Table 5
IRAM 30 m data.
| Core | Transition | RA (J2000) | Dec (J2000) | I | dI | rms |
| (h:m:s) | (°:′:′′) | (K km s-1) | (K km s-1) | (K) | ||
| (1) | (2) | (3) | (4) | (5) | (6) | (7) |
|
|
||||||
| C1-N | 13CO (2−1) | 18:42:46.95 | −4:04:08.5 | 11.80 | 0.06 | 0.02 |
| F1 | 13CO (2−1) | 18:53:16.46 | 1:26:09.9 | 22.85 | 0.08 | 0.02 |
| F2 | 13CO (2−1) | 18:53:19.06 | 1:26:52.6 | 23.39 | 0.07 | 0.02 |
| C1-N | C18O (2−1) | 18:42:46.95 | −4:04:08.5 | 5.92 | 0.08 | 0.03 |
| F1 | C18O (2−1) | 18:53:16.46 | 1:26:09.9 | 6.16 | 0.05 | 0.02 |
| F2 | C18O (2−1) | 18:53:19.06 | 1:26:52.6 | 6.03 | 0.05 | 0.02 |
Notes. Column 1 gives the name of the core observed while Col. 2 gives the transition observed. Columns 3 and 4 are the right ascension and declination, respectively, of the observation. The sum of the integrated intensities of all detected components is given in Col. 5. The uncertainty in this total integrated intensity is calculated as the sum of the uncertainties of the individual components and is given in Col. 6. The rms of the baseline is given in Col. 7.
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