\begin{table}%t5
\caption{\label{tab:fragmentation-results}Results from the fragmentation calibration setup.}
%\centering
\par
\begin{tabular}{c c c}
\hline\hline\noalign{\smallskip}
$K_0$ [kPa] & Slope $\alpha$ & Norm. largest fragment $\mu$ \\
\hline
3.00	& 0.361	 $\pm$  0.004  & 0.200 $\pm$  0.008 \\ 
3.50	& 0.429	 $\pm$  0.002  & 0.172 $\pm$  0.002 \\ 
4.00	& 0.518	 $\pm$  0.011  & 0.230 $\pm$  0.009 \\ 
4.25    & 0.523	 $\pm$   0.006  & 0.194  $\pm$  0.004 \\
4.50	& 0.673             $\pm$  0.017  & 0.234  $\pm$  0.007 \\ 
4.75	& 0.834             $\pm$  0.025  & 0.196  $\pm$  0.005 \\ 
5.00	& 0.832             $\pm$  0.063  & 0.198  $\pm$  0.011 \\ 
5.50	& 0.836             $\pm$  0.052  & 0.220  $\pm$  0.010 \\ 
6.00	& 2.027             $\pm$  0.121  & 0.171  $\pm$  0.002 \\ 
6.50	& 0.910             $\pm$  0.053  & 0.390  $\pm$  0.013 \\ 
\hline
\end{tabular}
\tablefoot {The slope $\alpha$ of the power~law increases with increasing bulk modulus~$K_0$. Remarkably, the size of the normalised biggest fragment remains nearly constant around $\mu \approx 0.2$ for $K_0 \le 6.0$~kPa.}
\end{table}