Fig. 3.

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Ratio of the linear (solid lines) and non-linear (dashed lines) power spectra of several two-body DDM models to that of a pure ΛCDM model with the same cosmological parameters, parameterised by the fraction , the decay rate Γddm, and the fraction of energy ε going into the ultra-relativistic daughter particle at each decay. The parameters (
, Ωb, h, As, ns) are kept fixed, and the spectra are computed today (z = 0). The non-linear spectra are predicted by the emulator introduced in Sect. 3.3 and plotted up to the maximum wavenumber at which this emulator is trusted.
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