Abstract

We study the impact of Early Dark Energy fluctuations in the linear and non-linear regimes of structure formation. In these models the energy density of dark energy is non-negligible at high redshifts and the fluctuations in the dark energy component can have the same order of magnitude of dark matter fluctuations. Since two basic approximations usually taken in the standard scenario of quintessence models, that both dark energy density during the matter dominated period and dark energy fluctuations on small scales are negligible, are not valid in such models, we first study approximate analytical solutions for dark matter and dark energy perturbations in the linear regime. This study is helpful to find consistent initial conditions for the system of equations and to analytically understand the effects of Early Dark Energy and its fluctuations, which are also verified numerically. In the linear regime we compute the matter growth and variation of the gravitational potential associated with the Integrated Sachs-Wolf effect, showing that these observables present important modifications due to Early Dark Energy fluctuations, though making them more similar to the ΛCDM model. We also make use of the Spherical Collapse model to study the influence of Early Dark Energy fluctuations in the nonlinear regime of structure formation, especially on δc parameter, and their contribution to the halo mass, which we show can be of the order of 10%. We finally compute how the number density of halos is modified in comparison to the ΛCDM model and address the problem of how to correct the mass function in order to take into account the contribution of clustered dark energy. We conclude that the inhomogeneous Early Dark Energy models are more similar to the ΛCDM model than its homogeneous counterparts.

Highlights

  • Background evolutionWe assume a universe with flat spatial section, Dark Matter (DM) and DE

  • In this paper we have studied the influence of inhomogeneous Early Dark Energy (EDE) both in linear and nonlinear stages of structure formation

  • We have evaluated the matter growth, the Integrated Sachs-Wolfe effect (ISW) effect, the contribution of DE fluctuations for the total mass of the halos, the halo abundance relative to ΛCDM model and its corrections due the extra DE mass contribution

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Summary

Background evolution

We assume a universe with flat spatial section, DM (baryons are treated as dark matter) and DE. In this case the DE energy density is given by: ρe (a) = ρ0e exp a (1 + w (a )) da For both models we choose the amount of DE at early times to be Ωee 0.018, consistent with the limits presented in [17], the amounts of matter and DE are Ω0m = 0.25 and Ω0e = 0.75 and the DE equation of state now is w0 = −0.9. This quantity, which depends only on the background evolution is important for the study of cluster number counts, which in turn depends on perturbative properties via the mass function Note that both models of EDE that we are considering present a smaller volume ΛCDM model and that important differences appear only at high−z.

Linear evolution
Non-negligible ceff
Negligible ceff
Matter growth and ISW effect
Nonlinear evolution
Abundance of halos
Findings
Conclusions
Full Text
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