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Table 4:

Envelope and disk masses for the full sample of Class 0 and I sources.
Source $M_{\rm env}$a $M_{\rm disk}$b $M_{\rm star}$c
  [$M_\odot $] [$M_\odot $] [$M_\odot $]
Class 0
L1448-mm 0.96 0.044 $\ldots$
IRAS2A 1.0 0.056 $\ldots$
IRAS4A1 4.5d 0.46 $\ldots$
IRAS4A2 -d 0.25 $\ldots$
IRAS4B 2.9d 0.24 $\ldots$
IRAS4B' -d 0.089 $\ldots$
L1527 0.56 0.029 $\ldots$
L483 0.82 0.0e $\ldots$
B335 0.93 0.017 $\ldots$
L1157 0.94 0.12 $\ldots$
Class I
L1489-IRS 0.11 0.018 1.3f
TMR1 0.11 0.0094 $\ldots$
TMC1A 0.12 0.035 0.35-0.7g
GSS30-IRS3 0.096 0.026 $\ldots$
WL 12 0.054 0.011 $\ldots$
Elias 29 0.047 0.011 2.5h
IRS 43 0.026 0.0081 1.0i
IRS 54j $\ldots$ <0.001 $\ldots$
IRS 63 0.098 0.053 0.36h

a Envelope mass determined from the direct scaling of the JCMT peak flux (minus the disk contribution). b Disk mass assuming a uniform dust temperature of 30 K. c Central mass from Keplerian velocity profiles (see specific references for details). dIRAS4A1 and IRAS4A2, respectively IRAS4B and IRAS4B' have larger scale circumbinary envelopes. e The compact flux in L483 is consistent with being solely from the larger scale envelope. f Stellar mass from Brinch et al. (2007), envelope and disk masses calculated under same assumptions as for the remainder of the sources using the continuum data from Brinch et al. g Brown & Chandler (1999). h Lommen et al. (2008), i This work. j IRS 54 is undetected in both interferometric and single-dish maps. A 3$\sigma $ upper limit to its disk mass is estimated from the SMA observations.

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