\begin{table}%t5 %\centering \par \caption{\label{table:test5}Results of the photometric inversion of simulated Eros-like shaped asteroids on different asteroidal orbits.} \begin{tabular}{ccccccccc} \hline\hline Simulated & $N$ & \multicolumn{1}{c}{$\lambda$(pole)} & \multicolumn{1}{c}{$\beta$(pole)} & \multicolumn{1}{c}{Period} & $b/a$ & $c/a$ & $k$ & $\epsilon$\\ Orbit & & \multicolumn{1}{c}{(deg)} & \multicolumn{1}{c}{(deg)} & \multicolumn{1}{c}{(h)} & & & (mag/$^{\circ}$) & (mag) \\ \hline 15 & $85$ & $59.8\pm0.3$ & $54.0\pm0.7$ & $19.150029\pm0.000024$ & $0.24\pm0.02$ & $0.22\pm0.01$ & $0.018\pm0.001$ & $0.054$ \\ 24 & $84$ & $45.5\pm0.1$ & $44.1\pm0.2$ & $19.150292\pm0.000002$ & $0.28\pm0.01$ & $0.28\pm0.01$ & $0.022\pm0.001$ & $0.058$ \\ 311 & $62$ & $50.4\pm0.2$ & $53.0\pm0.1$ & $19.150183\pm0.000005$ & $0.41\pm0.00$ & $0.41\pm0.00$ & $0.026\pm0.000$ & $0.091$ \\ 319 & $64$ & $50.5\pm0.6$ & $47.2\pm0.2$ & $19.150310\pm0.000013$ & $0.42\pm0.01$ & $0.42\pm0.01$ & $0.021\pm0.000$ & $0.060$ \\ 320 & $48$ & $43.4\pm0.9$ & $42.7\pm1.4$ & $19.150424\pm0.000021$ & $0.34\pm0.03$ & $0.34\pm0.03$ & $0.024\pm0.001$ & $0.068$ \\ 326 & $97$ & $49.3\pm0.4$ & $50.4\pm0.7$ & $19.149266\pm0.000012$ & $0.40\pm0.01$ & $0.40\pm0.01$ & $0.025\pm0.000$ & $0.058$ \\ 363 & $44$ & $45.1\pm0.4$ & $54.0\pm0.3$ & $19.149646\pm0.000037$ & $0.41\pm0.00$ & $0.41\pm0.00$ & $0.021\pm0.001$ & $0.073$ \\ 391 & $81$ & $55.2\pm0.8$ & $51.4\pm0.2$ & $19.150162\pm0.000021$ & $0.47\pm0.00$ & $0.44\pm0.00$ & $0.022\pm0.000$ & $0.077$ \\ 433 & $88$ & $49.0\pm0.2$ & $53.4\pm0.3$ & $19.149835\pm0.000006$ & $0.43\pm0.00$ & $0.40\pm0.00$ & $0.024\pm0.000$ & $0.143$ \\ 472 & $62$ & $44.7\pm0.5$ & $52.0\pm0.3$ & $19.149876\pm0.000008$ & $0.43\pm0.00$ & $0.43\pm0.00$ & $0.023\pm0.000$ & $0.081$ \\ \hline \end{tabular} \begin{list}{}{} \item[Note:] $N$ is the number of simulated Gaia detections for each case. The spin parameters adopted to compute the simulated cases are: Pole $=(48.5^\circ, 51.0^\circ)$, Period $= 19.150000$~h. \end{list} \end{table}