BOTTOM MESONS
($\boldsymbol B$ = $\pm1$)
${{\mathit B}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit b}}}$, ${{\mathit B}^{0}}$ = ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit b}}}$, ${{\overline{\mathit B}}^{0}}$ = ${\mathit {\overline{\mathit d}}}$ ${\mathit {\mathit b}}$, ${{\mathit B}^{-}}$ = ${\mathit {\overline{\mathit u}}}$ ${\mathit {\mathit b}}$,
similarly for ${{\mathit B}^{*}}$'s
INSPIRE search

${{\boldsymbol B}^{\pm}}/{{\boldsymbol B}^{0}}/{{\boldsymbol B}_{{s}}^{0}}/{{\boldsymbol b}}$-baryon ADMIXTURE

${{\mathit B}^{\pm}}/{{\mathit B}^{0}}/{{\mathit B}_{{s}}^{0}}/{{\mathit b}}$-baryon ADMIXTURE MEAN LIFE   $(1566 \pm3) \times 10^{-15}$ s 
CHARGED ${{\mathit b}}$-HADRON ADMIXTURE MEAN LIFE   $(1.72 \pm0.10) \times 10^{-12}$ s 
NEUTRAL ${{\mathit b}}$-HADRON ADMIXTURE MEAN LIFE   $(1.58 \pm0.14) \times 10^{-12}$ s 
MEAN LIFE RATIO ${\mathit \tau}_{\mathrm {charged~{{\mathit b}}-hadron}}/{\mathit \tau}_{\mathrm {neutral~{{\mathit b}}-hadron}}$   $1.09 \pm0.13$  
$\vert \Delta {\mathit \tau}_{{{\mathit b}}}\vert /{\mathit \tau}_{\mathrm {{{\mathit b}},{{\overline{\mathit b}}}}}$   $-0.001 \pm0.014$  
$\chi _{\mathit b}$ AT HIGH ENERGY   $0.1284 \pm0.0069$  
$\boldsymbol CP$ VIOLATION PARAMETERS in semileptonic ${\boldsymbol {\boldsymbol b}}$-hadron decays.
Re($\epsilon _{{\mathit {\mathit b}}}$) $/$ (1 + $\vert \epsilon _{{\mathit {\mathit b}}}$ $\vert {}^{2}$)   $-0.0013 \pm0.0004$  
${{\boldsymbol B}}$-HADRON PRODUCTION FRACTIONS IN HADRONIC ${{\boldsymbol Z}}$ DECAY
${{\boldsymbol B}}$-HADRON PRODUCTION FRACTIONS IN ${{\boldsymbol p}}{{\overline{\boldsymbol p}}}$ COLLISIONS AT Tevatron
PRODUCTION ASYMMETRIES
A${}^{ {{\mathit b}} {{\overline{\mathit b}}} }_{C}$   $0.007 \pm0.004$  
The branching fraction measurements are for an admixture of ${{\mathit B}}$ mesons and baryons at energies above the ${{\mathit \Upsilon}{(4S)}}$. Only the highest energy results (LHC, LEP, Tevatron, S ${{\mathit p}}{{\overline{\mathit p}}}$ S) are used in the branching fraction averages. In the following, we assume that the production fractions are the same at the LHC, LEP, and at the Tevatron.
For inclusive branching fractions, $\mathit e.g.,$ ${{\mathit B}}$ $\rightarrow$ ${{\mathit D}^{\pm}}$ anything, the values usually are multiplicities, not branching fractions. They can be greater than one.
The modes below are listed for a ${{\overline{\mathit b}}}$ initial state. ${{\mathit b}}~$modes are their charge conjugates. Reactions indicate the weak decay vertex and do not include mixing.