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Table 4:

1.2 mm and radio data.
Source ID $F_{\rm 1.2~mm}$a $F_{\rm {20~cm}}$b $F_{\rm {50~cm}}$b $F_{\rm {90~cm}}$b Major axis Minor axis $\alpha$c q
  (mJy) ($\mu $Jy) ($\mu $Jy) ($\mu $Jy) ( $\hbox{$^{\prime\prime}$ }$) ( $\hbox{$^{\prime\prime}$ }$)    
1.2 mm detections S/N > 4
L-1 2.95 $\pm $ 0.66 76.3 $\pm $ 9.0 142 $\pm $ 19 327 $\pm $ 74 2.9 X -0.84 $\pm $ 0.18 2.49 +0.20-0.20

L-9
4.00 $\pm $ 0.55 116.5 $\pm $ 9.2 195 $\pm $ 22 266 $\pm $ 69 1.9 0.7 -0.54 $\pm $ 0.03 2.35 +0.20-0.20

L-11
3.08 $\pm $ 0.58 314.8 $\pm $ 4.1 425 $\pm $ 43 651 $\pm $ 72 X X -0.45 $\pm $ 0.06 2.06 +0.25-0.25

L-22
3.41 $\pm $ 0.73 100.9 $\pm $ 7.1 238 $\pm $ 26 447 $\pm $ 70 1.7 X -1.02 $\pm $ 0.01 2.00 +0.23-0.23
1.2  mm tentative detections ${\it S/N}>3$
L-5 2.75 $\pm $ 0.76 71.0 $\pm $ 20.0 177 $\pm $ 23 322 $\pm $ 74 4.5 X -1.03 $\pm $ 0.06 2.28 +0.21-0.21

L-14
2.13 $\pm $ 0.71 159.5 $\pm $ 6.0 322 $\pm $ 33 426 $\pm $ 70 0.7 X -0.73 $\pm $ 0.09 1.81 +0.26-0.26

L-15
2.36 $\pm $ 0.62 68.6 $\pm $ 3.7 181 $\pm $ 21 258 $\pm $ 69 1.0 X -1.03 $\pm $ 0.14 2.31 +0.20-0.20

L-17
2.24 $\pm $ 0.64 341.0 $\pm $ 33.0 756 $\pm $ 78 1052 $\pm $ 75 X X -0.76 $\pm $ 0.10 1.68 +0.20-0.20

L-20
2.66 $\pm $ 0.78 51.1 $\pm $ 4.7 166 $\pm $ 19 264 $\pm $ 72 1.5 X -1.25 $\pm $ 0.18 1.95 +0.17-0.17

L-21
3.09 $\pm $ 0.81 138.3 $\pm $ 35.8 176 $\pm $ 38 350 $\pm $ 76 4.1 1.8 -0.64 $\pm $ 0.28 2.51 +0.37-0.37

L-23
3.13 $\pm $ 0.86 86.4 $\pm $ 7.2 172 $\pm $ 21 242 $\pm $ 71 1.3 X -0.77 $\pm $ 0.07 2.23 +0.23-0.23

L-25
2.56 $\pm $ 0.74 69.0 $\pm $ 9.0 166 $\pm $ 20 348 $\pm $ 72 1.4 X -1.09 $\pm $ 0.04 2.63 +0.25-0.25

L-27
2.48 $\pm $ 0.73 77.2 $\pm $ 13.7 106 $\pm $ 18 219 2.1 X -0.38 $\pm $ 0.39 2.47 +0.27-0.27
Other non detections at 1.2 mm
L-2 3.04 (1.46 $\pm $ 0.79) 42.0 90 $\pm $ 17 215 X X [-0.64]  

L-3
3.33 (1.04 $\pm $ 1.11) 105.0 $\pm $ 35.0 50 $\pm $ 17 227 7.6 X +0.89 $\pm $ 0.85  

L-4
3.42 (0.76 $\pm $ 1.14) 93.0 76 $\pm $ 17 220 X X [-0.64]  

L-6
2.22 (0.59 $\pm $ 0.74) 37.1 $\pm $ 6.4 69 $\pm $ 12 202 1.4 X -0.75 $\pm $ 0.42  

L-7
2.97 (1.39 $\pm $ 0.79) 101.7 $\pm $ 13.3 200 $\pm $ 23 216 2.0 0.8 -0.81 $\pm $ 0.29  

L-8
2.70 (-0.36 $\pm $ 0.90) 124.0 $\pm $ 14.0 219 $\pm $ 25 250 $\pm $ 72 1.4 X -0.58 $\pm $ 0.13  

L-10
3.01 (1.39 $\pm $ 0.81) 67.2 $\pm $ 11.7 94 $\pm $ 17 $\mathellipsis$ 3.7 X -0.40 $\pm $ 0.37  

L-12
3.64 (2.06 $\pm $ 0.79) 94.4 $\pm $ 4.7 182 $\pm $ 28 315 $\pm $ 69 1.3 X -0.81 $\pm $ 0.02  

L-13
3.15 (-0.49 $\pm $ 1.05) 39.0 58 $\pm $ 16 219 X X [-0.64]  

L-16
2.58 (0.51 $\pm $ 0.86) $\mathellipsis$ 145 $\pm $ 32 319 $\pm $ 77 X X -1.25 $\pm $ 0.76  

L-18
2.43 (-0.72 $\pm $ 0.81) 93.2 $\pm $ 9.4 162 $\pm $ 19 209 2.4 X -0.67 $\pm $ 0.36  

L-19
2.91 (0.89 $\pm $ 0.97) 102.2 $\pm $ 12.0 138 $\pm $ 18 231 $\pm $ 69 3.9 1.8 -0.44 $\pm $ 0.13  

L-24
2.64 (0.14 $\pm $ 0.88) 24.0 45 $\pm $ 14 211 X X [-0.64]  

L-26
2.58 (0.37 $\pm $ 0.86) 54.9 $\pm $ 13.4 84 $\pm $ 14 255 $\pm $ 72 3.5 X -0.86 $\pm $ 0.53  

L-28
2.96 (1.64 $\pm $ 0.66) 23.0 47 $\pm $ 12 213 X X [-0.64]  

L-29
2.94 (0.45 $\pm $ 0.98) 55.0 $\pm $ 12.0 76 $\pm $ 16 216 X X -0.39 $\pm $ 0.52  

L-30
1.89 (0.42 $\pm $ 0.63) 70.0 84 $\pm $ 18 236 X X [-0.64]  

L-31
2.82 (1.62 $\pm $ 0.60) 121.0 $\pm $ 39.0 157 $\pm $ 20 221 6.6 X -0.31 $\pm $ 0.50  

L-32
2.89 (1.61 $\pm $ 0.64) 48.0 60 $\pm $ 16 $\mathellipsis$ X X [-0.64]  

L-33
3.27 (-0.28 $\pm $ 1.09) 109.0 $\pm $ 33.0 87 $\pm $ 19 235 10.0 X +0.27 $\pm $ 0.61  

a The limits on $F_{\rm 1.2~mm}$ are ``3$\sigma $'' limits, except for the sources with 1.5 < $ {\it S/N}$ < 3 where they are the observed value plus 2$\sigma $. The values in brackets are the observed values used in stacks.
b The radio flux density limits are ``3$\sigma $'' limits.
c The values of $\alpha$ in brackets show the cases where $\alpha$ cannot be determined and is assumed equal to -0.64 (see text).



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