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Table 1.

Summary of the molecular line observations.

Center line Resolution Coverage Int. time τave Tsys Feff/Beff rms_ave
(km s−1) (MHz) (min) (K) (mK)
12CO(2–1) 0.25 225060–232840 261 0.10 230 1.56 20–15–50
12CO(2–1) 0.063 226398–228200, 229670–231497 105 0.18 230 1.56 50
13CO(2–1) 0.20 214920–222700 209 0.10 170 1.53 10
C18O(2–1)a 0.067 215420–217240, 218700–220520 160 0.16 220 1.52 50
C18O(2–1) 0.20 214080–221860 313 0.09 220 1.52 10–20
HCO+(1–0) 0.66 83710–91490 261 0.03 120 1.18 6–20
HCO+(1–0) 0.16 85050–86870, 88330–90148 110 0.03 120 1.18 30
N2H+(1–0) 0.63 87680–97475 313 0.03 110 1.18 10
N2H+(1–0) 0.157 89033–90860, 92315–94133 157 0.03 110 1.18 10
CS(2–1)b 0.60 92500–100280 209 0.02 80 1.19 7

Notes. To maximize the S/N in the lines of the low-resolution spectra, we combined them with the high-resolution data. The rms listed is thus the rms of the combined spectrum. (a)The setup also covers the 13CO line. (b) Only low-resolution data. All observations were obtained on 2014 March 5–6. We include the average sky opacity (τave) during the observations, the average system temperature, the ratio between forward efficiency and beam efficiency (Feff /Beff; Kramer et al. 2013), and the average rms for each configuration.

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