\begin{table}%t4 %\centering \par \caption{\label{tab:collision_table3lowz}As Table~\ref{tab:collision_table3} but for $Z=0.001^{a}$.} \small \begin{tabular}{rrrrrr} \hline\hline $N$ & $t$ & $M_{1,N\mbox{-}{\rm body}}$ & $M_{1,{\rm mix}}$ & $M_2$ & $M_{\rm merger}$\\ \hline 1 & 0.53120 & 77.8 & 77.7 & 70.7 & 135.4\\ 2 & 0.57294 & 148.5 & 135.4 & 82.8 & 198.3\\ 3 & 0.65612 & 231.3 & 198.1 & 58.5 & 239.6\\ 4 & 0.89154 & 289.8 & 239.1 & 96.6 & 308.5\\ 5 & 0.89155 & 386.4 & 308.5 & 78.5 & 364.2\\ 6 & 1.02208 & 464.9 & 363.5 & 1.5 & 364.9\\ 7 & 1.31086 & 466.4 & 363.4 & 56.3 & 404.7\\ 8 & 1.50575 & 522.6 & 403.4 & 48.9 & 440.2\\ 9 & 2.05327 & 571.3 & 434.9 & 72.7 & 487.5\\ 10 & 2.27966 & 643.8 & 390.1 & 2.0 & 392.0\\ 11 & 2.60213 & 645.0 & 260.1 & 3.5 & 263.3\\ & 2.83153 & 648.5 & 171.9$^{b}$ \\ \hline \end{tabular} \begin{list}{}{} \item[$^{a}$] Note that the merger sequence was terminated earlier than for $Z=0.02$ and that the merger remnant did not finish its evolution before the evolution code broke down. \item[$^{b}$] Mass and time at the moment the evolution code broke down, rather than the onset of carbon burning. \end{list} \end{table}