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Table 5:

Luminosities and star formation rates.
Source $z_{\rm phot}$ $L_{\rm {1.4~GHz}}$b $L_{\rm {FIR,mm}}$ $L_{\rm {FIR,radio}}$c $SFR_{\rm {mm}}$d $SFR_{\rm {radio}}$d $\nu$$L_{\nu}$(1.6 $\mu $m) $M_{\star}$ SMG/SFRG
    (1024 W Hz-1) (1012 $L_{\odot}$) ($M_{\odot }$ yr-1) (1011 $L_{\odot}$) (1011 $M_{\odot }$)  

L-1
1.92 1.60 4.63 $\pm $ 1.04 3.27 $\pm $ 0.81 834 588 1.67 1.03 SMG

L-2
1.92 0.96 4.77 1.96 $\pm $ 0.39 859 353 1.61 1.08 weak Radio?

L-3
1.73 0.33 5.22 0.66 $\pm $ 0.52 941 284 1.66 1.13 weak Radio

L-4
2.13 1.02 5.37 2.08 $\pm $ 3.08 966 1664 3.02 2.85 SFRG?

L-5
2.04 2.40 4.32 $\pm $ 1.19 4.90 $\pm $ 0.92 777 883 2.53 1.36 SMG?

L-6
2.26 1.10 3.49 2.25 $\pm $ 0.79 627 405 2.07 1.07 SFRG?

L-7
1.89 2.15 4.66 4.35 $\pm $ 1.06 839 788 2.19 1.55 ?

L-8
2.42 3.80 4.24 [7.75 $\pm $ 1.09] 763 [1396] 2.89 [1.52] SFRG

L-9
2.33 2.99 6.28 $\pm $ 0.86 6.11 $\pm $ 1.94 1130 1100 2.71 2.66 SMG

L-10
2.45 1.56 4.73 3.19 $\pm $ 1.05 851 574 4.01 2.31 ?

L-11
1.92 4.52 4.84 $\pm $ 0.91 [9.21 $\pm $ 3.63] 870 [1658] 1.57 [0.78] SMG

L-12
1.71 1.56 5.71 3.19 $\pm $ 1.12 1029 575 3.19 3.09 ?

L-13
2.22 0.86 4.95 1.75 $\pm $ 0.89 891 315 1.60 0.87 weak Radio

L-14
2.36 5.53 3.34 $\pm $ 1.11 [11.30 $\pm $ 2.99] 602 [2029] 3.37 [1.74] SMG?

L-15
1.86 1.92 3.71 $\pm $ 0.97 3.93 $\pm $ 0.76 667 707 3.09 3.21 SMG?

L-16
1.73 1.36 4.05 2.77 $\pm $ 1.51 729 499 1.34 0.92 SFRG?

L-17
1.90 7.90 3.52 $\pm $ 1.00 [16.12 $\pm $ 2.70] 633 [2902] 2.27 [1.07] SMG?

L-18
1.85 1.60 3.82 3.27 $\pm $ 0.86 688 589 3.05 2.17 SFRG

L-19
1.69 1.08 4.57 2.21 $\pm $ 0.53 822 398 1.67 0.99 ?

L-20
2.69 4.98 4.18 $\pm $ 1.22 10.20 $\pm $ 0.95 752 1830 5.68 7.16 SMG?

L-21
1.78 1.61 4.85 $\pm $ 1.27 3.23 $\pm $ 1.94 873 592 1.74 1.12 SMG?

L-22
2.57 5.70 5.35 $\pm $ 1.15 11.62 $\pm $ 4.323 964 2092 4.11 3.06 SMG

L-23
2.38 3.08 4.91 $\pm $ 1.35 6.28 $\pm $ 1.63 885 1130 2.27 1.27 SMG?

L-24
2.07 0.57 4.14 1.16 $\pm $ 0.29 746 209 1.82 1.02 weak Radio

L-25
1.47a 1.01 4.02 $\pm $ 1.16 2.07 $\pm $ 0.59 723 372 1.29 0.84 SMG?

L-26
1.72 0.73 4.05 1.49 $\pm $ 1.07 729 579 1.55 1.57 weak Radio

L-27
2.20 1.41 3.89 $\pm $ 1.15 2.87 $\pm $ 0.96 701 517 2.18 1.21 SMG?

L-28
1.88 0.48 4.65 0.98 $\pm $ 0.20 836 176 1.79 1.29 ?

L-29
1.93 0.77 4.62 1.58 $\pm $ 0.68 831 284 2.33 1.62 weak Radio

L-30
2.38 1.45 2.97 2.96 $\pm $ 2.39 534 1290 3.17 2.01 SFRG

L-31
2.74 3.13 4.43 6.39 $\pm $ 3.43 797 1150 3.65 1.37 ?

L-32
2.38 1.03 4.53 $\pm $ 1.00 2.10 $\pm $ 1.54 815 278 2.77 1.84 ?

L-33
2.18 0.92 5.13 1.87 $\pm $ 0.97 924 337 2.47 1.49 weak Radio?

a Spectroscopic redshift from Berta et al. (2007b).
b The value of $L_{\rm {1.4~GHz}}$, the rest-frame luminosity at 1.4 GHz, is the weighted average of the two determinations of $L_{\rm {1.4~GHz}}$ from 20 cm and 50 cm flux densities when both are available.
c The values of $L_{\rm {FIR,radio}}$, the infrared SFR derived from the radio flux densities and the stellar mass are dubious for sources with high 20 cm/1.2 mm flux densities ratios. They are reported, in brackets.
d SFR calculated by Kennicutt's formula (Eq. (6)) with a Salpeter IMF (see text).
The upper limits of $L_{\rm {FIR,mm}}$ and SFR $_{\rm {mm}}$ are ``3$\sigma $'' limits, except for the sources with 1.5 < S/N < 3 where they are the observed value plus 2$\sigma $.
The upper limits of $L_{\rm {FIR,radio}}$ and SFR $_{\rm {radio}}$ are ``3$\sigma $'' limits.


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