\begin{table}%t6
\caption{\textbf{(d)} Squared visibilitiess of Achernar in the $H$~band from VINCI, equipped with
the IONIC integrated optics beam combiner.
 \label{vinci_achernar2}}
 \small%\centering
\par
\begin{tabular}{cccrrr}
\hline\hline
\noalign{\smallskip}
JD$_0$ & Cal. & Stations & $B$~(m) & Az. & $V^2$ (\%)\\
\hline
475.861 & $\alpha$~Ind & E0-G1 & 52.48 & 126.0 & $ 70.8 _{ \pm 4.3 \pm 1.6 } $ \\
475.870 & $\alpha$~Ind & E0-G1 & 53.39 & 127.8 & $ 71.1 _{ \pm 4.8 \pm 1.6 } $ \\
477.781 & $\alpha$~Ind & E0-G1 & 42.26 & 109.7 & $ 78.7 _{ \pm 3.9 \pm 1.7 } $ \\
477.785 & $\alpha$~Ind & E0-G1 & 42.98 & 110.7 & $ 77.4 _{ \pm 3.7 \pm 1.7 } $ \\
479.941 & $\alpha$~Ind & E0-G1 & 59.78 & 146.1 & $ 65.3 _{ \pm 5.2 \pm 1.4 } $ \\
479.944 & $\alpha$~Ind & E0-G1 & 59.95 & 146.8 & $ 66.0 _{ \pm 5.4 \pm 1.4 } $ \\
479.949 & $\alpha$~Ind & E0-G1 & 60.19 & 147.9 & $ 65.3 _{ \pm 5.1 \pm 1.4 } $ \\
482.791 & $\alpha$~Ind & E0-G1 & 45.98 & 115.0 & $ 76.6 _{ \pm 7.3 \pm 1.7 } $ \\
482.824 & $\alpha$~Ind & E0-G1 & 50.39 & 122.1 & $ 72.5 _{ \pm 7.0 \pm 1.6 } $ \\
482.827 & $\alpha$~Ind & E0-G1 & 50.80 & 122.8 & $ 78.4 _{ \pm 7.1 \pm 1.8 } $ \\
483.718 & $\alpha$~Ind & E0-G1 & 34.05 & 98.7 & $ 82.0 _{ \pm 4.4 \pm 1.8 } $ \\
483.722 & $\alpha$~Ind & E0-G1 & 34.83 & 99.7 & $ 77.5 _{ \pm 4.1 \pm 1.7 } $ \\
483.727 & $\alpha$~Ind & E0-G1 & 35.78 & 101.0 & $ 80.1 _{ \pm 4.6 \pm 1.7 } $ \\
483.831 & $\alpha$~Ind & E0-G1 & 51.56 & 124.2 & $ 71.9 _{ \pm 7.2 \pm 1.7 } $ \\
483.835 & $\alpha$~Ind & E0-G1 & 52.05 & 125.1 & $ 70.9 _{ \pm 3.8 \pm 1.7 } $ \\
483.839 & $\alpha$~Ind & E0-G1 & 52.51 & 126.0 & $ 72.0 _{ \pm 4.2 \pm 1.7 } $ \\
484.767 & $\alpha$~Ind & E0-G1 & 43.17 & 110.9 & $ 75.3 _{ \pm 6.4 \pm 1.4 } $ \\
484.771 & $\alpha$~Ind & E0-G1 & 43.72 & 111.7 & $ 79.3 _{ \pm 5.7 \pm 1.4 } $ \\
485.887 & $\chi$~Phe & E0-G1 & 57.36 & 137.5 & $ 72.3 _{ \pm 6.5 \pm 1.2 } $ \\
\hline
\end{tabular}
\end{table}