Table 2
Properties of SABOCA sources.
| RA | Dec | F | θ | Δv | M F | M V | |
| Jy | ′′ | km s-1 | M ⊙ | M ⊙ | |||
|
|
|||||||
| Sa | 11:15:12.07 | –61:16:58.8 | 90 | 9.2 | 2.5 | 498 | 122 |
| S8 | 11:15:02.88 | –61:15:51.5 | 55 | 6.7 | − | 307 | − |
| Sc | 11:15:08.41 | –61:16:57.2 | 67 | 8.2 | 3.2 | 369 | 180 |
| S9 | 11:15:11.34 | –61:16:45.2 | 59 | 7.6 | 2.5 | 329 | 102 |
| Se | 11:15:13.73 | –61:17:24.3 | 46 | 8.5 | 2.5 | 258 | 114 |
| Sf | 11:15:11.25 | –61:17:12.0 | 45 | 9.6 | − | 249 | − |
| Sg | 11:15:10.33 | –61:16:16.4 | 22 | 4.9 | − | 122 | − |
Notes. The sources labeled S8 and S9 in the first column are the same as listed in Table 1 of Lebouteiller et al. (2008). Source S9 is associated with IRS 9A. The source size θ in Col. 5 is the geometric mean of the axes of the deconvolved size. At the distance of IRS 9A, 10′′ correspond to 0.33 pc. The data in the last three columns are described in Sect. 3.3.
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