\begin{table}%t2
\caption{Abundances and isotopic ratios implied by the weak (\mbox{$\Delta v = 1$}), LE (\mbox{$\Delta v = 1$}) and \mbox{$\Delta v = 2$} $^{12}$C$^{16}$O line lists as indicator of $^{12}$C abundance.  Note the large differences between 1D and 3D isotopic ratios.  Note also that the HM and \textsc{marcs} 1D models indicate higher abundances than the 1DAV, which in turn produces a higher abundance than the 3D model.}
\label{tableCO}
%\centering
\small
\begin{tabular}{l l c c c c c}
\hline \hline
% & & & & & & \\[-8pt]
$^{12}$C$^{16}$O Lines & Model & 3D & HM & \textsc{marcs} & 1DAV & Terrestrial\\
\hline
Weak & $\log \epsilon_{\rm C}$ & $8.40\pm0.01$ & $8.60\pm0.01$ & $8.55\pm0.02$ & $8.46\pm0.01$ & \\
($\Delta v = 1$) & $\log \epsilon_{^{12}{\rm C}}$ & $8.39\pm0.01$ & $8.59\pm0.01$ & $8.55\pm0.02$ & $8.45\pm0.01$ & \\
& $\log \epsilon_{^{13}{\rm C}}$ & $6.44 \pm 0.02$ & $6.76 \pm 0.02$ & $6.70 \pm 0.02$ & $6.58 \pm 0.02$ & \\
& $\log \epsilon_{^{18}{\rm O}}$ & $5.97 \pm 0.03$ & $6.31 \pm 0.04$ & $6.25 \pm 0.04$ & $6.12 \pm 0.03$ &  \\
& $^{12}$C/$^{13}$C & 88.8$^{+5.3}_{-5.0}$ & 68.6$^{+3.2}_{-3.0}$ & 70.6$^{+4.3}_{-4.1}$ & 74.0$^{+3.3}_{-3.2}$ & $89.4\pm 0.2$  \\
% & & & & & & \\[-8pt]
& $^{16}$O/$^{18}$O & 490$^{+41}_{-37}$ & 344$^{+30}_{-28}$ & 350$^{+35}_{-32}$ & 376$^{+31}_{-29}$ & $498.7\pm 0.1$  \\
% & & & & & & \\[-8pt]
\hline
LE & $\log \epsilon_{\rm C}$ & $8.48\pm0.04$ & $8.66\pm0.02$ & $8.67\pm0.03$ & $8.49\pm0.02$ & \\
($\Delta v = 1$) & $\log \epsilon_{^{12}{\rm C}}$ & $8.47\pm0.04$ & $8.66\pm0.02$ & $8.67\pm0.03$ & $8.49\pm0.02$ & \\
& $\log \epsilon_{^{13}{\rm C}}$ & $6.44 \pm 0.02$ & $6.76 \pm 0.02$ & $6.70 \pm 0.02$ & $6.58 \pm 0.02$ & \\
& $\log \epsilon_{^{18}{\rm O}}$ & $5.89 \pm 0.03$ & $6.24 \pm 0.04$ & $6.13 \pm 0.04$ & $6.09 \pm 0.03$ &  \\
& $^{12}$C/$^{13}$C & 107.6$^{+13}_{-12}$ & 80.3$^{+5.8}_{-5.4}$ & 93.2$^{+8.7}_{-7.9}$ & 80.0$^{+5.1}_{-4.8}$ & $89.4\pm 0.2$  \\
% & & & & & & \\[-8pt]
& $^{16}$O/$^{18}$O & 594$^{+80}_{-71}$ & 403$^{+42}_{-38}$ & 463$^{+57}_{-50}$ & 407$^{+39}_{-35}$ & $498.7\pm 0.1$  \\
 %& & & & & & \\[-8pt]
\hline
\mbox{$\Delta v = 2$} & $\log \epsilon_{\rm C}$ & $8.37\pm0.01$ & $8.69\pm0.02$ & $8.58\pm0.02$ & $8.51\pm0.02$ & \\
& $\log \epsilon_{^{12}{\rm C}}$ & $8.36\pm0.01$ & $8.68\pm0.02$ & $8.57\pm0.02$ & $8.50\pm0.02$ & \\
& $\log \epsilon_{^{13}{\rm C}}$ & $6.44 \pm 0.02$ & $6.76 \pm 0.02$ & $6.70 \pm 0.02$ & $6.58 \pm 0.02$ & \\
& $\log \epsilon_{^{18}{\rm O}}$ & $6.00 \pm 0.03$ & $6.22 \pm 0.04$ & $6.23 \pm 0.04$ & $6.07 \pm 0.03$ &  \\
& $^{12}$C/$^{13}$C & 82.8$^{+5.2}_{-4.9}$ & 83.9$^{+5.9}_{-5.5}$ & 75.0$^{+5.7}_{-5.3}$ & 82.8$^{+4.5}_{-4.3}$ & $89.4\pm 0.2$  \\
% & & & & & & \\[-8pt]
& $^{16}$O/$^{18}$O & 457$^{+39}_{-36}$ & 421$^{+43}_{-39}$ & 372$^{+41}_{-37}$ & 421$^{+38}_{-35}$ & $498.7\pm 0.1$  \\
\hline
\end{tabular}
\end{table}