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Table 1.

Differential number counts computed in different regions and overall cumulative number counts with corresponding overdensities.

Region S850 μm dN/dS S850 μm N(> S′) δ
(mJy) (deg−2 mJy−1) (mJy) (deg−2)
r < 4′ 2–5 1052.0 267.8 + 289.1 $ ^{+289.1}_{-267.8} $ 2 2716.0 549.0 + 602.6 $ _{-549.0}^{+602.6} $ 0.1 0.2 + 0.2 $ ^{+0.2}_{-0.2} $
5–8 195.8 53.4 + 54.0 $ ^{+54.0}_{-53.4} $ 3 1123.5 161.0 + 176.5 $ _{-161.0}^{+176.5} $ 0.1 0.1 + 0.2 $ ^{+0.2}_{-0.1} $
8–11 47.3 47.3 + 24.4 $ ^{+24.4}_{-47.3} $ 4 625.6 63.3 + 74.5 $ _{-63.3}^{+74.5} $ 0.2 0.1 + 0.2 $ ^{+0.2}_{-0.1} $
11–14 3.6 3.6 + 3.6 $ ^{+3.6}_{-3.6} $ 5 425.3 51.1 + 46.2 $ _{-51.1}^{+46.2} $ 0.6 0.2 + 0.1 $ ^{+0.1}_{-0.2} $

4′≤r < 9′ 2–5 533.8 249.1 + 218.9 $ ^{+218.9}_{-249.1} $ 6 273.5 43.0 + 43.6 $ _{-43.0}^{+43.6} $ 0.8 0.3 + 0.3 $ ^{+0.3}_{-0.3} $
5–8 93.7 24.9 + 28.6 $ ^{+28.6}_{-24.9} $ 7 163.5 35.2 + 31.9 $ _{-35.2}^{+31.9} $ 0.9 0.4 + 0.4 $ ^{+0.4}_{-0.4} $
8–11 27.0 11.4 + 13.9 $ ^{+13.9}_{-11.4} $ 8 95.8 27.1 + 26.3 $ _{-27.1}^{+26.3} $ 1.0 0.5 + 0.6 $ ^{+0.6}_{-0.5} $
11–14 8.7 8.7 + 9.0 $ ^{+9.0}_{-8.7} $ 9 55.2 25.5 + 17.2 $ _{-25.5}^{+17.2} $ 1.1 1.0 + 0.6 $ ^{+0.6}_{-1.0} $

r < 9′ 2–5 1045.2 260.7 + 306.1 $ ^{+306.1}_{-260.7} $ 10 32.1 18.0 + 10.3 $ _{-18.0}^{+10.3} $ 1.2 1.2 + 0.7 $ ^{+0.7}_{-1.2} $
5–8 130.9 24.9 + 21.9 $ ^{+21.9}_{-24.9} $ 11 16.5 16.5 + 11.8 $ _{-16.5}^{+11.8} $ 0.9 1.9 + 1.4 $ ^{+1.4}_{-1.9} $
8–11 31.8 11.8 + 10.5 $ ^{+10.5}_{-11.8} $ 12 4.3 4.3 + 9.9 $ _{-4.3}^{+9.9} $ –0.2 0.8 + 1.8 $ ^{+1.8}_{-0.8} $
11–14 7.6 7.6 + 6.5 $ ^{+6.5}_{-7.6} $ 13 1.2 1.2 + 1.2 $ ^{+1.2}_{-1.2} $ –0.6 0.4 + 0.3 $ ^{+0.3}_{-0.4} $

Notes. Uncertainties are the standard deviation of the number counts in each flux bin after 5000 realizations with de-boosting process following the Gaussian probability distributions described in Sect. 4.1. Due to the limited area, we calculated the average differential number counts across 3 mJy.

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