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Table 3:

Properties of the 1.3 mm continuum sources detected in the high-resolution PdBI maps.
Source Position (1.3 mm) Peak flux FWHM1 Flux density2 Separation3
  $\alpha$ (J2000) $\delta$ (J2000) (mJy/beam) (arcsec) (mJy) (AU)
L1448-C 03:25:38.87 30:44:05.3 59 $\pm $ 0.9 0.9 $\pm $ 0.05 57 $\pm $ 2 -
L1448-C / South1 03:25:38.95 30:44:03.2 11 $\pm $ 0.7 0.7 $\pm $ 0.1 11 $\pm $ 2 600
NGC 1333-IRS2A 03:28:55.56 31:14:37.1 26 $\pm $ 1.16 0.55 $\pm $ 0.07 18 $\pm $ 2 -
NGC 1333-IRS2A / SE 03:28:56.00 31:14:33.1 7 $\pm $ 1.16 0.23 $\pm $ 0.04 4 $\pm $ 1.5 1900
IRAM 04191 04:21:56.90 15:29:46.1 2 $\pm $ 0.37 0.28 $\pm $ 0.02 0.9 $\pm $ 0.4 -
L1527 04:39:53.87 26:03:09.8 50 $\pm $ 1.2 0.42 $\pm $ 0.05 65 $\pm $ 3 -
L1521-F 04:28:38.94 26:51:35.2 1 $\pm $ 0.12 0.65 $\pm $ 0.009 0.8 $\pm $ 0.2 -

Notes. (1) FWHM diameter is computed from a circular Gaussian fit to the visibilities.
(2) Flux integrated above the 3$\sigma $ level.
(3) Projected distance to the primary source.


Source LaTeX | All tables | In the text

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