\begin{table}%tB.1 \caption{\label{Odin table}Observed transitions and their parameters$^{{a}}$ in S140 with the Odin satellite in a five point NE-SW strip.} \small%\centerline { { \begin{tabular}{ l l l l l l l r r r rl} \hline \hline %&&&&&&&&&&& \\[-8pt] Species & Transition & Freq & $E_{\rm u}$ &$A$-coeff & $\Delta \upsilon$& Pos. & $\upsilon_{{\rm LSR}}$ & $T_{\rm peak}$ & $\int$ $T^{~*}_{{\rm A}}$ d$\upsilon$ &rms ¬e \\ & & [GHz] & [K] & [s$^{-1}$] &[kms$^{-1}$] &&[kms$^{-1}$]& [mK] & [K kms$^{-1}$]&[mK] &\\ \hline H$_2$O & 1$_{1,0}$--1$_{0,1}$& 556.936&61.0&3.46e-3 &0.27 & 1 &--8.0 & 207 & 0.64&39& \\ &&&&&&2& --6.9 & 517 & 2.74&68&\\ &&&&&&3& --6.6 & 632 &3.34 &19&\\ &&&&&&4& --7.0 & 379 &1.84 &57&\\ &&&&&&5& -- &-- & -- & 44& No detection. \\ H$_2^{18}$O & 1$_{1,0}$--1$_{0,1}$& 547.676 &60.5 &3.29e-3&0.34&3&-- &-- &-- &$\sim$8 & No detection.\\ CO & 5--4& 576.258 &83.0 &1.22e-5&0.32&1&--5.4 &6680& 47.1&67 & \\ &&&&&&2& --5.0 &11~760 &94.2 &47&\\ &&&&&&3& --5.5 & 13~240 &108.8 &43&\\ &&&&&&4& --6.6 & 8690 & 60.1 &50&\\ &&&&&&5& --6.9 & 2220 & 10.1 &160&\\ $^{13}$CO & 5--4& 550.926 &79.3 &1.10e-5&0.27&1& --7.8 & 2~740& 8.29 &115& \\ &&&&&&2& --7.4 & 5930 & 21.4&81&\\ &&&&&&3& --7.4 & 7110 & 27.7&61&\\ &&&&&&4& --7.6 & 3640 & 13.2&119&\\ &&&&&&5& --8.5 & 1190 &2.5&291&\\ NH$_3$ & 1$_{0}$--0$_{0}$& 572.498 &27.5& 1.61e-3&0.32&1& --8.0 & 444 & 1.18&99& \\ &&&&&&2& --7.4 & 467 & 1.83 &33&\\ &&&&&&3& --7.4 & 588 & 2.66 &29&\\ &&&&&&4& --7.3 & 381 & 1.86 &36&\\ &&&&&&5& -- & -- &-- &91&No detection\\ \hline \end{tabular}}} \medskip $^{{a}}$ Transition = the quantum numbers for the transition; Freq~= rest frequency of the transition; $E_{\rm u}$~= the upper state energy; $A$-coeff~= the Einstein $A$-coefficient; $\Delta \upsilon$~= the velocity resolution; Pos~= the strip position from NE to SW. $\upsilon_{\rm LSR}$~= the peak LSR~velocity; $T_{\rm peak}$~= the observed peak temperature of the transition; $\int$~$T^{~*}_{{\rm A}}$~d$\upsilon$~= the integrated intensity from the observed spectra not corrected for beam-efficiency or beam-filling; rms~=~noise. \end{table}