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\begin{tabular}{lrllll}
\hline
Exp.        & \1{$N_B$}  & \1{Mass [ $\mathrm{\,Me\kern -0.1em V}$ \xspace]} & \1{Width [ $\mathrm{\,Me\kern -0.1em V}$ \xspace]} & 
\1{$\sigma$} & \1{Frac.~[\%]\hskip-0.3cm} \\
\hline\hline
CDF [1] & 
$58$ & %
$4143.0\!\pm\!2.9\!\pm\!1.2$ & %
$11.7\,^{+\phantom{0}8.3}_{-\phantom{0}5.0}\!\pm\!3.7$ &
$3.8\phantom{\pm888}$ & \\
{\it Belle} [19] &
$\mathit{325}$ & %
$\mathit{4143.0}$ {\it fixed} & 
$\mathit{11.7}$ {\it fixed} &  
$\mathit{1.9\phantom{\pm888}}$ & \\
{\it CDF} [26] & 
$\mathit{115}$ & %
$\mathit{\!4143.4{^{+2.9}_{-3.0}}\!\pm\!\!0.6}$
 &
$\mathit{15.3\!^{+10.4}_{-\phantom{0}6.1}\!\!\pm\!\!2.5}$ & 
$\mathit{5.0\phantom{\pm888}}$ &
$\mathit{15\!\!\pm\!\!4\!\!\pm\!\!2}$ \\ 
LHCb [21] &
$346$ & %
$4143.4$ fixed & 
$15.3$ fixed   &
$1.4\phantom{\pm888}$        &
\quad $<\phantom{0}7$ \\ %
CMS [23] &
\!\!\!$\!2480$ & %
$4148.0\!\pm\!2.4\!\pm\!6.3$ &
$28\phantom{.0}\,^{+15\phantom{.0}}_{-11\phantom{.0}}\pm19$ & 
$5.0\phantom{\pm888}$ &
$10\!\pm\!3$ \\
D0 [25] &
$215$ & %
$4159.0\!\pm\!4.3\!\pm\!6.6$ &
$19.9\!\pm\!12.6\,^{+1.0}_{-8.0}$ &
$3.1\phantom{\pm888}$ &
$21\!\pm\!8\!\pm\!4$ \\
BaBar [22] &
$189$ & %
$4143.4$ fixed & 
$15.3$ fixed  &
$1.6\phantom{\pm888}$ &
\quad $<13$ \\%@~90\%CL \\
D0 [24] &
\1{--} &  %
$4152.5\!\pm\!1.7\,^{+6.2}_{-5.4}$ &
$16.3\!\pm\!5.6\!\pm\!\!11.4$ &
4.7--5.7$\phantom{\pm888}${\hskip-5cm\quad} & \quad\quad{--}
 \\
\hline
\!\!\! Average\!\!\!  &  & $4147.1\!\pm\!2.4$ & $15.7\!\pm\!6.3$ & & \\
\hline
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