Planck 2018 results
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Table 9.

Additional noise in μK2 from systematic effects for three different multipole ranges ( = 4–5,  ≃ 100, and  ≃ 500).

Effect Procedure 30 GHz 44 GHz 70 GHz
= 45
  Gain smoothing error......... Simulations + odd-even years ≲3 × 10−3 (TT) ≲3 × 10−3 (TT) ≲3 × 10−3 (TT)
≲6 × 10−3 (EE) ≲6 × 10−3 (EE) ≲6 × 10−3 (EE)
  ADC......... Simulations + half-rings ≲1 × 10−4 (TT) ≲1 × 10−5 (TT) ≲1 × 10−5 (EE)
≲1 × 10−5 (EE) ≲1 × 10−6 (EE) ≲1 × 10−6 (EE)
  Full (4π beam + dipole params)......... Simulations + odd-even years ≲7 × 10−3 (TT) ≲4 × 10−3 (TT) ≲1 × 10−3 (TT)
≲1 × 10−2 (EE) ≲1 × 10−2 (EE) ≲6 × 10−3 (EE)
100
  Gain smoothing error......... Simulations + odd-even years ≲1 × 10−4 (TT) ≲1 × 10−4 (TT) ≲1 × 10−5 (TT)
≲1 × 10−4 (EE) ≲1 × 10−4 (EE) ≲1 × 10−4 (EE)
  ADC......... Simulations + half-rings ≲1 × 10−6 (TT) ≲1 × 10−6 (TT) ≲1 × 10−6 (TT)
≲1 × 10−7 (EE) ≲1 × 10−7 (EE) ≲1 × 10−7 (EE)
  Full (4π beam + dipole params)......... Simulations + odd-even years ≲1 × 10−4 (TT) ≲1 × 10−3 (TT) ≲3 × 10−5 (TT)
≲1 × 10−3 (EE) ≲6 × 10−4 (EE) ≲4 × 10−4 (EE)
500
  Gain smoothing error......... Simulations + odd-even years ≲1 × 10−5 (TT) ≲1 × 10−5 (TT) ≲1 × 10−5 (TT)
≲1 × 10−5 (EE) ≲1 × 10−5 (EE) ≲1 × 10−5 (EE)
  ADC......... Simulations + half-rings ≲1 × 10−6 (TT) ≲1 × 10−6 (TT) ≲1 × 10−6 (TT)
≲1 × 10−7 (EE) ≲1 × 10−7 (EE) ≲1 × 10−7 (EE)
  Full (4π beam + dipole params)......... Simulations + odd-even years ∼1 × 10−5 (TT) ≲6 × 10−5 (TT) ≲7 × 10−6 (TT)
≲3 × 10−4 (EE) ≲4 × 10−4 (EE) ≲2 × 10−4 (EE)

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