3 BUSKULIC 1996 D ALEP ${\it{}E}^{\it{}ee}_{\rm{}cm}$= $88 - 94$ GeV $5732$ $\pm5$ $\pm20$ 2157 ABREU 1995 B DLPH ${\it{}E}^{\it{}ee}_{\rm{}cm}$= $88 - 94$ GeV $5681$ $\pm11$ 1738 AKERS 1995 E 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 1999 N 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( ${{\mathit b}}$ $\rightarrow$ ${{\mathit B}}{}^{**}$)= $0.32$ $\pm0.03$ $\pm0.06$. 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