Table 3.
Results of the MCMC exploration with the three considered likelihoods: Like-F03, Like-F05, and Like-F06.
| Parameter | Like-F03 | Like-F05 | Like-F06 |
|---|---|---|---|
| ωbh2 | 0.02174 ± 0.00030 | 0.02225 ± 0.00027 | 0.02230 ± 0.00025 |
| ωch2 | 0.1210 ± 0.0033 | 0.1204 ± 0.0027 | 0.1189 ± 0.0025 |
| 100θMC | 1.04088 ± 0.00071 | 1.04082 ± 0.00057 | 1.04074 ± 0.00053 |
| ln(1010As) | 3.066 ± 0.037 | 3.072 ± 0.039 | 3.082 ± 0.037 |
| ns | 0.9548 ± 0.0089 | 0.9639 ± 0.0081 | 0.9704 ± 0.0073 |
| τ | 0.068 ± 0.019 | 0.075 ± 0.019 | 0.079 ± 0.019 |
| APS | 3.9 ± 3.4 | 15 ± 11 | 7.0 ± 5.6 |
| ACIB | 2.8 ± 2.4 | 1341 ± 8.6 | 5.7 ± 4.3 |
| Adust | 0.00013 ± 0.00011 | 0.0052 ± 0.00032 | 0.00031 ± 0.00020 |
| H0 | 66.5 ± 1.4 | 67.1 ± 1.2 | 67.6 ± 1.1 |
| Ωm | 0.325 ± 0.021 | 0.318 ± 0.017 | 0.311 ± 0.015 |
| ΩΛ | 0.675 ± 0.021 | 0.681 ± 0.017 | 0.690 ± 0.015 |
Notes. Constraints on parameters are given as marginal mean with 68% CL error on: main parameters (top), nuisance parameters (middle), and derived parameters (bottom). The Planck quoted values are obtained with Planck 2015 high-ℓ likelihood.
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