Table 1
IRAS 4A: envelope continuum emission at 880 μm and derived parametersa.
α(J2000)b | 3h29m10.520s |
δ(J2000)b |
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Tdustc | 50 K |
|
|
rmsI | 20 mJy beam-1 |
rmsQ | 2.5 mJy beam-1 |
rmsU | 2.5 mJy beam-1 |
|
|
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4.1 ± 0.4 Jy |
![]() |
1.03 ± 0.02 Jy beam-1 |
FWHMd | 1156 AU (![]() |
|
|
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160 ± 16 mJy |
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38.2 ± 2.5 mJy beam-1 |
Ωpole | 14 arcsec2 |
|
|
τ | 0.07 |
NH2f | 1.2 × 1024 cm-2 |
nH2f | 1.1 × 108 cm-3 |
Massf | 0.8 M⊙ |
Notes.
See Appendix A of Frau et al. (2010) for details.
Diameter of the circle with the same area as the region of the source with intensity above half of the peak.
Assuming κ250 GHz = 1.5 cm2 g-1 and a gas-to-dust ratio of 100 (Girart et al. 2006).
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