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Table 1:

Integrated line intensities, $\int
T_{\rm MB}\ {\rm d}\varv$ (K km s-1) over the central 22 $.\!\!^{\prime\prime}$$\times $ 22 $.\!\!^{\prime\prime}$5 of each sourcea and emission-weighted, average line-widths.

Transition
$\nu$ (GHz)b $E_{\rm up}$ (K)b SMM1 SMM3 SMM4 S68N SMM1-S SMM4-W SMM4-S
+0E 338.1245 78.1 0.25 0.22 0.30 0.85 ... 0.09 0.41
-1E 338.3446 70.5 0.58 0.45 1.09 2.90 0.52 0.90 1.38
+0A 338.4087 65.0 0.71 0.62 1.35 3.66 1.06 1.26 2.21
-2A 338.5129 102.7 0.06 0.01 ... 0.24 0.08 0.20 ...
$\pm $3Ac 338.5420 114.8 0.11 0.16 0.15 0.40 ... ... ...
+1E 338.6150 86.1 0.16 0.08 0.18 0.45 ... 0.34 ...
+2A 338.6399 102.7 0.09 0.07 ... 0.26 ... ... ...
$\pm $2Ec 338.7223 89.1 0.21 0.16 0.28 1.05 ... 0.13 0.11
$\Delta\varv$(km s-1)     $3.4 \pm 0.9$ $4.4 \pm 2.5$ $4.0 \pm 0.7$ $7.2 \pm 1.3$ $4.3 \pm 0.9$ $4.0 \pm 0.3$ $4.1 \pm 0.3$

Notes. (a) Non-detections are marked by ``...'', for which an upper limit of 0.03 K km s-1 applies. (b) Frequencies and upper level energies are from the Cologne Database for Molecular Spectroscopy (CDMS; Müller et al. 2001). (c) Lines are blended. The frequencies and upper level energies are average values.


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