2015
DOI: 10.1103/physrevd.91.064029
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Dark energy and equation of state oscillations with collisional matter fluid in exponential modified gravity

Abstract: We study some aspects of cosmological evolution in a universe described by a viable curvature corrected exponential F (R) gravity model, in the presence of matter fluids consisting of collisional matter and radiation. Particularly, we express the FriedmannRobertson-Walker equations of motion in terms of parameters that are appropriate for describing the dark energy oscillations and compare the dark energy density and the dark energy equation of state parameter corresponding to collisional and noncollisional ma… Show more

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Cited by 26 publications
(15 citation statements)
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“…Namely, that of dark energy oscillations [395] (see also e.g. [396][397][398][399]). The degree of freedom associated to the modification of GR (that is, dF (R)/dR) leads to high frequency oscillations of the dark energy around the line of the phantom divide during matter era.…”
Section: Late-time Evolution In Mimetic Gravitymentioning
confidence: 99%
“…Namely, that of dark energy oscillations [395] (see also e.g. [396][397][398][399]). The degree of freedom associated to the modification of GR (that is, dF (R)/dR) leads to high frequency oscillations of the dark energy around the line of the phantom divide during matter era.…”
Section: Late-time Evolution In Mimetic Gravitymentioning
confidence: 99%
“…Also there are other modified gravity theories namely scalar tensor theory, Brane world scenario, f (G), f (R, G) and f (R) gravity theories, where R is the Ricci scalar, G = R μνρλ R μνρλ − R μν R μν + R 2 is the Gauss Bonnet invariant term and R μνρλ and R μν are the usual Riemann curvature tensor and Ricci tensor respectively. These modified theories (Sotiriou and Faraoni 2010;Nojiri and Odintsov 2003Capozziello 2002;Starobinsky 1980;Kerner 1982;Barrow and Ottewi 1983;Faraoni 2006;Schmidt 2007;Mitra et al 2014;Carroll et al 2004;Capozziello et al 2006;Nojiri et al 2009;Oikonomou et al 2015) are considered as gravitational alternatives for DE and may serve as dark matter (Sobouti 2007).…”
Section: Introductionmentioning
confidence: 98%
“…where Λ = 7.93m 2 ,γ = 1/1000, m = 1.57 × 10 −67 eV, b is an arbitrary parameter [43,44,56] and n is a positive real parameter. This model has quite appealing inflationary dynamics in the context of constant-roll inflation, as we now evince.…”
Section: Constant-roll Evolution With Curvature-corrected Exponentialmentioning
confidence: 99%
“…Actually, by solving the differential equation (III.12) numerically we will be able to find how the dark energy oscillations behave at late-times, so for small redshifts. For our numerical analysis we shall use the following initial conditions [43,44,[54][55][56],…”
Section: A the Radiation Matter Domination Eras And Transition To Lmentioning
confidence: 99%