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Table 2.

Continuum detections at S/N ≥ 4.5.

ID RAJ2000 DecJ2000 S/N S1.1 mm, peak S1.1 mm,uv−fit rs z
(hh:mm:ss.ss) (±dd:mm:ss.ss) (mJy beam−1) (mJy) (″)
(1) (2) (3) (4) (5) (6) (7) (8)
A2744-ID01 (a) 00:14:19.80 −30:23:07.66 25.9 1.433 ± 0.056 1.570 ± 0.073 0.05 ± 0.01 2.9 (c)
A2744-ID02 (a) 00:14:18.25 −30:24:47.47 14.4 1.292 ± 0.091 2.816 ± 0.229 0.23 ± 0.04 2.585 (d)
A2744-ID03 (a) 00:14:20.40 −30:22:54.42 13.9 0.798 ± 0.058 1.589 ± 0.125 0.26 ± 0.03 3.058 (d)
A2744-ID04 (a) 00:14:17.58 −30:23:00.56 13.8 0.932 ± 0.068 1.009 ± 0.074 0.06 ± 0.02 1.498 (d)
A2744-ID05 (a) 00:14:19.12 −30:22:42.20 7.7 0.655 ± 0.086 1.113 ± 0.135 0.19 ± 0.05 2.409 (d)
A2744-ID06 (a) 00:14:17.28 −30:22:58.60 6.5 0.574 ± 0.089 1.283 ± 0.241 0.26 ± 0.08 (e)
A2744-ID07 (a) 00:14:22.10 −30:22:49.67 6.2 0.455 ± 0.074 0.539 ± 0.082 0.07 ± 0.04 2.644 (d)
A2744-ID08 (b) 00:14:24.73 −30:24:34.20 4.8 0.270 ± 0.056 ... ... ...
A2744-ID09 (b) 00:14:21.23 −30:23:28.70 4.7 0.256 ± 0.055 ... ... ...
A2744-ID10 (b) 00:14:17.72 −30:23:02.25 4.5 0.286 ± 0.063 ... ... ...
A2744-ID11 (b) 00:14:22.63 −30:23:30.45 4.5 0.253 ± 0.056 ... ... ...
MACSJ0416-ID01 (a) 04:16:10.79 −24:04:47.53 15.4 1.010 ± 0.066 1.319 ± 0.103 0.23 ± 0.06 2.086 (c)
MACSJ0416-ID02 (a) 04:16:06.96 −24:03:59.96 6.8 0.406 ± 0.062 0.574 ± 0.132 0.32 ± 0.15 1.953 (c)
MACSJ0416-ID03 (a) 04:16:08.81 −24:05:22.58 5.8 0.389 ± 0.067 0.411 ± 0.072 0.10 ± 0.07 (e)
MACSJ0416-ID04 (a) 04:16:11.67 −24:04:19.44 5.1 0.333 ± 0.066 0.478 ± 0.166 0.37 ± 0.21 (e)
MACSJ0416-ID05 (b) 04:16:10.52 −24:05:04.77 4.6 0.302 ± 0.066 ... ... 1.849 (f)
MACSJ1149-ID01 (a) 11:49:36.09 +22:24:24.60 5.9 0.442 ± 0.074 0.579 ± 0.134 0.28 ± 0.13 1.46 (c)
MACSJ1149-ID02 (b) 11:49:40.32 +22:24:42.00 4.6 0.524 ± 0.113 ... ... ...
MACSJ1149-ID03 (b) 11:49:35.41 +22:23:38.60 4.5 0.326 ± 0.072 ... ... ...
A370-ID01 (a) 02:39:56.57 −01:34:26.40 25.1 1.624 ± 0.065 1.925 ± 0.088 0.22 ± 0.03 1.06 (f)
A370-ID02 (a) 02:39:57.58 −01:34:53.67 9.1 1.656 ± 0.182 1.778 ± 0.192 0.10 ± 0.05 (g)
A370-ID03 (a) 02:39:58.15 −01:34:24.52 7.0 0.655 ± 0.094 1.007 ± 0.205 0.42 ± 0.13 1.258 (h)
A370-ID04 (b) 02:39:53.25 −01:33:29.26 4.7 0.439 ± 0.094 ... ... ...
A370-ID05 (b) 02:39:53.20 −01:34:38.16 4.5 0.283 ± 0.063 ... ... ...
AS1063-ID01 (a) 22:48:49.06 −44:32:25.39 89.3 6.295 ± 0.071 6.806 ± 0.119 0.14 ± 0.01 (g)
AS1063-ID02 (a) 22:48:47.29 −44:30:48.06 10.9 1.282 ± 0.118 1.273 ± 0.142 0.10 ± 0.05 1.438 (f)
AS1063-ID03 (a) 22:48:46.58 −44:30:46.83 5.2 0.648 ± 0.124 1.396 ± 0.399 0.45 ± 0.14 (g)
AS1063-ID04 (b) 22:48:41.79 −44:31:57.80 4.9 0.338 ± 0.069 ... ... 0.611 (i)
AS1063-ID05 (b) 22:48:42.24 −44:32:29.20 4.6 0.320 ± 0.069 ... ... ...

Notes. Column 1: Source ID. Columns 2, 3: Centroid J2000 position of ID. Column 4: Signal-to-noise ratio of the detection, that is, the ratio of peak intensity and background rms. Column 5: PB-corrected peak intensity and 1σ error. Column 6: PB-corrected integrated flux density and 1σ error from uv fitting. Column 7: Effective radius and 1σ error from uv fitting, defined as (half-light radius). Column 8: Source redshift;

(a)

high-significance (S/N ≥ 5) detections;

(b)

low-significance (4.5 ≤ S/N < 5) detections; instead of performing a uv fitting, we estimate the integrated flux density using the peak intensity and assuming given source size parameters (see Sect. 2.1); for sources that lack redshift estimates, we assume a Gaussian redshift distribution with mean z = 2 and σ = 0.5;

(c)

spectroscopic redshift from GLASS, already noted in Papers II and IV;

(d)

spectroscopic redshift from Bauer et al. (in prep.);

(e)

photometric redshift found in Paper II;

(f)

spectroscopic redshift from GLASS;

(g)

photometric redshift from HFF-DeepSpace;

(h)

spectroscopic redshift from Lagattuta et al. (2022);

(i)

spectroscopic redshift from CLASH.

The photometric redshift’s best value and 1σ error from SED fitting are presented here only for reference, as we use the full probability distribution found for each photometric redshift.

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