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Fig. 6.

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Effect of 1b-DDM parameters on the linear (solid) and non-linear (dashed) matter power spectrum. Left: Effect of varying the decay rate Γddm with a fixed fraction f ddm ini = 1 $ f_{\mathrm{ddm}}^{\mathrm{ini}} = 1 $. Right: Effect of varying the fraction f ddm ini $ f_{\mathrm{ddm}}^{\mathrm{ini}} $ with a fixed decay rate Γddm = (1/13.5) Gyr−1. The other parameters ( Ω dm ini $ \Omega_{\mathrm{dm}}^{\mathrm{ini}} $, Ωb, h, As, ns) are kept fixed, and the spectra are computed today (z = 0). Dashed lines show the predictions of the emulator of Hubert et al. (2021). Our pipeline relies on the prescription of Eq. (16), shown as a dotted line, which smoothly interpolates from the linear to non-linear behaviour.

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