\begin{table}%t3
\par
%\centering
\par
\caption{\label{tbl:lines}Atomic parameters of spectral lines employed in magnetic inversions.}
\begin{tabular}{llrlcccc}
\hline\hline
\noalign{\smallskip}
Ion &~~~$\lambda$ (\AA) & $E_{\rm lo}$ (ev) &~~$\log gf$ & $J_{\rm lo}$ & $J_{\rm up}$ & $g_{\rm lo}$ & $g_{\rm up}$ \\
\noalign{\smallskip}
\hline
\ion{Cr}{ii} & 4824.127\tablefootmark{a} &  3.871 & $-0.970$ & 4.5 & 4.5 & 1.34 & 1.34 \\
\ion{Fe}{ii} & 4824.198           & 10.288 & $-1.215$ & 4.5 & 4.5 & 1.45 & 1.22 \\
\ion{Fe}{ii} & 4824.838           &  8.145 & $-1.893$ & 4.5 & 3.5 & 1.25 & 1.24 \\
\ion{Fe}{ii} & 4923.927           &  2.891 & $-1.320$ & 2.5 & 1.5 & 2.00 & 2.40 \\
\ion{Fe}{ii} & 5018.440\tablefootmark{a} &  2.891 & $-1.271$\tablefootmark{b} & 2.5 & 2.5 & 2.00 & 1.87 \\
\ion{Fe}{ii} & 5019.462           &  5.569 & $-2.697$ & 3.5 & 4.5 & 1.14 & 1.10 \\
\hline
\end{tabular}
\tablefoot{The columns specify the ion, the central wavelength $\lambda$,
excitation potential of the lower atomic level $E_{\rm lo}$, quantum numbers $J$ and Land\'e factors
$g$ for both the lower and upper levels.\\
\tablefoottext{a}{Dominant blend components.}
\tablefoottext{b}{Oscillator strength is adjusted in the MDI inversion.}}
\end{table}