Table 1
878 μm continuum emission parameters.
| α(J2000) | δ(J2000) |
|
S ν | ⌀Peak / 2 b | T dust a | N H2 c | n H2 c | Massc | |
| Source | h:m:s | °:′:′′ | (Jy beam-1) | (Jy) | (103 AU) | (K) | (1023 cm-2) | (106 cm-3) | (M⊙) |
|
|
|||||||||
| MM1 | 23:13:45.349 | 61:28:10.47 | 5.24 | 6.07 ± 0.05 | 4.93 | 245 | 14 | 23 | 17 |
| MM2 | 23:13:44.698 | 61:28:12.30 | 0.563 | 1.87 ± 0.08 | 9.38 | 40 | 8.4 | 7.5 | 37 |
| MM3 | 23:13:46.397 | 61:28:14.05 | 0.358 | 0.52 ± 0.05 | 6.04 | 40 | 5.6 | 7.8 | 10 |
| MM3b | 23:13:45.976 | 61:28:13.52 | 0.214 | 0.57 ± 0.06 | 9.54 | 40 | 2.5 | 2.2 | 11 |
| MM4 | 23:13:43.774 | 61:28:11.74 | 0.419 | 1.30 ± 0.06 | 8.36 | 40 | 7.4 | 7.4 | 26 |
| MM5 | 23:13:45.207 | 61:28:16.83 | 0.149 | 0.18 ± 0.04 | 6.28 | 40 | 1.8 | 2.4 | 3.5 |
| MM6 | 23:13:46.849 | 61:28:10.12 | 0.251 | 0.39 ± 0.05 | 6.75 | 43 | 3.1 | 3.8 | 7.0 |
| MM7 | 23:13:45.140 | 61:27:58.44 | 0.404 | 0.97 ± 0.07 | 7.60 | 58 | 4.3 | 4.7 | 12 |
| MM7b | 23:13:44.622 | 61:27:58.30 | 0.224 | 0.37 ± 0.05 | 6.75 | 58 | 2.1 | 2.6 | 4.7 |
| MM9 | 23:13:43.770 | 61:28:02.32 | 0.153 | 0.31 ± 0.05 | 8.36 | 54 | 1.2 | 1.2 | 4.2 |
| MM10 | 23:13:46.439 | 61:28:05.30 | 0.229 | 0.36 ± 0.05 | 6.52 | 43 | 3.1 | 3.9 | 6.5 |
| MM11 | 23:13:44.421 | 61:28:25.76 | 0.194 | 0.50 ± 0.05 | 8.17 | 40 | 2.9 | 3.0 | 9.6 |
| MM12 | 23:13:46.019 | 61:28:01.47 | 0.137 | 0.32 ± 0.04 | 9.54 | 43 | 1.3 | 1.1 | 5.6 |
| MM13 | 23:13:45.092 | 61:28:26.36 | 0.105 | 0.18 ± 0.04 | 8.71 | 40 | 0.94 | 0.90 | 3.5 |
Notes.
For the sources detected by QZM11 we use the temperature they use. For the rest of the sources we adopt 40 K.
Assuming κ341.4 GHz = 0.015 cm2 g-1 (Ossenkopf & Henning 1994). See Appendix 1 in Frau et al. (2010) for details on the calculation. The uncertainties are approximately 50% of the computed values.
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