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Table 3:

Derived values from the stacked flux densitiesa.
Sample N z $F_{\rm 1.2~mm}$ $F_{\rm {20~cm}}$ $F_{\rm 1.2~mm}$/ $F_{\rm 24~\mu m}$ $L_{\rm {1.4~GHz}}$ $L_{\rm {FIR,mm}}$c $L_{\rm {FIR,radio}}$ SFR $_{\rm {mm}}$ SFR $_{\rm {radio}}$ q
      (mJy) ($\mu $Jy)   (1024 W Hz-1) (1012 $L_{\odot}$) ($M_{\odot }$ yr-1)  
All 33 2.08 1.56 $\pm $ 0.22 92.6 $\pm $ 12.0 2.76 $\pm $ 0.50 2.03 $\pm $ 0.26 2.45 $\pm $ 0.35 4.14 $\pm $ 0.53 441 745 2.11 $\pm $ 0.12
S/N > 3b 13 2.11 2.83 $\pm $ 0.14 128.5 $\pm $ 26.0 4.94 $\pm $ 0.51 2.89 $\pm $ 0.58 3.99 $\pm $ 0.20 5.90 $\pm $ 1.18 718 1062 2.17 $\pm $ 0.11
S/N < 3b 20 2.06 0.72 $\pm $ 0.18 69.3 $\pm $ 7.4 1.28 $\pm $ 0.40 1.48 $\pm $ 0.16 1.38 $\pm $ 0.35 3.02 $\pm $ 0.32 248 543 2.00 $\pm $ 0.16

a The average stacked flux densities are computed with equal weights to avoid biases. Their approximate rms are computed as the standard deviation of the mean.
b S/N at 1.2 mm.
c $L_{\rm {FIR,mm}}$ is computed with (Eq. (3)) and the dust temperatures coming from the stacked SED (see text): 37 K for the entire sample, 36 K for the 13 sources with S/N > 3 at 1.2 mm, and 39 K for the 20 sources with S/N < 3.

Source LaTeX | All tables | In the text

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