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We study the effects of Horndeski models of dark energy on the observables of the large-scale structure in the late time universe. A novel classification into {it Late dark energy}, {it Early dark energy} and {it Early modified gravity} scenarios is proposed, according to whether such models predict deviations from the standard paradigm persistent at early time in the matter domination epoch. We discuss the physical imprints left by each specific class of models on the effective Newton constant $mu$, the gravitational slip parameter $eta$, the light deflection parameter $Sigma$ and the growth function $fsigma_8$ and demonstrate that a convenient way to dress a complete portrait of the viability of the Horndeski accelerating mechanism is via two, redshift-dependent, diagnostics: the $mu(z)-Sigma(z)$ and the $fsigma_8(z)-Sigma(z)$ planes. If future, model-independent, measurements point to either $Sigma-1<0$ at redshift zero or $mu-1<0$ with $Sigma-1>0$ at high redshifts or $mu-1>0$ with $Sigma-1<0$ at high redshifts, Horndeski theories are effectively ruled out. If $fsigma_8$ is measured to be larger than expected in a $Lambda$CDM model at $z>1.5$ then Early dark energy models are definitely ruled out. On the opposite case, Late dark energy models are rejected by data if $Sigma<1$, while, if $Sigma>1$, only Early modifications of gravity provide a viable framework to interpret data.
We summarise the effective field theory of dark energy construction to explore observable predictions of linear Horndeski theories. Based on cite{Perenon:2016blf}, we review the diagnostic of these theories on the correlation of the large-scale struc
Shift-symmetric Horndeski theories admit an interesting class of Schwarzschild black hole solutions exhibiting time-dependent scalar hair. By making use of Lema^{i}tre coordinates, we analyze perturbations around these types of black holes, and demon
In this paper we show that an equivalence between Horndeski and beyond Horndeski theories and general relativity with an effective imperfect fluid can be formally established. The formal equivalence is discussed for several particular cases of intere
The Horndeski theories are extended into the Lovelock gravity theory. When the canonical scalar field is uniquely kinetically coupled to the Lovelock tensors, it is named after Lovelock scalar field. The Lovelock scalar field model is a subclass of t
We study certain bi-scalar-tensor theories emanating from conformal symmetry requirements of Horndeskis four-dimensional action. The former scalar is a Galileon with shift symmetry whereas the latter scalar is adjusted to have a higher order conforma