2017
DOI: 10.1140/epjc/s10052-016-4590-y
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Constraints on reconstructed dark energy model from SN Ia and BAO/CMB observations

Abstract: The motivation of the present work is to reconstruct a dark energy model through the dimensionless dark energy function X (z), which is the dark energy density in units of its present value. In this paper, we have shown that a scalar field φ having a phenomenologically chosen X (z) can give rise to a transition from a decelerated to an accelerated phase of expansion for the universe. We have examined the possibility of constraining various cosmological parameters (such as the deceleration parameter and the eff… Show more

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Cited by 67 publications
(43 citation statements)
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“…This explains both the observed growth of structures at the early times and the late time cosmic acceleration measurements. Also, the transition between the DM era and the THDE era takes place within the redshift interval [0.637,0.962], which are in good compatibility with several recent studies [81][82][83][84][85][86][87][88][89][90]. It is also observed that j stays positive and approaches to the CDM ( j = 1) model as z → −1.…”
Section: Discussionsupporting
confidence: 87%
See 1 more Smart Citation
“…This explains both the observed growth of structures at the early times and the late time cosmic acceleration measurements. Also, the transition between the DM era and the THDE era takes place within the redshift interval [0.637,0.962], which are in good compatibility with several recent studies [81][82][83][84][85][86][87][88][89][90]. It is also observed that j stays positive and approaches to the CDM ( j = 1) model as z → −1.…”
Section: Discussionsupporting
confidence: 87%
“…3. From this figure, it is clear that our model can describe the current accelerated universe, and the transition redshift z t (i.e., q(z t ) = 0) from the deceleration phase to an accelerated phase occurs within the intervals [0.637, 0.962] (for upper panel) and [0.776, 0.889] (for lower panel), which are in good agreement with the results, 0.5 < z t < 1, as reported in [81][82][83][84][85][86][87][88][89][90]. The evolution of j (z) has also been plotted in Fig.…”
Section: Interacting Thde With Hubble Cutoffsupporting
confidence: 90%
“…This approach is an excellent platform to study DE and indeed one may find several attempts in the literature. Specifically, one may use parametric criteria toward reconstructing directly the evolution of DE density ρ de (z) [50][51][52] and the potential of the scalar field [53]. 1 Comparing the two methods, namely w (z) and ρ de (z) for the same observational data sets, it has been found that the latter method leads to tighter constraints on the free parameters than the former [50][51][52].…”
Section: Introductionmentioning
confidence: 99%
“…V φ , ten different quintessence models are suggested by [36]. Here we start from Equation (12) in [37] where…”
Section: ϕCdm Cosmologymentioning
confidence: 99%