Table 4
Compressed likelihood discussed in Sect. 5.1.6.
| Smooth DE models | Planck TT+lowP | R | ℓA | Ωbh2 | ns |
|
|
|||||
| R .......................... | 1.7488 ± 0.0074 | 1.0 | 0.54 | −0.63 | −0.86 |
| ℓ A .......................... | 301.76 ± 0.14 | 0.54 | 1.0 | −0.43 | −0.48 |
| Ωbh2 .......................... | 0.02228 ± 0.00023 | −0.63 | −0.43 | 1.0 | 0.58 |
| n s .......................... | 0.9660 ± 0.0061 | −0.86 | −0.48 | 0.58 | 1.0 |
|
|
|||||
| Marginalized over AL | Planck TT+lowP | R | ℓ A | Ωbh2 | n s |
|
|
|||||
| R .......................... | 1.7382 ± 0.0088 | 1.0 | 0.64 | −0.75 | −0.89 |
| ℓ A .......................... | 301.63 ± 0.15 | 0.64 | 1.0 | −0.55 | −0.57 |
| Ωbh2 .......................... | 0.02262 ± 0.00029 | −0.75 | −0.55 | 1.0 | 0.71 |
| n s .......................... | 0.9741 ± 0.0072 | −0.89 | −0.57 | 0.71 | 1.0 |
Notes. The left columns give the marginalized mean values and standard deviation for the parameters of the compressed likelihood for Planck TT+lowP, while the right columns present the normalized covariance or correlation matrix D for the parameters of the compressed likelihood for Planck TT+lowP. The covariance matrix C is then given by Cij = σiσjDij (without summation), where σi is the standard deviation of parameter i. While the upper values were derived for wCDM and are consistent with those of ΛCDM and the { w0,wa } model, we marginalized over the amplitude of the lensing power spectrum for the lower values, which leads to a more conservative compressed likelihood.
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