Fig. 2

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Ratio to the ΛCDM (blue) model as a function of the smoothing mass M of the purely nonlinear rms fluctuations ℒ = σNL/σL for RPCDM (orange) and wCDM (green) models. In the internal panel, we plot, in the same way, the ratio to the ΛCDM model of the purely nonlinear power spectrum 𝒫 = PNL/PL of each model. We note that 𝒫RPCDM (orange) closely follows 𝒫ΛCDM (blue) up to kC = 0.4 h Mpc, after which it deviates significantly. For the wCDM model (green), the purely nonlinear spectra are very distinct above kC = 1. h Mpc. On the purely nonlinear ratios of rms fluctuations, the difference is strong on mass scales 1012−1014 M⊙/h. It is precisely this range of mass that we will study from the DM halos.
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