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Table 3:

Results of elliptical Gaussian and point source fits to the continuum visibilities for the Class I sources.
Source Position Sizea, FWHM Flux (density)
  RA Dec $\theta_{1.1{\rm ~mm}}$ $F_{\rm 1.1~mm}$b $S_{\rm 850~\mu{\rm m}}$(15 $\hbox {$^{\prime \prime }$ }$)c
  (J2000.0) (J2000.0) [ $\hbox {$^{\prime \prime }$ }$] [mJy] [mJy beam-1]
TMR1 04 39 13.91 +25 53 20.63 $\ldots$d 79d 480
TMC1A 04 39 35.20 +25 41 44.35 0.69 $\times$ 0.40 256 (246) 780
TMC1A-2 04 39 34.80 +25 41 43.87 3.7 $\times$ 1.1 48 (26) $\ldots$
IRS 43 16 27 26.91 -24 40 50.62 1.9 $\times$ 0.13 75 (56) 990
IRS 54 16 27 51.80d -24 31 45.4d $\ldots$ $\ldots$ $\ldots$
IRS 63 16 31 35.65 -24 01 29.55 0.63 $\times$ 0.0096 473 (459) 1220
GSS30-IRS3 16 26 21.71 -24 22 50.63 1.4 $\times$ 1.3 204 (144) 990
WL 12 16 26 44.19 -24 34 48.74 1.9 $\times$ 1.5 104 (64) 360
Elias 29 16 27 09.44 -24 37 19.99 5.8 $\times$ 1.8 109 (48) 590

a Deconvolved size from Gaussian fit. b Flux density from Gaussian fit to SMA data in the (u,v)-plane. Number in parentheses from point source fit. cPeak flux at 850 $\mu $m in JCMT 15 $\hbox {$^{\prime \prime }$ }$single-dish beam. dTMR1 unresolved in SMA observations. Only result from point source fit listed. e IRS 54 undetected at the SMA; position from Spitzer Space Telescope observations.

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