Constraints from growth-rate data on some coupled dark energy models mimicking a ΛCDMΛCDM expansion

preprint2016arXivOpen access

Abstract

The ΛCDMΛCDM expansion could be mimicked by a dark energy coupled to matter. Then, the equation of state wˉ\bar w and coupling Qˉ\bar Q of this coupled dark energy could not be constrained by observations of the Hubble function alone. Also, in this paper, we determine the constraints on two such coupled dark energy models considering some current and forecast Euclid-like growth-rate data and assuming the prior on the ΛCDMΛCDM dark matter density parameter today Ωm0=0.295±0.04Ω_{m0}=0.295\pm 0.04. The first model is defined by a constant equation of state. We find that at 2σ2σ, wˉ=−1.02−0.22+0.06\bar w=-1.02_{-0.22}^{+0.06} and the coupling function Qˉ0\bar Q_0 today is Qˉ0H0−3=0.057−0.148+0.353\bar Q_0H_0^{-3}=0.057_{-0.148}^{+0.353} with H0H_0 the Hubble constant. The second model is defined by a varying equation of state wˉ=wˉa−wˉbln⁡(1+z)\bar w=\bar w_a-\bar w_b\ln(1+z), with zz the redshift and (wˉa,wˉb)(\bar w_a,\bar w_b), two constants. We find that at 2σ2σ, wˉa=−0.99−0.90+0.17\bar w_a=-0.99_{-0.90}^{+0.17}, wˉb=−0.04−1.17+0.31\bar w_b=-0.04_{-1.17}^{+0.31} and Qˉ0H0−3=0.0002−0.18+1.35\bar Q_0H_0^{-3}=0.0002_{-0.18}^{+1.35}. These constraints on coupled dark energy agreed with a ΛCDMΛCDM model but are too poor to discard confidently a coupled dark energy different from vacuum but mimicking a ΛCDMΛCDM expansion.

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