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Table B.1.

Characteristics of the continuum-detected target sources.

Name RA Dec Freq. S/N S/N Sν νLν LIR
(h:min:s) (deg:min:s) (GHz) (tap.) (μJy) log10(L/L)
DEIMOS_COSMOS_873756 10:00:02.72 +02:37:39.99 347.4 21.7 20.1 1355 ± 76 11.41 12.26
DEIMOS_COSMOS_818760 10:01:54.86 +02:32:31.43 347.2 9.5 9.6 1077 ± 130 11.31 12.16
DEIMOS_COSMOS_488399 10:03:01.15 +02:02:35.77 291.5 9.3 9.0 253 ± 32 10.83 11.67
DEIMOS_COSMOS_494057 09:58:28.50 +02:03:06.42 295.7 7.1 5.6 179 ± 30 10.66 11.51
DEIMOS_COSMOS_848185 10:00:21.50 +02:35:11.03 307.6 7.1 7.5 319 ± 50 10.88 11.73
vuds_cosmos_5100822662 09:58:57.90 +02:04:51.38 349.8 6.5 4.8 210 ± 38 10.60 11.45
vuds_cosmos_5101218326 10:01:12.50 +02:18:52.37 348.1 6.5 6.3 462 ± 79 10.95 11.79
vuds_cosmos_5180966608 10:01:37.48 +02:08:23.39 350.4 5.7 5.6 419 ± 84 10.90 11.74
DEIMOS_COSMOS_396844 10:00:59.65 +01:53:47.52 348.0 5.6 4.6 346 ± 69 10.82 11.67
CANDELS_GOODSS_19 03:32:22.97 −27:46:29.32 350.6 5.4 3.9 278 ± 61 10.71 11.57
DEIMOS_COSMOS_683613 10:00:09.41 +02:20:13.41 295.8 5.1 5.1 245 ± 54 10.80 11.65
DEIMOS_COSMOS_552206 09:58:26.80 +02:08:26.80 296.7 4.5 4.5 285 ± 73 10.86 11.71
vuds_cosmos_5101209780 Multi-component object, see Appendix D.1
DEIMOS_COSMOS_422677 10:01:59.46 +01:56:12.93 355.9 4.3 3.2 375 ± 123 10.84 11.68
vuds_cosmos_5100969402 10:01:20.11 +02:17:01.13 346.0 4.0 3.9 327 ± 99 10.80 11.65
vuds_cosmos_5100994794 10:00:41.18 +02:17:14.27 346.0 4.0 2.3 117 ± 36 10.35 11.20
CANDELS_GOODSS_32 03:32:17.01 −27:41:13.97 356.2 3.9 3.2 230 ± 65 10.62 11.47
DEIMOS_COSMOS_460378 10:00:11.39 +01:59:54.00 302.3 3.8 2.8 116 ± 35 10.46 11.31
DEIMOS_COSMOS_539609 09:59:07.25 +02:07:21.02 314.5 3.7 3.2 187 ± 54 10.64 11.48
vuds_efdcs_530029038 Multi-component object, see Appendix D.1
DEIMOS_COSMOS_493583 10:00:23.36 +02:03:04.23 349.4 3.6 2.9 235 ± 81 10.64 11.50
DEIMOS_COSMOS_417567 10:02:04.14 +01:55:43.93 289.9 3.6 3.7 201 ± 60 10.73 11.58
DEIMOS_COSMOS_881725 Multi-component object, see Appendix D.1

Notes. The frequency is the mean of the channels used to derive the continuum. The flux Sν was measured using the 2D-fit approached described in Sect. 3.1. The monochromatic luminosity νLν is derived at (1 + z) νobs and does not need any assumption on the galaxy SEDs. The total infrared luminosity LIR (8−1000 μm) is derived assuming Bethermin et al. (2017) SED (see discussion in Sect. 4). The measurement uncertainties do not include the calibration uncertainties (∼4.5% on average and up to 10%, see Sect. 2.3).

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