$159$ $\pm23$ $\pm77$ |
|
1 |
|
LHCB |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
$69.9$ $\pm3.2$ $\pm6.6$ |
36k |
2, 3 |
|
LHCB |
$48$ $\pm3$ $\pm6$ |
3122 |
4, 3 |
|
BABR |
$47$ $\pm7$ $\pm10$ |
|
5 |
|
BABR |
1
Separated from the spin-3 component ${{\mathit D}_{{s3}}^{*}{(2860)}^{-}}$ by a fit of the helicity angle of the ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$ system, with a statistical significance of the spin-3 and spin-1 components in excess of 10 $\sigma $.
|
2
From the combined fit of the ${{\mathit D}^{+}}{{\mathit K}_S^0}$ and ${{\mathit D}^{0}}{{\mathit K}^{+}}$ modes in the model including the ${{\mathit D}_{{s2}}^{*}{(2573)}^{+}}$, ${{\mathit D}_{{s1}}^{*}{(2700)}^{+}}$ and spin-0 ${{\mathit D}_{{sJ}}^{*}{(2860)}^{+}}$.
|
3
Possible contribution from the ${{\mathit D}_{{s3}}^{*}{(2860)}}$ state.
|
4
From simultaneous fits to the two ${{\mathit D}}{{\mathit K}}$ mass spectra and to the total ${{\mathit D}^{*}}{{\mathit K}}$ mass spectrum.
|
5
Superseded by AUBERT 2009AR.
|
|