Abstract:Abstract. -In this work we investigate the behavior of two-dimensional (2D) cosmological models, starting with the Jackiw-Teitelboim (JT) theory of gravitation. A geometrical term, non-linear in the scalar curvature R, is added to the JT dynamics to test if it could play the role of dark energy in a 2D expanding universe. This formulation makes possible, first, the description of an early (inflationary) 2D universe, when the van der Waals (vdW) equation of state is used to construct the energymomentum tensor o… Show more
“…This is also the case to describe the transition to a final period (leaving the matter dominated era) when the non-linear term in R starts to show its effects and promotes the desired accelerated regime, that would correspond to the dark energy dominated era. The results have also shown that the role of the non-linear term is similar to the one found in 2D (when it is used the JT model [7]); although this parallel can be done only qualitatively: different forms in the explicit expressions for the dynamics are found and also different values of parameters are necessary to select the more interesting scenarios. In both cases the analysis and results remain as theoretical explorations of hypothetical universes in lower dimensions.…”
Section: +H; 9880 -Kmentioning
confidence: 70%
“…These ideas come in substitution to the standard formulations that take the dark energy as a "usual" source [6]. This approach was tested in a 2D context recently by these authors [7], working with the Jackiw-Teitelboim (JT) model [1,9].…”
Section: +H; 9880 -Kmentioning
confidence: 99%
“…The results include (using the 3D Robertson-Walker metric) the description of periods dominated by matter and/or radiation [4], inflationary young 3D universes and finally old universes dominated by dark energy in transition from a matter dominated period [8]; where the dark energy constituent is modeled using different equations of state [4,5,8]. As we mentioned before the central idea of this work is to include in the field equations a new term, non-linear in the curvature scalar R. This discussion was done in [6] for 4D models and in [7] for 2D models. We start with the new field equations…”
Section: +H; 9880 -Kmentioning
confidence: 99%
“…The normalized boundary conditions are in this case : a(0) = 1, ȧ(0) = 1 e ρ(0) = 1. These conditions simulate a young 3D universe, in the beginning of an inflationary period [5,7,8].…”
By the inclusion of an additional term, nonlinear in the scalar curvature R, it is tested if dark energy could rise as a geometrical effect in 3D gravitational formulations. We investigate a cosmological fluid obeying a non-polytropic equation of state (the van der Waals equation) that is used to construct the energy–momentum tensor of the sources, representing the hypothetical inflaton in gravitational interaction with a matter contribution. Following the evolution in time of the scale factor, its acceleration, and the energy densities of constituents it is possible to construct the description of an inflationary 3D universe, followed by a matter-dominated era. For later times it is verified that, under certain conditions, the nonlinear term in R can generate the old 3D universe in accelerated expansion, where the ordinary matter is represented by the barotropic limit of the van der Waals constituent.
“…This is also the case to describe the transition to a final period (leaving the matter dominated era) when the non-linear term in R starts to show its effects and promotes the desired accelerated regime, that would correspond to the dark energy dominated era. The results have also shown that the role of the non-linear term is similar to the one found in 2D (when it is used the JT model [7]); although this parallel can be done only qualitatively: different forms in the explicit expressions for the dynamics are found and also different values of parameters are necessary to select the more interesting scenarios. In both cases the analysis and results remain as theoretical explorations of hypothetical universes in lower dimensions.…”
Section: +H; 9880 -Kmentioning
confidence: 70%
“…These ideas come in substitution to the standard formulations that take the dark energy as a "usual" source [6]. This approach was tested in a 2D context recently by these authors [7], working with the Jackiw-Teitelboim (JT) model [1,9].…”
Section: +H; 9880 -Kmentioning
confidence: 99%
“…The results include (using the 3D Robertson-Walker metric) the description of periods dominated by matter and/or radiation [4], inflationary young 3D universes and finally old universes dominated by dark energy in transition from a matter dominated period [8]; where the dark energy constituent is modeled using different equations of state [4,5,8]. As we mentioned before the central idea of this work is to include in the field equations a new term, non-linear in the curvature scalar R. This discussion was done in [6] for 4D models and in [7] for 2D models. We start with the new field equations…”
Section: +H; 9880 -Kmentioning
confidence: 99%
“…The normalized boundary conditions are in this case : a(0) = 1, ȧ(0) = 1 e ρ(0) = 1. These conditions simulate a young 3D universe, in the beginning of an inflationary period [5,7,8].…”
By the inclusion of an additional term, nonlinear in the scalar curvature R, it is tested if dark energy could rise as a geometrical effect in 3D gravitational formulations. We investigate a cosmological fluid obeying a non-polytropic equation of state (the van der Waals equation) that is used to construct the energy–momentum tensor of the sources, representing the hypothetical inflaton in gravitational interaction with a matter contribution. Following the evolution in time of the scale factor, its acceleration, and the energy densities of constituents it is possible to construct the description of an inflationary 3D universe, followed by a matter-dominated era. For later times it is verified that, under certain conditions, the nonlinear term in R can generate the old 3D universe in accelerated expansion, where the ordinary matter is represented by the barotropic limit of the van der Waals constituent.
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