Table 2.
Parameters considered in the joint analysis of stacked weak lensing and counts.
| Parameter | Description | Prior | Posterior |
|---|---|---|---|
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Cold dark matter density parameter at z = 0 | [0.1, 0.4] |
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| 109As | Amplitude of the primordial matter power spectrum | [0.8, 8] |
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| Ωm | Total matter density parameter at z = 0 | – |
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| σ8 | Amplitude of the matter power spectrum at z = 0 | – |
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| S8 ≡ σ8(Ωm/0.3)0.5 | Clustering amplitude | – |
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| Ωb | Baryon density parameter at z = 0 | 𝒩(0.0493, 0.0016) | – |
| ns | Primordial power spectrum spectral index | 𝒩(0.9649, 0.0210) | – |
| h ≡ H0/(100 km/s/Mpc) | Normalised Hubble constant | 𝒩(0.7, 0.03) | – |
| α | Amplitude of the log λ* − log M200 relation | [−2, 2] |
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| β | Slope of the log λ* − log M200 relation | [0, 3] |
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| γ | Redshift evolution of the log λ* − log M200 relation | [−3, 3] |
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| σintr | Intrinsic scatter of the log λ* − log M200 relation | [0.01, 0.5] |
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| log c0 | Amplitude of the log c200 − log M200 relation | [0, 1.3] |
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| foff | Fraction of miscentred clusters | 𝒩(0.3, 0.1) | – |
| σoff | Miscentring scale (in h−1 Mpc) | [0, 0.5] |
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| Ft | Truncation factor of the BMO density profile | 𝒩(3, 0.5) | – |
| (s, q) | Parameters entering the mass function correction factor |
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– |
Notes. In the first and second columns we list the symbols and descriptions of the parameters, respectively. The third column reports the priors on the parameters, and in particular a range represents a uniform prior, while 𝒩(μ, σ) stands for a Gaussian prior with mean μ and standard deviation σ. In the fourth column, we show the median values of the 1D marginalised posteriors, along with the 16th and 84th percentiles. The posterior is not reported in cases where it closely aligns with the prior.
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