Table 7.
Results for fNL for local isocurvature NG determined from the SMICA Planck 2018 map with the Binned bispectrum estimator.
Independent |
Joint |
|||||
---|---|---|---|---|---|---|
Shape | Cold dark matter | Neutrino density | Neutrino velocity | Cold dark matter | Neutrino density | Neutrino velocity |
T a,aa…… | −0.1 ± 5.6 | −0.1 ± 5.6 | −0.1 ± 5.6 | 15 ± 16 | −15 ± 54 | −29 ± 49 |
T a,ai…… | −3 ± 11 | −6 ± 16 | 27 ± 29 | −30 ± 31 | 87 ± 220 | 310 ± 360 |
T a,ii…… | 440 ± 950 | −150 ± 290 | 480 ± 360 | 11000 ± 8500 | −1800 ± 4500 | −1100 ± 3800 |
T i,aa…… | 33 ± 53 | 0.3 ± 9.2 | −0.1 ± 4.9 | 95 ± 120 | 46 ± 110 | −27 ± 49 |
T i,ai…… | 28 ± 67 | −9 ± 23 | 14 ± 21 | −1300 ± 1000 | −32 ± 670 | 98 ± 170 |
T i,ii…… | 110 ± 280 | −130 ± 250 | 270 ± 230 | 2500 ± 2000 | −140 ± 2600 | −1000 ± 1400 |
E a,aa…… | 48 ± 26 | 48 ± 26 | 48 ± 26 | 25 ± 42 | −60 ± 120 | 43 ± 130 |
E a,ai…… | 140 ± 91 | 170 ± 98 | 72 ± 51 | 28 ± 150 | 330 ± 590 | 280 ± 370 |
E a,ii…… | 100 ± 2500 | 2000 ± 1500 | 310 ± 460 | −8100 ± 4400 | −9400 ± 5500 | −6100 ± 2800 |
E i,aa…… | 110 ± 77 | 75 ± 34 | 31 ± 21 | 43 ± 140 | 90 ± 170 | −94 ± 120 |
E i,ai…… | 330 ± 180 | 210 ± 100 | 43 ± 35 | 830 ± 580 | 500 ± 890 | 460 ± 360 |
E i,ii…… | 1800 ± 1200 | 1900 ± 1100 | 170 ± 230 | −1400 ± 2300 | −1300 ± 4800 | −380 ± 1000 |
T+E a,aa…… | −2.5 ± 5.0 | −2.5 ± 5.0 | −2.5 ± 5.0 | 4 ± 10 | −53 ± 28 | 2 ± 26 |
T+E a,ai…… | −10 ± 10 | −14 ± 14 | −1 ± 21 | −14 ± 21 | 160 ± 110 | 250 ± 110 |
T+E a,ii…… | −450 ± 520 | −350 ± 260 | −56 ± 210 | −3100 ± 1500 | −4100 ± 1600 | −2100 ± 920 |
T+E i,aa…… | 20 ± 28 | −0.5 ± 8.0 | −3.5 ± 4.2 | 96 ± 52 | 44 ± 49 | −37 ± 26 |
T+E i,ai…… | −32 ± 46 | −18 ± 20 | −7 ± 14 | 190 ± 180 | 350 ± 240 | 23 ± 77 |
T+E i,ii…… | −290 ± 210 | −340 ± 210 | −51 ± 110 | −640 ± 400 | −2000 ± 990 | 38 ± 300 |
Notes. In each case the adiabatic mode is considered together with one isocurvature mode (either cold-dark-matter, neutrino-density, or neutrino-velocity isocurvature). As explained in the text this gives six different fNL parameters, indicated by the different combinations of the adiabatic (a) and isocurvature (i) modes. Results are shown for both an independent and a fully joint analysis, for T-only, E-only, and full T+E data. In all cases the lensing bias has been subtracted.
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