The NIKA2 cosmological legacy survey at 2 mm: Catalogs, colors, redshift distributions, and implications for deep surveys

Open Access

Table B.1.

High-quality (95 % purity) 2 mm N2CLS catalog in the GOODS-N field.

N2CLS name	IAU name	R.A._2 mm	Dec_2 mm	S/N_2 mm	S_2 mm	S/N_1.2 mm	S_1.2 mm
		deg	deg		mJy		mJy
N2GN_1_01	N2GN J123633+621408	189.1400	62.2361	35.7	1.22 $\begin{matrix} 0.13 \\ - 0.12 \end{matrix}$ $Mathematical equation: $ \substack{0.13 \\ -0.12} $$	40.0	5.00 $\begin{matrix} 0.48 \\ - 0.48 \end{matrix}$ $Mathematical equation: $ \substack{0.48 \\ -0.48} $$
N2GN_1_02	N2GN J123730+621259	189.3786	62.2160	16.6	0.86 $\begin{matrix} 0.15 \\ - 0.13 \end{matrix}$ $Mathematical equation: $ \substack{0.15 \\ -0.13} $$	25.6	4.77 $\begin{matrix} 0.43 \\ - 0.58 \end{matrix}$ $Mathematical equation: $ \substack{0.43 \\ -0.58} $$
N2GN_1_03	N2GN J123707+621408	189.2802	62.2355	15.3	0.52 $\begin{matrix} 0.07 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.07 \\ -0.09} $$	23.2	2.91 $\begin{matrix} 0.30 \\ - 0.22 \end{matrix}$ $Mathematical equation: $ \substack{0.30 \\ -0.22} $$
N2GN_1_04	N2GN J123711+622211	189.2991	62.3700	18.8	1.85 $\begin{matrix} 0.29 \\ - 0.23 \end{matrix}$ $Mathematical equation: $ \substack{0.29 \\ -0.23} $$	21.4	8.06 $\begin{matrix} 0.68 \\ - 0.91 \end{matrix}$ $Mathematical equation: $ \substack{0.68 \\ -0.91} $$
N2GN_1_05	N2GN J123711+621330	189.2988	62.2253	16.0	0.60 $\begin{matrix} 0.10 \\ - 0.08 \end{matrix}$ $Mathematical equation: $ \substack{0.10 \\ -0.08} $$	20.6	2.71 $\begin{matrix} 0.28 \\ - 0.31 \end{matrix}$ $Mathematical equation: $ \substack{0.28 \\ -0.31} $$
N2GN_1_06	N2GN J123652+621226	189.2160	62.2072	13.3	0.46 $\begin{matrix} 0.09 \\ - 0.08 \end{matrix}$ $Mathematical equation: $ \substack{0.09 \\ -0.08} $$	19.1	2.36 $\begin{matrix} 0.23 \\ - 0.29 \end{matrix}$ $Mathematical equation: $ \substack{0.23 \\ -0.29} $$
N2GN_1_07	N2GN J123645+621448	189.1923	62.2470	9.3	0.31 $\begin{matrix} 0.06 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.06 \\ -0.09} $$	19.0	2.29 $\begin{matrix} 0.24 \\ - 0.22 \end{matrix}$ $Mathematical equation: $ \substack{0.24 \\ -0.22} $$
N2GN_1_08	N2GN J123631+621714	189.1333	62.2875	11.3	0.56 $\begin{matrix} 0.12 \\ - 0.11 \end{matrix}$ $Mathematical equation: $ \substack{0.12 \\ -0.11} $$	18.0	3.38 $\begin{matrix} 0.42 \\ - 0.43 \end{matrix}$ $Mathematical equation: $ \substack{0.42 \\ -0.43} $$
N2GN_1_09	N2GN J123627+621217	189.1139	62.2046	10.6	0.36 $\begin{matrix} 0.08 \\ - 0.08 \end{matrix}$ $Mathematical equation: $ \substack{0.08 \\ -0.08} $$	18.0	2.20 $\begin{matrix} 0.31 \\ - 0.25 \end{matrix}$ $Mathematical equation: $ \substack{0.31 \\ -0.25} $$
N2GN_1_11	N2GN J123713+621826	189.3081	62.3072	13.1	0.49 $\begin{matrix} 0.08 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.08 \\ -0.09} $$	15.2	2.14 $\begin{matrix} 0.33 \\ - 0.29 \end{matrix}$ $Mathematical equation: $ \substack{0.33 \\ -0.29} $$
N2GN_1_12	N2GN J123636+621155	189.1530	62.1985	8.3	0.27 $\begin{matrix} 0.10 \\ - 0.07 \end{matrix}$ $Mathematical equation: $ \substack{0.10 \\ -0.07} $$	15.1	1.79 $\begin{matrix} 0.25 \\ - 0.29 \end{matrix}$ $Mathematical equation: $ \substack{0.25 \\ -0.29} $$
N2GN_1_13	N2GN J123658+621451	189.2440	62.2476	11.7	0.37 $\begin{matrix} 0.07 \\ - 0.08 \end{matrix}$ $Mathematical equation: $ \substack{0.07 \\ -0.08} $$	14.6	1.71 $\begin{matrix} 0.21 \\ - 0.25 \end{matrix}$ $Mathematical equation: $ \substack{0.21 \\ -0.25} $$
N2GN_1_14	N2GN J123701+621146	189.2567	62.1963	6.7	0.28 $\begin{matrix} 0.10 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.10 \\ -0.09} $$	13.3	1.88 $\begin{matrix} 0.25 \\ - 0.27 \end{matrix}$ $Mathematical equation: $ \substack{0.25 \\ -0.27} $$
