\begin{table}%t1 \caption{\label{t:lines}Observed molecular lines.} \small \begin{tabular}{ll@{\ }r@{\ }l@{\ }ll c r@{\ }l r@{\ }l c r@{\ }l cc} \hline \hline \noalign{\smallskip} Molecule &\multicolumn{4}{c}{Transition} & Frequency &$E_{\rm up}$& \multicolumn{5}{c}{Peak position (mpc)$^{(d)}$} & \multicolumn{2}{c}{$\int T_{\rm mb}{\rm d}v${}$^{(e)}$} & \multicolumn{2}{c}{\nmb\ (\scm)$^{(g)}$} \\ & & & & & (MHz) & (K) & \multicolumn{2}{c}{NE slice} & \multicolumn{2}{c}{SW slice} & model & \multicolumn{2}{c}{(\kkms)} & $n=10^5$~\ccm & LTE \\ \noalign{\smallskip} \hline \noalign{\smallskip} \cch &$N_J$ &=& $4_{7/2}$&$\to$ $3_{5/2}$ &349400.5$^{(a)}$ &42 & --14 & $\pm$ 1.8 & --23 & $\pm$ 1.0 & --16 & 10.2 & $\pm$ 1.9 & \pow{5.5}{14} & \pow{2.7}{14} \\ \cch &$N_J$ &=& $4_{9/2}$&$\to$ $3_{7/2}$ &349337.8$^{(b)}$ &42 & --14 & $\pm$ 1.5 & --23 & $\pm$ 1.6 & --16 & 13.5 & $\pm$ 2.4 & \pow{6.4}{14} & \pow{2.9}{14} \\ o-\hhco &$J_{KpKo}$ &=& $5_{15}$ &$\to$ $4_{14}$ &351768.6 &62 & --3 & $\pm$ 1.3 & --7 & $\pm$ 1.9 & --12 & 11.1 & $\pm$ 1.9 & \pow{9.7}{14} & \pow{4.3}{13} \\ SO &$N_J$ &=& $8_9$ &$\to$ $7_8$ &346528.5 &79 & --2 & $\pm$ 1.4 & --5 & $\pm$ 1.0 & 8 & 6.1 & $\pm$ 1.1 & \pow{1.5}{15} & \pow{7.7}{13} \\ \eico &$J$ &=& 2 &$\to$ 1 &219560.4 &16 & 0 & $\pm$ 1.2 & 0 & $\pm$ 1.4 & 0 & 95.2 &$\pm$ 16 & \pow{1.5}{16} & \pow{1.8}{16} \\ HCN &$J$ &=& 3 &$\to$ 2 &265886.2$^{(c)}$ &26 & 3 & $\pm$ 2.5 & --1 & $\pm$ 1.8 & 8 & 420 &$\pm$ 78 & \pow{8.1}{15} & \pow{4.4}{14} \\ \thco &$J$ &=& 3 &$\to$ 2 &330588.0 &32 & 4 & $\pm$ 1.9 & --1 & $\pm$ 3.0 & 2 & 132 &$\pm$ 22 & $>$\pow{2.1}{16}$^{(f)}$ & $>$\pow{2.5}{16}$^{(f)}$ \\ \hline \end{tabular} $^{(a)}$ Blend of $F=4$--3 and $F=3$--2 hyperfine components (separation 1.4~MHz). $^{(b)}$ Blend of $F=5$--4 and $F=4$--3 hyperfine components (separation 1.3~MHz). $^{(c)}$ Blend of $F=3$--3, $F=3$--2 and $F=2$--1 hyperfine components (total separation 1.5~MHz). $^{(d)}$ Fitted position of the emission peak along the slice through the northeast and southwest cores (see Fig.~\ref{fig:images}), and the modeled slice (Fig.~\ref{fig:model}, bottom panel), all relative to the \eico\ peak. $^{(e)}$ Fitted value of integrated intensity at peak position along the northeast slice (see Fig.~\ref{fig:images}); uncertainties include fitting uncertainty and 15\% absolute calibration uncertainty. $^{(f)}$ Column density uncertain due to high optical depth; values listed here are lower limits. $^{(g)}$ Beam-averaged column densities for $n=10^5$~\ccm\ and in LTE, both at $T=85$~K. \end{table}