Source |
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![]() ![]() ![]() |
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SMG/SFRG |
(1024 W Hz-1) | (1012 ![]() |
(![]() |
(1011 ![]() |
(1011 ![]() |
|||||
L-1 |
1.92 | 1.60 | 4.63 ![]() |
3.27 ![]() |
834 | 588 | 1.67 | 1.03 | SMG |
L-2 |
1.92 | 0.96 | 4.77 | 1.96 ![]() |
859 | 353 | 1.61 | 1.08 | weak Radio? |
L-3 |
1.73 | 0.33 | 5.22 | 0.66 ![]() |
941 | 284 | 1.66 | 1.13 | weak Radio |
L-4 |
2.13 | 1.02 | 5.37 | 2.08 ![]() |
966 | 1664 | 3.02 | 2.85 | SFRG? |
L-5 |
2.04 | 2.40 | 4.32 ![]() |
4.90 ![]() |
777 | 883 | 2.53 | 1.36 | SMG? |
L-6 |
2.26 | 1.10 | 3.49 | 2.25 ![]() |
627 | 405 | 2.07 | 1.07 | SFRG? |
L-7 |
1.89 | 2.15 | 4.66 | 4.35 ![]() |
839 | 788 | 2.19 | 1.55 | ? |
L-8 |
2.42 | 3.80 | 4.24 | [7.75 ![]() |
763 | [1396] | 2.89 | [1.52] | SFRG |
L-9 |
2.33 | 2.99 | 6.28 ![]() |
6.11 ![]() |
1130 | 1100 | 2.71 | 2.66 | SMG |
L-10 |
2.45 | 1.56 | 4.73 | 3.19 ![]() |
851 | 574 | 4.01 | 2.31 | ? |
L-11 |
1.92 | 4.52 | 4.84 ![]() |
[9.21 ![]() |
870 | [1658] | 1.57 | [0.78] | SMG |
L-12 |
1.71 | 1.56 | 5.71 | 3.19 ![]() |
1029 | 575 | 3.19 | 3.09 | ? |
L-13 |
2.22 | 0.86 | 4.95 | 1.75 ![]() |
891 | 315 | 1.60 | 0.87 | weak Radio |
L-14 |
2.36 | 5.53 | 3.34 ![]() |
[11.30 ![]() |
602 | [2029] | 3.37 | [1.74] | SMG? |
L-15 |
1.86 | 1.92 | 3.71 ![]() |
3.93 ![]() |
667 | 707 | 3.09 | 3.21 | SMG? |
L-16 |
1.73 | 1.36 | 4.05 | 2.77 ![]() |
729 | 499 | 1.34 | 0.92 | SFRG? |
L-17 |
1.90 | 7.90 | 3.52 ![]() |
[16.12 ![]() |
633 | [2902] | 2.27 | [1.07] | SMG? |
L-18 |
1.85 | 1.60 | 3.82 | 3.27 ![]() |
688 | 589 | 3.05 | 2.17 | SFRG |
L-19 |
1.69 | 1.08 | 4.57 | 2.21 ![]() |
822 | 398 | 1.67 | 0.99 | ? |
L-20 |
2.69 | 4.98 | 4.18 ![]() |
10.20 ![]() |
752 | 1830 | 5.68 | 7.16 | SMG? |
L-21 |
1.78 | 1.61 | 4.85 ![]() |
3.23 ![]() |
873 | 592 | 1.74 | 1.12 | SMG? |
L-22 |
2.57 | 5.70 | 5.35 ![]() |
11.62 ![]() |
964 | 2092 | 4.11 | 3.06 | SMG |
L-23 |
2.38 | 3.08 | 4.91 ![]() |
6.28 ![]() |
885 | 1130 | 2.27 | 1.27 | SMG? |
L-24 |
2.07 | 0.57 | 4.14 | 1.16 ![]() |
746 | 209 | 1.82 | 1.02 | weak Radio |
L-25 |
1.47a | 1.01 | 4.02 ![]() |
2.07 ![]() |
723 | 372 | 1.29 | 0.84 | SMG? |
L-26 |
1.72 | 0.73 | 4.05 | 1.49 ![]() |
729 | 579 | 1.55 | 1.57 | weak Radio |
L-27 |
2.20 | 1.41 | 3.89 ![]() |
2.87 ![]() |
701 | 517 | 2.18 | 1.21 | SMG? |
L-28 |
1.88 | 0.48 | 4.65 | 0.98 ![]() |
836 | 176 | 1.79 | 1.29 | ? |
L-29 |
1.93 | 0.77 | 4.62 | 1.58 ![]() |
831 | 284 | 2.33 | 1.62 | weak Radio |
L-30 |
2.38 | 1.45 | 2.97 | 2.96 ![]() |
534 | 1290 | 3.17 | 2.01 | SFRG |
L-31 |
2.74 | 3.13 | 4.43 | 6.39 ![]() |
797 | 1150 | 3.65 | 1.37 | ? |
L-32 |
2.38 | 1.03 | 4.53 ![]() |
2.10 ![]() |
815 | 278 | 2.77 | 1.84 | ? |
L-33 |
2.18 | 0.92 | 5.13 | 1.87 ![]() |
924 | 337 | 2.47 | 1.49 | weak Radio? |
a Spectroscopic redshift from Berta et al. (2007b).
b The value of
,
the rest-frame luminosity at 1.4 GHz, is the weighted average of the two determinations of
from 20 cm and 50 cm flux densities when both are available.
c The values of
,
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
and SFR
are ``3
'' limits, except for the sources with 1.5 < S/N < 3 where they are the observed value plus 2
.
The upper limits of
and SFR
are ``3
'' limits.
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