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

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Volume 708 (April 2026)

A&A, 708 (2026) A295

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Table B.3.

Continued.

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
N2CO_1_60	N2CO J100010+022223	150.0424	2.3737	5.3	0.51 $\begin{matrix} 0.16 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.14} $$	8.3	2.68 $\begin{matrix} 0.50 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.50 \\ -0.46} $$
N2CO_1_62	N2CO J100012+021211	150.0544	2.2029	5.9	0.55 $\begin{matrix} 0.17 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.15} $$	8.3	2.71 $\begin{matrix} 0.52 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.52 \\ -0.46} $$
N2CO_1_63	N2CO J095950+022827	149.9610	2.4743	4.9	0.44 $\begin{matrix} 0.18 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.14} $$	8.3	2.62 $\begin{matrix} 0.51 \\ - 0.44 \end{matrix}$ $Mathematical equation: $ \substack{0.51 \\ -0.44} $$
N2CO_1_65	N2CO J100112+020852	150.3008	2.1477	8.5	0.86 $\begin{matrix} 0.16 \\ - 0.17 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.17} $$	8.2	2.85 $\begin{matrix} 0.55 \\ - 0.49 \end{matrix}$ $Mathematical equation: $ \substack{0.55 \\ -0.49} $$
N2CO_1_67	N2CO J095953+021853	149.9721	2.3147	7.8	0.72 $\begin{matrix} 0.16 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.15} $$	8.0	2.58 $\begin{matrix} 0.54 \\ - 0.51 \end{matrix}$ $Mathematical equation: $ \substack{0.54 \\ -0.51} $$
N2CO_1_71	N2CO J100104+022634	150.2693	2.4427	4.7	0.43 $\begin{matrix} 0.17 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.14} $$	7.8	2.58 $\begin{matrix} 0.54 \\ - 0.49 \end{matrix}$ $Mathematical equation: $ \substack{0.54 \\ -0.49} $$
N2CO_1_72	N2CO J100024+022947	150.1001	2.4962	7.0	0.65 $\begin{matrix} 0.15 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.15 \\ -0.14} $$	7.7	2.53 $\begin{matrix} 0.54 \\ - 0.49 \end{matrix}$ $Mathematical equation: $ \substack{0.54 \\ -0.49} $$
N2CO_1_74	N2CO J100057+021309	150.2393	2.2193	6.7	0.63 $\begin{matrix} 0.17 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.15} $$	7.7	2.50 $\begin{matrix} 0.53 \\ - 0.48 \end{matrix}$ $Mathematical equation: $ \substack{0.53 \\ -0.48} $$
N2CO_1_76	N2CO J100105+022151	150.2718	2.3631	5.4	0.34 $\begin{matrix} 0.14 \\ - 0.11 \end{matrix}$ $Mathematical equation: $ \substack{0.14 \\ -0.11} $$	7.7	2.41 $\begin{matrix} 0.51 \\ - 0.47 \end{matrix}$ $Mathematical equation: $ \substack{0.51 \\ -0.47} $$
N2CO_1_78	N2CO J100117+023218	150.3230	2.5378	6.0	0.64 $\begin{matrix} 0.19 \\ - 0.17 \end{matrix}$ $Mathematical equation: $ \substack{0.19 \\ -0.17} $$	7.6	2.73 $\begin{matrix} 0.59 \\ - 0.52 \end{matrix}$ $Mathematical equation: $ \substack{0.59 \\ -0.52} $$
N2CO_1_79	N2CO J100058+020138	150.2436	2.0285	6.1	0.62 $\begin{matrix} 0.17 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.15} $$	7.5	2.72 $\begin{matrix} 0.57 \\ - 0.53 \end{matrix}$ $Mathematical equation: $ \substack{0.57 \\ -0.53} $$
N2CO_1_85	N2CO J100041+022547	150.1749	2.4291	4.6	0.42 $\begin{matrix} 0.17 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.14} $$	7.4	2.37 $\begin{matrix} 0.53 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.53 \\ -0.46} $$
