$\bf{
0.89 \pm1.13}$
|
OUR EVALUATION
|
$\bf{
0.9 \pm1.1}$
|
OUR AVERAGE
|
$1.3$ $\pm6.3$ $\pm2.4$ |
3.8M |
1 |
|
LHCB |
$1.0$ $\pm1.1$ $\pm0.3$ |
|
2 |
|
LHCB |
$-3$ $\pm20$ $\pm7$ |
|
3 |
|
BELL |
$-12$ $\pm12$ |
1.8M |
4 |
|
CDF |
$9$ $\pm26$ $\pm6$ |
0.7M |
|
|
BABR |
$-59$ $\pm59$ $\pm21$ |
|
5 |
|
LHCB |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
$2.3$ $\pm1.5$ $\pm0.3$ |
|
1 |
|
LHCB |
$4.0$ $\pm2.8$ $\pm0.4$ |
|
1 |
|
LHCB |
$-4.4$ $\pm2.3$ $\pm0.6$ |
21M |
6 |
|
LHCB |
$2.5$ $\pm4.3$ $\pm0.7$ |
7M |
7 |
|
LHCB |
$-3.0$ $\pm3.2$ $\pm1.0$ |
9.6M |
5 |
|
LHCB |
$4.6$ $\pm5.8$ $\pm1.2$ |
3.0M |
8 |
|
LHCB |
$-13.4$ $\pm7.7$ ${}^{+2.6}_{-3.4}$ |
2.3M |
9 |
|
LHCB |
$-9.2$ $\pm14.5$ ${}^{+2.5}_{-3.3}$ |
0.8M |
10 |
|
LHCB |
$-3.5$ $\pm6.2$ $\pm1.2$ |
|
5 |
|
LHCB |
$3.3$ $\pm10.6$ $\pm1.4$ |
|
8 |
|
LHCB |
$26$ $\pm36$ $\pm8$ |
|
|
|
BABR |
$1$ $\pm30$ $\pm25$ |
|
|
|
BELL |
$80$ $\pm60$ $\pm20$ |
|
|
|
BABR |
1
Requires ${{\mathit D}^{0}}$ to originate from ${{\mathit D}^{*}{(2010)}^{+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$. Measures the parameter $\Delta {{\mathit Y}_{{{f}}}}$ $\simeq{}$ $−{{\mathit A}_{{{\Gamma}}}^{f}}$ up to 1$\%$ corrections from ${{\mathit y}_{{{CP}}}^{f}}$.
|
2
A combination of ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ and ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ from AAIJ 2021AI, AAIJ 2020, AAIJ 2017AK and AAIJ 2015AA
|
3
An improved measurement of ${{\overline{\mathit D}}^{0}}−{{\mathit D}^{0}}$ mixing and a search for $\mathit CP$ violation in ${{\mathit D}^{0}}$ decays to $\mathit CP$-even final states ${{\mathit K}^{+}}{{\mathit K}^{-}}$ and ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ using the final Belle data sample of 976 fb${}^{-1}$.
|
4
Combined result from ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ and ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$, with ${{\mathit D}^{0}}$ from ${{\mathit D}^{*+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$ (and cc).
|
5
Measured using ${{\mathit D}^{*+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$, ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ decays (and cc).
|
6
Measured using ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ decays, combines measurements with ${{\mathit D}^{0}}$ either from partially reconstructed semileptonic ${{\mathit B}}$ hadron decays or from ${{\mathit D}^{*+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$.
|
7
Measured using ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays, combines measurements with ${{\mathit D}^{0}}$ either from partially reconstructed semileptonic ${{\mathit B}}$ hadron decays or from ${{\mathit D}^{*+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$.
|
8
Measured using ${{\mathit D}^{*+}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$, ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays (and cc).
|
9
Measured using ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ decays, with ${{\mathit D}^{0}}$ from partially reconstructed semileptonic ${{\mathit B}}$ hadron decays.
|
10
Measured using ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays, with ${{\mathit D}^{0}}$ from partially reconstructed semileptonic ${{\mathit B}}$ hadron decays.
|