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Table 3

PILS-Cygnus continuum source properties.

Source Beam size ″×″ S850 µm (Jy beam−1) rms (Jy beam−1) Mbeam (M) Dust opacity (τ) Lbol (L)(a) RT=100 K (AU)(a)
N30-MM1 1.45 × 1.31 1.29 0.014 7.25 0.31 2500
S26 1.46 × 1.31 0.60 0.004 23.98 1.02 7000
N12-MM2 1.43 × 1.27 0.50 0.003 3.20 0.14 400
N63 1.37 × 1.10 1.66 0.005 10.83 0.58 300
N53-MM2 1.44 × 1.28 0.41 0.004 2.92 0.13 400 ± 200 300
N54 1.42 × 1.24 0.27 0.010 2.02 0.09 160 200
N51 1.47 × 1.22 0.42 0.009 2.70 0.12 1300 ± 200 600
N38 1.45 × 1.25 0.62 0.009 3.59 0.16 300 300
N48-MM1 1.56 × 1.37 0.25 0.004 1.87 0.07 2000 ± 700 700
S8-NE core 1.54 × 1.31 0.30 0.005 1.89 0.08 1200

Notes. (a)We use Lbol values from Pitts et al. (2022), with the values for N38 and N54 from San José-García (2015) and Kryukova et al. (2014) respectively. The 100 K is the radius at which the temperature rises above 100 K ( cm; Bisschop et al. 2007). With a beam size of ~1″.5, or ~5000 AU for S26, and ~2000 AU for all other sources, it implies that the 100 K radius is resolved for only N30 and S26.

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