N2CO_1_87	N2CO J100109+021727	150.2907	2.2897	4.8	0.44 $\begin{matrix} 0.17 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.14} $$	7.3	2.35 $\begin{matrix} 0.52 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.52 \\ -0.46} $$
N2CO_1_88	N2CO J100056+020842	150.2342	2.1450	5.2	0.49 $\begin{matrix} 0.18 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.15} $$	7.3	2.37 $\begin{matrix} 0.52 \\ - 0.47 \end{matrix}$ $Mathematical equation: $ \substack{0.52 \\ -0.47} $$
N2CO_1_93	N2CO J100106+021532	150.2783	2.2587	5.2	0.50 $\begin{matrix} 0.19 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.19 \\ -0.15} $$	7.2	2.45 $\begin{matrix} 0.54 \\ - 0.48 \end{matrix}$ $Mathematical equation: $ \substack{0.54 \\ -0.48} $$
N2CO_1_97	N2CO J100013+020902	150.0534	2.1495	5.9	0.57 $\begin{matrix} 0.18 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.15} $$	7.1	2.39 $\begin{matrix} 0.52 \\ - 0.48 \end{matrix}$ $Mathematical equation: $ \substack{0.52 \\ -0.48} $$
N2CO_1_99	N2CO J100118+022352	150.3279	2.3980	4.8	0.51 $\begin{matrix} 0.20 \\ - 0.16 \end{matrix}$ $Mathematical equation: $ \substack{0.20 \\ -0.16} $$	7.0	2.56 $\begin{matrix} 0.55 \\ - 0.52 \end{matrix}$ $Mathematical equation: $ \substack{0.55 \\ -0.52} $$
N2CO_1_101	N2CO J100046+021309	150.1923	2.2197	7.9	0.75 $\begin{matrix} 0.17 \\ - 0.16 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.16} $$	6.9	2.25 $\begin{matrix} 0.57 \\ - 0.51 \end{matrix}$ $Mathematical equation: $ \substack{0.57 \\ -0.51} $$
N2CO_1_108	N2CO J095944+022109	149.9344	2.3530	7.0	0.68 $\begin{matrix} 0.18 \\ - 0.16 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.16} $$	6.6	2.23 $\begin{matrix} 0.57 \\ - 0.51 \end{matrix}$ $Mathematical equation: $ \substack{0.57 \\ -0.51} $$
N2CO_1_111	N2CO J100018+021241	150.0769	2.2107	4.8	0.45 $\begin{matrix} 0.18 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.14} $$	6.6	2.21 $\begin{matrix} 0.56 \\ - 0.49 \end{matrix}$ $Mathematical equation: $ \substack{0.56 \\ -0.49} $$
N2CO_1_114	N2CO J100103+022140	150.2639	2.3616	6.3	0.56 $\begin{matrix} 0.16 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.14} $$	6.5	2.07 $\begin{matrix} 0.55 \\ - 0.48 \end{matrix}$ $Mathematical equation: $ \substack{0.55 \\ -0.48} $$
N2CO_1_118	N2CO J100035+022827	150.1477	2.4740	6.1	0.57 $\begin{matrix} 0.17 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.14} $$	6.4	2.04 $\begin{matrix} 0.53 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.53 \\ -0.46} $$
N2CO_1_128	N2CO J100048+023016	150.2042	2.5033	6.1	0.57 $\begin{matrix} 0.16 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.14} $$	6.2	1.71 $\begin{matrix} 0.50 \\ - 0.45 \end{matrix}$ $Mathematical equation: $ \substack{0.50 \\ -0.45} $$
N2CO_1_138	N2CO J095958+020604	149.9915	2.0998	5.2	0.49 $\begin{matrix} 0.18 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.15} $$	5.9	1.98 $\begin{matrix} 0.59 \\ - 0.50 \end{matrix}$ $Mathematical equation: $ \substack{0.59 \\ -0.50} $$
N2CO_1_143	N2CO J095948+022752	149.9546	2.4641	5.7	0.54 $\begin{matrix} 0.16 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.15} $$	5.9	1.94 $\begin{matrix} 0.59 \\ - 0.50 \end{matrix}$ $Mathematical equation: $ \substack{0.59 \\ -0.50} $$
