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Table 3.

Parameter constraints for the base ΛCDM cosmology (as defined in Planck Collaboration XVI 2014), illustrating the impact of replacing the lowE likelihood with the lowE-S2 likelihood presented in the paper.

TT+lowE TT+lowE-S2 TTTEEE+lowE TTTEEE+lowE-S2
Parameter 68% Limits 68% Limits 68% Limits 68% Limits
Ωbh2 0.02212 ± 0.00022 0.02214 ± 0.00021 0.02236 ± 0.00015 0.02237 ± 0.00015
Ωch2 0.1206 ± 0.0021 0.1205 ± 0.0021 0.1202 ± 0.0014 0.1201 ± 0.0013
100θMC 1.04077 ± 0.00047 1.04080 ± 0.00047 1.04090 ± 0.00031 1.04090 ± 0.00031
τ 0.0522 ± 0.0080
ln(1010As) 3.040 ± 0.016 3.051 ± 0.013 3.045 ± 0.016 3.054 ± 0.013
ns 0.9626 ± 0.0057 0.9631 ± 0.0056 0.9649 ± 0.0044 0.9651 ± 0.0043

H0 66.88 ± 0.92 66.95 ± 0.90 67.27 ± 0.60 67.32 ± 0.60
Ωm 0.321 ± 0.013 0.320 ± 0.013 0.3166 ± 0.0084 0.3158 ± 0.0082
ΩΛ 0.679 ± 0.013 0.680 ± 0.013 0.6834 ± 0.0084 0.6842 ± 0.0082
σ8 0.8118 ± 0.0089 0.8155 ± 0.0083 0.8120 ± 0.0073 0.8154 ± 0.0067
zre 7.50 ± 0.82 8.04 ± 0.60 7.68 ± 0.79 8.14 ± 0.60
109As 2.092 ± 0.034 2.113 ± 0.028 2.120 ± 0.028
109Ase−2τ 1.884 ± 0.014 1.884 ± 0.014 1.884 ± 0.012 1.884 ± 0.012
Age/Gyr 13.830 ± 0.037 13.827 ± 0.036 13.800 ± 0.024 13.798 ± 0.024

Notes. We also show the change when including the high-ℓ polarization.

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