Table 2.
Scaling of different large-scale-structure probes with σ8 and Ωm.
| σ8 | Ωm | |
|---|---|---|
| Faraday rotation power spectrum at ℓ ≃ 104 | 2.1 | −0.1 |
| Faraday conversion power spectrum at ℓ ≃ 104 (thermal electrons) | 2.1 | −0.1 |
| Faraday conversion power spectrum at ℓ ≃ 104 (relativistic electrons) | 2.1 | 1 |
| Halo number counts from thermal SZ | 9 | 3 |
| Thermal SZ power spectrum at ℓ ≃ 3000 | 8.1 | 3.2 |
| CMB lensing power spectrum at ℓ ≃ 30 | 2 | 0.5 |
Notes. The scaling reported is to be understood as 
with P any of the considered probe. These values are given at the peaking multipole of ℓ(ℓ + 1)Cℓ for the Faraday rotation angle, the Faraday conversion rate, the tSZ flux, and the peaking multipole of 
for the lensing potential.
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