N2CO_1_156	N2CO J100105+023239	150.2741	2.5447	4.7	0.46 $\begin{matrix} 0.18 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.14} $$	5.6	1.89 $\begin{matrix} 0.57 \\ - 0.50 \end{matrix}$ $Mathematical equation: $ \substack{0.57 \\ -0.50} $$
N2CO_1_166	N2CO J100015+020531	150.0630	2.0921	6.6	0.61 $\begin{matrix} 0.17 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.15} $$	5.4	1.72 $\begin{matrix} 0.56 \\ - 0.45 \end{matrix}$ $Mathematical equation: $ \substack{0.56 \\ -0.45} $$
N2CO_1_167	N2CO J100006+023306	150.0281	2.5519	4.8	0.48 $\begin{matrix} 0.19 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.19 \\ -0.15} $$	5.4	1.90 $\begin{matrix} 0.60 \\ - 0.51 \end{matrix}$ $Mathematical equation: $ \substack{0.60 \\ -0.51} $$
N2CO_1_170	N2CO J100057+021347	150.2373	2.2284	5.0	0.46 $\begin{matrix} 0.18 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.14} $$	5.3	1.71 $\begin{matrix} 0.54 \\ - 0.46 \end{matrix}$ $Mathematical equation: $ \substack{0.54 \\ -0.46} $$
N2CO_1_204	N2CO J100119+022617	150.3303	2.4385	4.7	0.50 $\begin{matrix} 0.20 \\ - 0.16 \end{matrix}$ $Mathematical equation: $ \substack{0.20 \\ -0.16} $$	4.8	1.81 $\begin{matrix} 0.67 \\ - 0.55 \end{matrix}$ $Mathematical equation: $ \substack{0.67 \\ -0.55} $$
N2CO_1_208	N2CO J100027+023344	150.1166	2.5632	5.2	0.54 $\begin{matrix} 0.21 \\ - 0.17 \end{matrix}$ $Mathematical equation: $ \substack{0.21 \\ -0.17} $$	4.8	1.67 $\begin{matrix} 0.62 \\ - 0.52 \end{matrix}$ $Mathematical equation: $ \substack{0.62 \\ -0.52} $$
N2CO_2_29b	N2CO J100001+022819	150.0083	2.4721	7.1	0.67 $\begin{matrix} 0.15 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.15 \\ -0.14} $$	–	–
N2CO_2_37	N2CO J100114+020208	150.3123	2.0356	6.6	0.71 $\begin{matrix} 0.20 \\ - 0.17 \end{matrix}$ $Mathematical equation: $ \substack{0.20 \\ -0.17} $$	–	< 2.71
N2CO_2_44	N2CO J095945+023438	149.9380	2.5773	6.3	0.79 $\begin{matrix} 0.22 \\ - 0.19 \end{matrix}$ $Mathematical equation: $ \substack{0.22 \\ -0.19} $$	–	< 2.92
N2CO_2_49	N2CO J100100+020923	150.2523	2.1566	6.1	0.57 $\begin{matrix} 0.16 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.14} $$	–	< 2.68
N2CO_2_61b	N2CO J095952+020544	149.9671	2.0957	5.5	0.53 $\begin{matrix} 0.16 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.16 \\ -0.14} $$	–	–
N2CO_2_76	N2CO J100042+020739	150.1759	2.1276	4.9	0.46 $\begin{matrix} 0.18 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.15} $$	–	< 2.24
N2CO_2_77	N2CO J095953+020734	149.9735	2.1261	4.9	0.45 $\begin{matrix} 0.18 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.14} $$	–	< 3.17
N2CO_2_85	N2CO J100059+022603	150.2489	2.4343	4.7	0.43 $\begin{matrix} 0.17 \\ - 0.14 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.14} $$	–	< 2.82
N2CO_2_88	N2CO J100050+022953	150.2103	2.4983	4.6	0.41 $\begin{matrix} 0.17 \\ - 0.13 \end{matrix}$ $Mathematical equation: $ \substack{0.17 \\ -0.13} $$	–	< 2.51
N2CO_2_90	N2CO J095944+022227	149.9346	2.3744	4.6	0.45 $\begin{matrix} 0.18 \\ - 0.15 \end{matrix}$ $Mathematical equation: $ \substack{0.18 \\ -0.15} $$	–	< 3.10

Notes. ^(b)These two 2-mm sources are complex blends with a slightly-offset bright 1.2 mm counterpart and potentially a fainter emission coming from the 2 mm object (see Carvajal- Bohorquez et al. in prep.). For this reason, we cannot provide an upper limit on their 1.2 mm flux.

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