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Table 4.

0.87 mm integrated flux densities, source sizes, polarization intensities, and fractions.

Name On the 0.87 mm reconstructed maps
From the visibility amplitude curve
Flux densitya Mass Peak intensity Peak Pib pfracc 0.87 mm flux density

(Jy) (M) (Jy/beam) (mJy/beam) (%) (Jy)
B335 0.21±0.04 0.02 0.24 25.3 10.5 0.51±0.05
SVS13 1.40±0.28 0.29 1.06 14.8 2.5 1.54±0.15d
HH797 0.47±0.09 0.10 0.71 5.7 3.0 0.94±0.09
L1448C 0.57±0.11 0.11 0.65 12.5 1.00±0.01
L1448N 1.50±0.30 0.31 1.34 20.3 2.7 1.93±0.19d
L1448-2A 0.34±0.07 0.07 0.27 5.7 0.48±0.05
IRAS03282 0.44±0.09 0.09 0.65 9.9 1.17±0.12
NGC 1333 IRAS4A 2.38±0.48 0.50 2.57 77.3 8.8 6.79±0.68
NGC 1333 IRAS4B 1.42±0.28 0.30 2.89 14.9 4.7 4.10±0.41
IRAS16293 4.81±0.96 0.26 3.83 39.2 1.7 5.96±0.60d
L1157 0.43±0.09 0.10 0.71 31.4 4.5 1.07±0.11
CB230 0.22±0.04 0.09 0.37 14.3 6.4 0.58±0.06

Notes.

(a)

Flux density estimated within the central 6000 au for SVS13, 3000 au for other sources.

(b)

Not all the sources have an intensity peak co-spatial with the polarized intensity peak.

(c)

Polarization fraction defined as the unweighted ratio of the median polarization to total flux.

(d)

The visibility data allows us to separate the two components of wide binaries. The fluxes are those of the object located at the phase center, e.g., L1448N-B, SVS13-B and IRAS16293-A.

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