\begin{table}%t6%t7 \caption{\label{arcs_radio_all}Predicted number of radio (1.4~GHz) arcs produced by SMGs for an all-sky survey, using all the synthetic cluster population to compute the optical depths (see Fig.~\ref{fig:arcCounts}).} \small%\centerline { \begin{tabular}{@{\extracolsep{-1mm}}c|cc|cc|cc|cc|cc|cc} \hline\hline &&&&&&&&&&&& \\[-8pt] $B_{1.4~{\rm GHz}}^{~(1)}$ & \multicolumn{2}{c|}{$\rm 500~\mu Jy~arcsec^{-2}$} & \multicolumn{2}{c|}{$\rm 100~\mu Jy~arcsec^{-2}$} & \multicolumn{2}{c|}{$\rm 50~\mu Jy~arcsec^{-2}$} & \multicolumn{2}{c|}{$\rm 10~\mu Jy~arcsec^{-2}$} & \multicolumn{2}{c|}{$\rm 5~\mu Jy~arcsec^{-2}$} & \multicolumn{2}{c}{$\rm 1~\mu Jy~arcsec^{-2}$} \\ $d_{0}^{~(2)}$ & $7.5$ & $10$ & $7.5$ & $10$ & $7.5$ & $10$ & $7.5$ & $10$ & $7.5$ & $10$ & $7.5$ & $10$ \\ &&&&&&&&&&&& \\[-8pt] \hline &&&&&&&&&&&& \\[-8pt] SPZ DB$^{~(3)}$ &50 (8) &25 (0) &583 (233) &250 (100) &1333 (575) &575 (250) &8275 (3792) &3600 (1650) &18~283 (8275) &7950 (3600) &110~017 (50767) &47~825 (22075) \\ PHZ DB$^{~(3)}$ &50 (8) &17 (0) &550 (225) &233 (92) &1258 (550) &542 (233) &7800 (3575) &3342 (1533) &17~242 (7800) &7383 (3342) &103~783 (47892) &44~450 (20517) \\ CHM DB$^{~(3)}$ &100 (17) &42 (8) &1142 (458) &517 (208) &2608 (1142) &1167 (517) &16~200 (7425) &7267 (3325) &35~808 (16200) &16~058 (7267) &215~517 (99458) &96~633 (44592) \\ \hline &&&&&&&&&&&& \\[-8pt] SPZ SM$^{~(3)}$ &42 (8) &17 (0) &542 (225) &233 (100) &1058 (542) &458 (233) &3567 (2208) &1550 (958) &5608 (3567) &2433 (1567) &14~325 (9658) &2394 (4200) \\ PHZ SM$^{~(3)}$ &42 (8) &17 (0) &508 (208) &217 (92) &1000 (508) &425 (217) &3367 (2083) &1442 (892) &5292 (3367) &2267 (1442) &13~508 (9117) &5783 (3900) \\ CHM SM$^{~(3)}$ &83 (8) &42 (8) &1058 (442) &475 (200) &2075 (1058) &933 (475) &6992 (4317) &3133 (1933) &10~983 (6992) &492 (3133) &28~058 (18925) &12~583 (8483) \\ \hline \end{tabular}} \medskip $^{(1)}$~Surface brightness limit used to determine the number of arcs; $^{(2)}$~arc length-to-width ratio thresholds; $^{(3)}$~redshift distribution and number count function, as introduced in Figs.~\ref{fig:zd} and~\ref{fig:cc}. \\ Values with and without brackets correspond to $S_{850~\mu{\rm m}} /S_{1.4~{\rm GHz}}=100$ and~$50$, respectively. \end{table}