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Planck 2018 results
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Table C.3.

Parameters of spectral model fit in Sect. 4 for B modes.

LR24 LR33 LR42 LR52 LR62 LR71
ℓ range Ad [μK2]
4–11...... 36 ± 3 78 ± 4 359 ± 5 506 ± 4
12–19...... 29 ± 2 43 ± 2 116 ± 3 158 ± 3 422 ± 4
20–39...... 31 ± 1 43 ± 1 89 ± 1 134 ± 2 183 ± 2 398 ± 2
40–59...... 19 ± 1 25 ± 1 53 ± 1 86 ± 2 137 ± 2 241 ± 2
60–79...... 14 ± 1 19 ± 1 35 ± 1 68 ± 2 108 ± 2 170 ± 2
80–99...... 17 ± 1 19 ± 1 36 ± 2 58 ± 2 97 ± 2 173 ± 2
100–119...... 14 ± 2 18 ± 2 31 ± 2 54 ± 2 92 ± 2 167 ± 2
120–139...... 18 ± 2 29 ± 2 52 ± 3 131 ± 3
140–159...... 9 ± 3 23 ± 2 46 ± 3 74 ± 3 122 ± 3
As (μK2)
4–11...... 6.7 ± 0.3 8.8 ± 0.2 9.7 ± 0.2 12.4 ± 0.2 10.8 ± 0.2 9.9 ± 0.2
12–19...... 1.5 ± 0.2 0.9 ± 0.1 1.4 ± 0.1 2.7 ± 0.1 6.1 ± 0.2
20–39...... 0.4 ± 0.1 0.4 ± 0.1 1.0 ± 0.1 0.7 ± 0.1 1.2 ± 0.1 3.2 ± 0.1
40–59...... 0.0 ± 0.1 0.3 ± 0.1 0.2 ± 0.1 0.6 ± 0.1 1.7 ± 0.1
60–79...... 0.0 ± 0.1 0.0 ± 0.1 0.0 ± 0.1 0.0 ± 0.1 0.0 ± 0.2 0.6 ± 0.2
80–99...... 0.0 ± 0.2 0.0 ± 0.2 0.0 ± 0.2 0.0 ± 0.1 0.0 ± 0.3 0.5 ± 0.2
100 –119...... 0.0 ± 0.2 0.0 ± 0.3 0.0 ± 0.4 0.6 ± 0.3 0.9 ± 0.3
120–139...... 0.0 ± 0.3 0.0 ± 0.2 0.0 ± 0.2 0.0 ± 0.2 0.0 ± 0.3 0.0 ± 0.4
140–159...... 0.0 ± 0.5 0.0 ± 0.6 0.0 ± 0.6 0.0 ± 0.4 0.0 ± 0.4 0.0 ± 0.3
βd
4–11...... 1.68 ± 0.07 1.60 ± 0.04 1.54 ± 0.03 1.55 ± 0.02
12–19...... 1.53 ± 0.04 1.61 ± 0.04 1.57 ± 0.03 1.53 ± 0.02
20–39...... 1.53 ± 0.06 1.51 ± 0.03 1.53 ± 0.03 1.55 ± 0.03 1.56 ± 0.02
40–59...... 1.58 ± 0.1 1.51 ± 0.05 1.48 ± 0.04 1.50 ± 0.03 1.54 ± 0.02
60–79...... 1.22 ± 0.14 1.4 ± 0.13 1.52 ± 0.08 1.51 ± 0.05 1.52 ± 0.03
80–99...... 1.50 ± 0.19 1.42 ± 0.09 1.46 ± 0.06 1.49 ± 0.04 1.52 ± 0.03
100–119...... 1.56 ± 0.13 1.56 ± 0.08 1.54 ± 0.05 1.50 ± 0.03
120–139...... 1.80 ± 0.19 1.66 ± 0.06
140–159...... 1.37 ± 0.10 1.48 ± 0.07 1.53 ± 0.05
βs
4–11...... −3.13 ± 0.08 −3.10 ± 0.06 −3.18 ± 0.04 −3.14 ± 0.04
12–19...... −3.26 ± 0.17 −3.17 ± 0.18 −3.44 ± 0.16 −3.32 ± 0.10 −3.13 ± 0.08
20–39...... −3.14 ± 0.18 −3.12 ± 0.16 −3.04 ± 0.17 −2.95 ± 0.15
40–59...... −3.11 ± 0.18 −3.11 ± 0.18 −3.12 ± 0.18
60–79...... −3.08 ± 0.18 −3.09 ± 0.18
80–99...... −3.11 ± 0.18 −3.12 ± 0.18 −3.12 ± 0.18 −3.11 ± 0.18 −3.12 ± 0.18 −3.12 ± 0.18
100–119...... −3.11 ± 0.18 −3.11 ± 0.19 −3.13 ± 0.18 −3.15 ± 0.18
120–139...... −3.11 ± 0.18 −3.12 ± 0.18 −3.11 ± 0.18 −3.10 ± 0.18
140–159...... −3.11 ± 0.18 −3.11 ± 0.18 −3.11 ± 0.18 −3.12 ± 0.18 −3.11 ± 0.18
ρ
4–11...... 0.39 ± 0.04 0.55 ± 0.02 0.55 ± 0.01 0.69 ± 0.01 0.67 ± 0.01 0.48 ± 0.01
12–19...... −0.13 ± 0.05 −0.13 ± 0.06 0.42 ± 0.04 0.41 ± 0.02 0.49 ± 0.02 0.24 ± 0.01
20–39...... 0.30 ± 0.03 0.28 ± 0.02 0.33 ± 0.01
40–59...... 0.02 ± 0.07 0.17 ± 0.04 0.20 ± 0.02
60–79...... 0.45 ± 0.32
80–99...... −0.01 ± 0.24 −0.01 ± 0.2 0.05 ± 0.05
100–119......
120–139......
140–159......
χ2(Nd.o.f. = 23)
4–11...... 19.7 14.1 4.4 12.2 12.7 24.1
12–19...... 23.1 14.1 35.0 17.6 19.2 43.3
20–39...... 21.5 23.5 19.4 24.7 24.3 31.8
40–59...... 24.4 10.9 10.9 11.1 9.7 8.8
60–79...... 18.8 25.5 19.5 20.5 16.8 14.4
80–99...... 22.4 13.4 16.3 18.3 16.1 20.1
100–119...... 29.8 34.7 40.3 45.5 53.7 46.5
120–139...... 21.5 18.2 23.0 27.7 27.7 30.0
140–159...... 27.2 31.4 29.8 34.8 34.0 32.4

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