$\mathit CP$ VIOLATION

$\mathit A_{CP}$ is defined as
${B( {{\overline{\mathit B}}} \rightarrow {{\overline{\mathit f}}} )–B( {{\mathit B}} \rightarrow {{\mathit f}} )\over B( {{\overline{\mathit B}}} \rightarrow {{\overline{\mathit f}}} )+B( {{\mathit B}} \rightarrow {{\mathit f}} )}$,
the $\mathit CP$-violation charge asymmetry of inclusive ${{\mathit B}^{\pm}}$ and ${{\mathit B}^{0}}$ decay.

${{\overline{\mathit A}}}_{CP}$( ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{s}}}{{\mathit \gamma}}$ ) = ($\mathit A_{CP}$( ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit X}_{{s}}}{{\mathit \gamma}}$ ) + $\mathit A_{CP}$( ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit X}_{{s}}}{{\mathit \gamma}}$ ))/2

INSPIRE   PDGID:
S049A06
VALUE DOCUMENT ID TECN  COMMENT
$0.0091$ $\pm0.0121$ $\pm0.0013$ 1
WATANUKI
2019
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
1  Using a sum-of-exclusive technique with ${\mathit m}_{{{\mathit X}_{{s}}}}$ $<$ 2.8 GeV/c${}^{2}$.
Conservation Laws:
$\mathit CP$ INVARIANCE
References:
WATANUKI 2019
PR D99 032012 Measurements of isospin asymmetry and difference of direct $CP$ asymmetries in inclusive $B \to X_s \gamma$ decays