BOTTOM MESONS
($\mathit B$ = $\pm1$)
${{\mathit B}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit b}}}$, ${{\mathit B}^{0}}$ = ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit b}}}$, ${{\overline{\mathit B}}^{0}}$ = ${\mathit {\overline{\mathit d}}}$ ${\mathit {\mathit b}}$, ${{\mathit B}^{-}}$ = ${\mathit {\overline{\mathit u}}}$ ${\mathit {\mathit b}}$,
similarly for ${{\mathit B}^{*}}$'s 		INSPIRE   JSON PDGID:
S051

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

 
$\mathbf {Production fractions at {{\mathit Z}}}$
${{\mathit B}^{\pm}}/{{\mathit B}^{0}}/{{\mathit B}_{{{s}}}^{0}}/{{\mathit b}}$-baryon ADMIXTURE MEAN LIFE   $(1.5673 \pm0.0029) \times 10^{-12}$ 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   $0.1259 \pm0.0042$  
 
$\mathit CP$ VIOLATION PARAMETERS in semileptonic ${\mathit {\mathit b}}$-hadron decays.
Re($\epsilon _{{\mathit {\mathit b}}}$) $/$ (1 + $\vert \epsilon _{{\mathit {\mathit b}}}$ $\vert {}^{2}$)
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, the production fractions are provided separately at three different colliders (LEP, ${{\mathit p}}{{\overline{\mathit p}}}$ Tevatron, and ${{\mathit p}}{{\mathit p}}$ LHC) and are used for the subsequent measurements accordingly.

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.
FOOTNOTES