Planck 2015 results
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Table E.1

Goodness-of-fit tests for the 2015 Planck temperature and polarization spectra.

Frequency [GHz] Multipole rangea χ 2 b χ2/N N d PTE [%] d

TT
  100 × 100 ..................... 30–1197 1234.37 1.06 1168 1.37 8.7
  143 × 143 ..................... 30–1996 2034.45 1.03 1967 1.08 14.1
  143 × 217 ..................... 30–2508 2566.74 1.04 2479 1.25 10.7
  217 × 217 ..................... 30–2508 2549.66 1.03 2479 1.00 15.8
Combined TT ..................... 30–2508 2546.67 1.03 2479 0.96 16.8
TE
  100 × 100 ..................... 30–999 1088.78 1.12 970 2.70 0.5
  100 × 143 ..................... 30–999 1032.84 1.06 970 1.43 7.9
  100 × 217 ..................... 505–999 526.56 1.06 495 1.00 15.8
  143 × 143 ..................... 30–1996 2028.43 1.03 1967 0.98 16.4
  143 × 217 ..................... 505–1996 1606.25 1.08 1492 2.09 2.0
  217 × 217 ..................... 505–1996 1431.52 0.96 1492 –1.11 86.7
Combined TE ..................... 30–1996 2046.11 1.04 1967 1.26 10.5
EE
  100 × 100 ..................... 30–999 1027.89 1.06 970 1.31 9.6
  100 × 143 ..................... 30–999 1048.22 1.08 970 1.78 4.1
  100 × 217 ..................... 505–999 479.72 0.97 495 –0.49 68.1
  143 × 143 ..................... 30–1996 2000.90 1.02 1967 0.54 29.2
  143 × 217 ..................... 505–1996 1431.16 0.96 1492 –1.11 86.8
  217 × 217 ..................... 505–1996 1409.58 0.94 1492 –1.51 93.6
Combined EE ..................... 30–1996 1986.95 1.01 1967 0.32 37.2

Notes.

(a)

The range used in the high- likelihood.

(b)

The χ2 are with respect to the best-fit from the Plik TT+lowTEB data combination in a ΛCDM framework.

(c)

Δχ2 = χ2N is the difference from the mean assuming that the best-fit base TTΛCDM model is correct, expressed in units of the expected dispersion, .

(d)

Probability to exceed the tabulated value of χ2.

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