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Table 7:

Properties of the ATLASGAL sources with a counterpart in the mid-infrared emission, derived by fitting the 870 and 70 $\mu $m points with a modified black body.

Source
Radius da $F_{24~\mu{\rm m}}$ $F_{70~\mu {\rm m}}$ Td L M $\Sigma $
  (pc) (kpc) (Jy) (Jy) (K) ($\times$ $10^4~L_{\odot}$) ($\times$ $10^2~M_{\odot}$) (g cm-2)
(1) (2) (3) (4) (5) (6) (7) (8) (9)
C2 0.7 12.6 7.6 $\pm$ 1.5 119.8 $\pm$ 24.0 25 5 60 0.81
C3 0.7 12.6 4.0 $\pm$ 0.8 68.8 $\pm$ 13.8 25 3 30 0.41
C4 0.7 12.6 2.1 $\pm$ 0.4 42.8 $\pm$ 8.6 27 2 10 0.14
C5 0.7 12.6 3.8 $\pm$ 0.8 29.0 $\pm$ 5.8 26 1 10 0.14
C7 0.7 11.7 9.1 $\pm$ 1.8 107.3 $\pm$ 21.5 28 3 20 0.27
C8 0.7 11.7 7.2 $\pm$ 1.4 94.2 $\pm$ 18.8 33 2 6 0.08
C10 0.7 11.7 - 100.6 $\pm$ 20.1 29 3 10 0.14
C11 0.7 11.7 6.8 $\pm$ 1.4 51.4 $\pm$ 10.3 28 2 9 0.12
C13 0.6 11.7 2.6 $\pm$ 0.5 72.0 $\pm$ 14.4 32 1 4 0.07
C14 0.5 4.7 5.1 $\pm$ 1.0 17.8 $\pm$ 3.6 20 0.3 9 0.24

Notes. Column (1): ATLASGAL continuum source; Col. (2): radius of the APEX continuum source; Col. (3): distance of the source; Col. (4): flux density at 24 $\mu $m of the IR source associated with the ATLASGAL 870 $\mu $m source; Col. (5): flux density at 70 $\mu $m of the IR source associated with the ATLASGAL 870 $\mu $m source; Col. (6)-(8): output of the modified black body fit. In particular: the dust temperature; the luminosity; the mass; and the surface density. (a) All the sources are assumed to be at the far kinematic distances, except C14.


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