Table 3
Parameters of the millimeter-continuum sources.
| Core | RA | Dec | Fν, 3mm(a) | Fν,2mm(a) | θS (b) | D(c) | N (H2)(d) | Md(d) | n (H2)(d) | β (e) |
|---|---|---|---|---|---|---|---|---|---|---|
| h:m:s | ○:′:″ | Jy | Jy | ″ | pc | ×1021cm−2 | M⊙ | ×104 cm−3 | ||
| N | 05:37:41.55 | 36:07:31.9 | 3.0 × 10−4 | 8.3 × 10−4 | 2.4 | 0.18 | 5.7(1.2) | 2.9(1.5) | 1.1 | 0.34 |
| S | 05:37:42.31 | 36:07:15.2 | 1.4 × 10−4 | 3.9 × 10−4 | 2.0 | 0.15 | 2.1(0.5) | 0.7(0.4) | 0.5 | 0.21 |
Notes. (a)’Flux density integrated in the 3σ rms level.(b)Deconvolved angular diameter.(c)Deconvolved linear diameter.(d)H2 mass computed from the dust thermal continuum emission as described in Sect. 4.2, assuming a dust temperature equal to the excitation temperature of CH3OH (Table 5) and a dust mass opacity coefficient β = 1.7.(e)Dust opacity index computed comparing the integrated flux densities at the two frequencies observed as described in Sect. 4.2.
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