Table 4
CIB anisotropy Cℓ, at 217, 353, 545, and 857 GHz in 
sr.
| ⟨ ℓ ⟩ | 202 | 388 | 583 | 784 | 985 | 1192 | 1431 | 1717 | 2060 |
| ℓmin | 80 | 280 | 480 | 680 | 880 | 1080 | 1296 | 1555 | 1866 |
| ℓmax | 280 | 480 | 680 | 880 | 1080 | 1296 | 1555.2 | 1866 | 2240 |
|
|
|||||||||
| 217 GHz | |||||||||
| Cℓ × 105 | 127.03 | 55.95 | 43.65 | 33.71 | 23.18 | 16.49 | 16.67 | 2.11 | 20.51 |
|
28.23 | 8.53 | 6.08 | 5.29 | 4.90 | 5.07 | 5.59 | 5.38 | 6.39 |
|
0.10 | 0.18 | 0.33 | 0.46 | 0.50 | 0.52 | 0.76 | 0.13 | 1.90 |
|
|
|||||||||
| 353 GHz | |||||||||
| Cℓ × 104 | 755.17 | 414.68 | 215.18 | 193.02 | 117.35 | 110.63 | 92.76 | 80.20 | 74.84 |
|
83.18 | 33.25 | 16.05 | 12.64 | 8.64 | 8.05 | 6.84 | 6.70 | 7.56 |
|
0.47 | 1.04 | 1.23 | 2.01 | 1.93 | 2.65 | 3.21 | 3.99 | 5.33 |
|
|
|||||||||
| 545 GHz | |||||||||
| Cℓ × 102 | 2246.54 | 1091.71 | 547.60 | 454.01 | 302.39 | 271.87 | 231.55 | 196.63 | 168.44 |
|
229.92 | 81.11 | 35.42 | 24.90 | 16.12 | 13.15 | 10.0 | 8.12 | 7.12 |
|
2.13 | 4.16 | 4.72 | 7.14 | 7.50 | 9.84 | 12.07 | 14.76 | 18.18 |
|
|
|||||||||
| 857 GHz | |||||||||
| Cℓ × 10-2 | 561.65 | 262.93 | 120.57 | 93.57 | 67.65 | 53.24 | 46.82 | 39.02 | 33.88 |
|
58.61 | 18.82 | 7.40 | 4.79 | 3.24 | 2.36 | 1.76 | 1.35 | 1.09 |
|
0.63 | 1.18 | 1.22 | 1.72 | 1.97 | 2.26 | 2.86 | 3.44 | 4.29 |
Notes. The conversion to Jy2sr-1 (with the photometric convention νIν = const.) involves multiplication by 231483, 83135, 3391.5 and 4.99 at 217, 353, 545, and 857 GHz, respectively. 
are the statistical errors; 
are the systematic errors introduced by the beam uncertainty (see Sect. 4.2.2).
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