Table 13
For each of the four foreground cleaned maps, we compute fNL for the local, equilateral, and orthogonal modes using two different polarization masks, one with fsky = 0.74 and the other with fsky = 0.64, while for temperature we use a single mask with fsky = 0.76.
fsky = 0.74 | fsky = 0.64 | Difference | |||||||
Local | Equilateral | Orthogonal | Local | Equilateral | Orthogonal | Local | Equilateral | Orthogonal | |
|
|||||||||
SMICA | |||||||||
T .............. | 6.8 ± 5.4 | −17 ± 66 | −48 ± 33 | ... | ... | ... | ... | ... | ... |
E .............. | 25 ± 30 | 147 ± 159 | −137 ± 73 | 48 ± 31 | 220 ± 168 | −180 ± 81 | −23 ± 16 | −73 ± 68 | 43 ± 34 |
T+E .............. | 4.0 ± 4.8 | 5 ± 46 | −30 ± 21 | 4.6 ± 5.2 | 19 ± 55 | −37 ± 22 | −0.7 ± 1.2 | −14 ± 14 | 6.7 ± 7.7 |
SEVEM | |||||||||
T .............. | 8.1 ± 5.8 | −11 ± 75 | −49 ± 34 | ... | ... | ... | ... | ... | ... |
E .............. | 44 ± 38 | 302 ± 183 | −172 ± 91 | 43 ± 39 | 303 ± 191 | −170 ± 96 | 1 ± 19 | 0 ± 76 | −2 ± 49 |
T+E .............. | 6.4 ± 5.0 | 15 ± 52 | −44 ± 23 | 6.2 ± 5.3 | 31 ± 54 | −50 ± 25 | 0.2 ± 1.3 | −16 ± 15 | 6.3 ± 8.8 |
NILC | |||||||||
T .............. | 6.4 ± 5.8 | −31 ± 76 | −50 ± 33 | ... | ... | ... | ... | ... | ... |
E .............. | −1 ± 30 | 64 ± 162 | −78 ± 77 | 22 ± 30 | 190 ± 162 | −84 ± 77 | −23 ± 16 | −124 ± 67 | 6 ± 37 |
T+E .............. | 3.3 ± 4.9 | −15 ± 50 | −27 ± 23 | 4.0 ± 5.3 | 1 ± 56 | −33 ± 23 | −0.7 ± 1.3 | −16 ± 13 | 5.4 ± 7.5 |
Commander | |||||||||
T .............. | 6.4 ± 6.6 | −3 ± 77 | −49 ± 36 | ... | ... | ... | ... | ... | ... |
E .............. | 28 ± 37 | 278 ± 178 | −56 ± 81 | 61 ± 38 | 337 ± 188 | −122 ± 91 | −32 ± 20 | −60 ± 92 | 66 ± 47 |
T+E .............. | 5.2 ± 5.4 | 30 ± 50 | −39 ± 23 | 6.0 ± 5.7 | 45 ± 55 | −51 ± 25 | −0.7 ± 1.5 | −15 ± 14 | 11.5 ± 8.9 |
Notes. We then calculate the difference between the two measurements and compare with expectations from simulations, obtained in the following way: firstly, we generate realistic Gaussian realizations for each component separation pipeline, not including foregrounds; then, for each simulated map and NG model, we measure fNL using the two masks in turn; finally, we calculate the standard deviation on 100 realizations. See the main text for more details and a discussion of these results, which were obtained using the low resolution modal pipeline.
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