${{\mathit D}^{\pm}}$ $\mathit CP$-VIOLATING DECAY-RATE ASYMMETRIES

This is the difference between ${{\mathit D}^{+}}$ and ${{\mathit D}^{-}}$ partial widths for the decay to state ${{\mathit f}}$, divided by the sum of the widths:$
$ $\mathit A_{CP}({{\mathit f}}$)= [$\Gamma $( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit f}}$ ) $−$ $\Gamma $( ${{\mathit D}^{-}}$ $\rightarrow$ ${{\overline{\mathit f}}}$ )]/[$\Gamma $( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit f}}$ ) + $\Gamma $( ${{\mathit D}^{-}}$ $\rightarrow$ ${{\overline{\mathit f}}}$ )].

$\mathit A_{\mathit CP}$( ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}$ ) in ${{\mathit D}^{\pm}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}$

INSPIRE   PDGID:
S031A6
VALUE (%) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ -0.01 \pm0.07 }$ OUR AVERAGE
$-0.004$ $\pm0.061$ $\pm0.045$ 6M
AAIJ
2019T
LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8, 13 TeV
$-1.8$ $\pm2.7$ $\pm1.6$ 780
ABLIKIM
2019M
BES3 ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at 3773 MeV
$-0.25$ $\pm0.28$ $\pm0.14$ 277k
KO
2013
BELL ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at ${{\mathit \Upsilon}{(nS)}}$
$0.13$ $\pm0.36$ $\pm0.25$ 159k
LEES
2013E
BABR ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at ${{\mathit \Upsilon}{(4S)}}$
$-0.2$ $\pm1.5$ $\pm0.9$ 5.2k
MENDEZ
2010
CLEO ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at 3774 MeV
$7.1$ $\pm6.1$ $\pm1.2$ 949 1
LINK
2002B
FOCS ${{\mathit \gamma}}$ nucleus, ${{\overline{\mathit E}}}_{\gamma }\approx{}$180 GeV
• • We do not use the following data for averages, fits, limits, etc. • •
$-0.16$ $\pm0.58$ $\pm0.25$
KO
2010
BELL ${{\mathit e}^{+}}{{\mathit e}^{-}}$ $\approx{}{{\mathit \Upsilon}{(4S)}}$
$6.9$ $\pm6.0$ $\pm1.5$ 949 2
LINK
2002B
FOCS ${{\mathit \gamma}}$ nucleus, ${{\overline{\mathit E}}}_{\gamma }\approx{}$180 GeV
1  LINK 2002B measures $\mathit N$( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$ )/$\mathit N$( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}$ ), the ratio of numbers of events observed, and similarly for the ${{\mathit D}^{-}}$.
2  LINK 2002B measures $\mathit N$( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$ )/$\mathit N$( ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}$ ), the ratio of numbers of events observed, and similarly for the ${{\mathit D}^{-}}$.
Conservation Laws:
$\mathit CP$ INVARIANCE
References:
AAIJ 2019T
PRL 122 191803 Search for $CP$ violation in $D_s^+\to K_S^0 \pi^+$, $D^+\to K_S^0 K^+$ and $D^+\to \phi \pi^+$ decays
ABLIKIM 2019M
PR D99 032002 Measurements of the absolute branching fractions and $CP$ asymmetries for $D^+\rightarrow K_{S,L}^0 K^+(\pi^0)$
KO 2013
JHEP 1302 098 Search for $\mathit CP$ Violation in the Decay ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$
LEES 2013E
PR D87 052012 Search for $\mathit CP$ Violation in the Decays ${{\mathit D}^{\pm}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}$ , ${{\mathit D}_{{s}}^{\pm}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}$ , and ${{\mathit D}_{{s}}^{\pm}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{\pm}}$
KO 2010
PRL 104 181602 Search for $\mathit CP$ Violation in the Decays ${{\mathit D}_{{{}(s)}}}^{+}} \rightarrow {{\mathit K}_S^0} {{\mathit \pi}^{+}} and {{\mathit D}_{{{}(s)}}}^{+}} \rightarrow {{\mathit K}_S^0} {{\mathit K}^{+}}
MENDEZ 2010
PR D81 052013 Measurements of ${{\mathit D}}$ Meson Decays to Two Pseudoscalar Mesons
LINK 2002B
PRL 88 041602 Search for $\mathit CP$ Violation in the Decays ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}$ and ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$
Also
PRL 88 159903 (errat.) Erratum: LINK 2002B Search for $\mathit CP$ Violation in the Decays ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}$ and ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$