2017
DOI: 10.1103/physrevd.96.103505
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Study of the observational compatibility of an inhomogeneous cosmology with linear expansion according to SNe Ia

Abstract: Most of current cosmological theories are built combining an isotropic and homogeneous manifold with a scale factor that depends on time. If one supposes a hyperconical universe with linear expansion, an inhomogeneous metric can be obtained by an appropriate transformation that preserves the proper time. This model locally tends to a flat Friedman-Robertson-Walker metric with linear expansion. The objective of this work is to analyse the observational compatibility of the inhomogeneous metric considered. For t… Show more

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Cited by 6 publications
(42 citation statements)
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“…For example, hyperconical universes produce inhomogeneous metrics compatible with the observed expansion and they locally approach to the flat FRW metric. To be consistent with the ΛCDM model, it can be assumed as a local perturbation theory in inhomogeneous universes expanding regardless of the matter content [7]. On the other hand, physical properties of inhomogeneous spaces are interesting because they can be used to trace dark energy and dark matter [8].…”
Section: A1 Motivationmentioning
confidence: 99%
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“…For example, hyperconical universes produce inhomogeneous metrics compatible with the observed expansion and they locally approach to the flat FRW metric. To be consistent with the ΛCDM model, it can be assumed as a local perturbation theory in inhomogeneous universes expanding regardless of the matter content [7]. On the other hand, physical properties of inhomogeneous spaces are interesting because they can be used to trace dark energy and dark matter [8].…”
Section: A1 Motivationmentioning
confidence: 99%
“…Metric. From the above hypotheses, a radially inhomogeneous metric g is obtained with the same local Ricci curvature as the flat FRW metric [7]. The nonzero elements in comoving polar coordinates (t, r , θ, φ) are g 00 = 2k −1 (b−1)+1, g r r = −a 2 /b 2 , g 0r = −ar /tôb, g θθ = −a 2 r 2 and g φφ = −a 2 r 2 sin 2 θ; where k −1 := 1 − β 2 ± is the spatial curvature, a(t) := t/tô is the scale factor and b(r ) 2 := 1 − kr 2 /t 2 o is an auxiliary function.…”
Section: B Hyperconical Universesmentioning
confidence: 99%
“…The aim of this paper is to analyse the symmetry properties of a radially inhomogeneous hyperconical model according to the Killing vectors of the metric, the Lagrangian formalism and the Arnowitt-Deser-Misner (ADM) equations [18,19,20]. This work expands new results obtained from the family of metrics proposed in [16,17]. The model is also based on the same hypothesis of linear expansion as [14,15], but analyses the curvature tensor according to the point of view of a hypothetical observer located in the hypersurface of an expanding universe (hypercone section), which can have both positive or negative curvature.…”
Section: Motivationmentioning
confidence: 85%
“…If the Hubble parameter is defined as H :=ȧ/a, this linear expansion corresponds to H = 1/t, which is compatible with the empirical age of the universe [10,13,11,12]. For this reason, alternative cosmological models are based on the equality 1/H = t, such as the Dirac-Milne model and the inhomogeneous hyperconical model [14,15,16,17]. However, symmetry properties of these universes have not been analysed yet, so it is necessary to explore conserved quantities and contrast them with physical observables.…”
Section: Motivationmentioning
confidence: 99%
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