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Table 4

Resolutions, RMS noises, and source densities of each individual facet.

0.3″ 0.6″ 1.2″



Facet Resolution (arcsec2) RMS (μJy beam−1) ρ (degree−2) Resolution (arcsec2) RMS (μJy beam−1) ρ (degree−2) Resolution (arcsec2) RMS (μJy beam−1) ρ (degree−2)
1 0.36×0.45 29 668 0.61×0.67 37 797 1.25×2.74 60 668
2 0.35×0.42 21 1278 0.58×0.63 29 1388 1.09×2.03 56 943
3 0.34×0.40 20 1824 0.56×0.61 27 1824 1.05×1.71 50 1450
4 0.34×0.41 20 1491 0.57×0.62 28 1336 1.06×1.81 49 1052
5 0.34×0.41 19 1594 0.57×0.62 26 1403 1.05×1.78 51 989
6 0.34×0.41 19 1596 0.57×0.62 27 1500 1.06×1.87 47 1093
7 0.35×0.42 22 928 0.58×0.63 30 877 1.06×1.97 54 577
8 0.36×0.43 28 718 0.62×0.65 36 778 1.15×2.51 62 692
9 0.35×0.43 22 875 0.58×0.64 30 967 1.08×2.11 55 611
10 0.34×0.41 18 1615 0.56×0.61 25 1456 1.04×1.68 47 1023
11 0.33×0.39 15 2118 0.55×0.59 22 1764 1.02×1.45 48 900
12 0.33×0.39 16 2281 0.55×0.60 22 1811 1.02×1.52 41 1057
13 0.34×0.40 17 1843 0.56×0.61 25 1740 1.03×1.63 44 1214
14 0.34×0.42 21 1435 0.57×0.62 28 1373 1.05×1.78 56 1071
15 0.34×0.40 16 1860 0.55×0.60 22 1571 1.02×1.53 41 1062
16 0.33×0.38 14 2071 0.54×0.59 21 1678 1.00×1.40 40 912
17 0.33×0.39 15 1983 0.55×0.59 21 1721 1.01×1.48 39 1132
18 0.34×0.41 20 1269 0.57×0.62 27 1218 1.04×1.78 49 860
19 0.35×0.43 25 1115 0.59×0.64 33 1158 1.09×2.14 58 974
20 0.35×0.42 21 1203 0.58×0.63 28 1239 1.06×1.92 49 848
21 0.34×0.40 17 1942 0.55×0.60 24 1733 1.02×1.54 43 1152
22 0.33×0.38 15 2315 0.55×0.59 21 1966 1.00×1.41 41 1145
23 0.33×0.40 17 1826 0.56×0.61 24 1756 1.03×1.60 44 1178
24 0.35×0.42 21 863 0.58×0.63 30 1052 1.05×1.94 52 821
25 0.34×0.40 19 1573 0.56×0.61 26 1433 1.03×1.63 51 948
26 0.35×0.42 20 1365 0.57×0.63 27 1455 1.07×2.01 54 997
27 0.35×0.43 28 712 0.60×0.64 37 785 1.12×2.32 63 630
28 0.35×0.42 24 1044 0.58×0.63 32 1121 1.09×2.11 58 742
29 0.36×0.45 28 679 0.56×0.61 38 658 1.28×2.82 71 679
30 0.35×0.44 28 734 0.60×0.66 36 824 1.14×2.50 61 657

Notes. The facet numbers correspond to the numbers in Fig. 14. The source density (ρ) is based on the catalogues after cleaning our source detections, as discussed in Sec. 5.

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