N2GN_1_15	N2GN J123618+621550	189.0762	62.2640	6.6	0.32 $\begin{matrix} 0.10 \\ - 0.12 \end{matrix}$ $Mathematical equation: $ \substack{0.10 \\ -0.12} $$	13.2	2.38 $\begin{matrix} 0.43 \\ - 0.35 \end{matrix}$ $Mathematical equation: $ \substack{0.43 \\ -0.35} $$
N2GN_1_16	N2GN J123622+621615	189.0930	62.2721	4.7	0.23 $\begin{matrix} 0.13 \\ - 0.12 \end{matrix}$ $Mathematical equation: $ \substack{0.13 \\ -0.12} $$	12.5	2.33 $\begin{matrix} 0.37 \\ - 0.35 \end{matrix}$ $Mathematical equation: $ \substack{0.37 \\ -0.35} $$
N2GN_1_17	N2GN J123738+621734	189.4097	62.2934	11.4	0.51 $\begin{matrix} 0.10 \\ - 0.11 \end{matrix}$ $Mathematical equation: $ \substack{0.10 \\ -0.11} $$	11.9	2.00 $\begin{matrix} 0.31 \\ - 0.42 \end{matrix}$ $Mathematical equation: $ \substack{0.31 \\ -0.42} $$
N2GN_1_18	N2GN J123702+621425	189.2619	62.2413	6.7	0.21 $\begin{matrix} 0.08 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.08 \\ -0.09} $$	11.6	1.36 $\begin{matrix} 0.27 \\ - 0.21 \end{matrix}$ $Mathematical equation: $ \substack{0.27 \\ -0.21} $$
N2GN_1_23	N2GN J123656+621207	189.2333	62.2023	4.7	0.17 $\begin{matrix} 0.11 \\ - 0.09 \end{matrix}$ $Mathematical equation: $ \substack{0.11 \\ -0.09} $$	9.5	1.23 $\begin{matrix} 0.31 \\ - 0.29 \end{matrix}$ $Mathematical equation: $ \substack{0.31 \\ -0.29} $$
N2GN_1_24	N2GN J123719+621219	189.3289	62.2048	4.2	0.20 $\begin{matrix} 0.18 \\ - 0.12 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.12} $$	8.9	1.49 $\begin{matrix} 0.34 \\ - 0.37 \end{matrix}$ $Mathematical equation: $ \substack{0.34 \\ -0.37} $$
N2GN_1_25	N2GN J123712+621212	189.3037	62.2026	4.6	0.20 $\begin{matrix} 0.13 \\ - 0.11 \end{matrix}$ $Mathematical equation: $ \substack{0.13 \\ -0.11} $$	8.7	1.32 $\begin{matrix} 0.34 \\ - 0.26 \end{matrix}$ $Mathematical equation: $ \substack{0.34 \\ -0.26} $$
N2GN_1_28	N2GN J123728+621920	189.3638	62.3227	5.8	0.27 $\begin{matrix} 0.13 \\ - 0.13 \end{matrix}$ $Mathematical equation: $ \substack{0.13 \\ -0.13} $$	7.9	1.38 $\begin{matrix} 0.39 \\ - 0.36 \end{matrix}$ $Mathematical equation: $ \substack{0.39 \\ -0.36} $$
N2GN_1_34	N2GN J123644+621938	189.1864	62.3275	5.6	0.36 $\begin{matrix} 0.19 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.19 \\ -0.14} $$	6.9	1.63 $\begin{matrix} 0.61 \\ - 0.50 \end{matrix}$ $Mathematical equation: $ \substack{0.61 \\ -0.50} $$
N2GN_1_36	N2GN J123658+620930	189.2443	62.1585	6.4	0.36 $\begin{matrix} 0.14 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.14 \\ -0.14} $$	6.0	1.19 $\begin{matrix} 0.43 \\ - 0.38 \end{matrix}$ $Mathematical equation: $ \substack{0.43 \\ -0.38} $$
N2GN_2_13	N2GN J123720+621128	189.3374	62.1913	7.4	0.43 $\begin{matrix} 0.11 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.11 \\ -0.14} $$	–	< 2
N2GN_2_20	N2GN J123608+621251	189.0370	62.2142	5.1	0.24 $\begin{matrix} 0.13 \\ - 0.12 \end{matrix}$ $Mathematical equation: $ \substack{0.13 \\ -0.12} $$	3.3	0.52 $\begin{matrix} 0.29 \\ - 0.28 \end{matrix}$ $Mathematical equation: $ \substack{0.29 \\ -0.28} $$

Notes. The first and second columns: N2CLS short names and the IAU names, respectively. The R.A._2 mm and Dec_2 mm columns are the coordinates of the sources measured in the 2 mm maps. The four last columns (S/N_2 mm, S_2 mm, S/N_1.2 mm et S_1.2 mm) are the S/N at 2 mm, the N2CLS flux at 2 mm, the S/N at 1.2 mm, and the N2CLS flux at 1.2 mm, respectively. For the source without 1.2 mm counterpart, we provide a 5 σ upper limit on the flux. The redshifts are provided in Berta et al. (2025).

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