Table 4.
Priors on the cosmological and non-cosmological parameters used in our analysis.
| Cosmological parameters | |
|---|---|
| q∥ | 𝒰[0.8, 1.2] |
| q⊥ | 𝒰[0.8, 1.2] |
| f/ffid | 𝒰[0.0, 2.0] |
| dm | 𝒰[−3, 3] |
| Non-cosmological parameters | |
| (1 + b1)σ8 | 𝒰[0, 3] |
| b2σ82 | 𝒩[0, 52] |
| bsσ82 | 𝒩[0, 52] |
| α0 | 𝒩[0, 12.52] |
| α2 | 𝒩[0, 12.52] |
| α4 | 𝒩[0, 12.52] |
| sn0 |
![]() |
| sn2 |
![]() |
| sn4 |
![]() |
Notes. Here, 𝒰 stands for a uniform prior and 𝒩(μ, σ2) for a Gaussian prior with mean μ and variance σ2. The cosmological parameters are listed in the top subpanel and the non-cosmological parameters are listed in the bottom subpanel. For the stochastic parameters, the prior width on sn0 is scaled by the Poissonian shot-noise (
), while the prior widths for sn2 and sn4 are scaled by the expected fraction of satellite galaxies, the effective velocity dispersion of the satellites, and the Poissonian shot-noise:
,
, respectively (see Maus et al. (2024) for details).
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