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Table 8.

Summary of a selection of the cases investigated for the weak-lensing code comparison, ordered according to the number of parameters involved.

Case No. of parameters Parameters
max
Flat Non-flat MG IA
1 5 Ωm, 0 Ωb, 0hnsσ8 1500 or 5000
2 6 Ωm, 0 Ωb, 0hnsσ8 ΩDE, 0 1500 or 5000
3 7 Ωm, 0 Ωb, 0w0wahnsσ8 1500 or 5000
4 8 Ωm, 0 Ωb, 0w0wahnsσ8 ΩDE, 0 1500 or 5000
5 8 Ωm, 0 Ωb, 0w0wahnsσ8 γ 1500 or 5000
6 9 Ωm, 0 Ωb, 0w0wahnsσ8 ΩDE, 0 γ 1500 or 5000
7 10 Ωm, 0 Ωb, 0w0wahnsσ8 𝒜IA ηIA βIA 1500 or 5000
8 11 Ωm, 0 Ωb, 0w0wahnsσ8 ΩDE, 0 𝒜IA ηIA βIA 1500 or 5000
9 11 Ωm, 0 Ωb, 0w0wahnsσ8 γ 𝒜IA ηIA βIA 1500 or 5000
10 12 Ωm, 0 Ωb, 0w0wahnsσ8 ΩDE, 0 γ 𝒜IA ηIA βIA 1500 or 5000

Notes. In non-flat cases, ΩDE, 0 is included as a free cosmological parameter (or equivalently ΩK, 0). The quantity max is the maximum multipole included in the analysis. MG corresponds to the modified gravity γ parameter (see Eq. (32)), changing the growth of structure. IA refers to intrinsic alignment parameters (discussed in Sect. 3.3.1).

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