Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case

Abstract In this paper we performed investigation of the spatially-flat cosmological models whose spatial section is product of three- (“our Universe”) and extra-dimensional parts. The matter source chosen to be the perfect fluid which exists in the entire space. We described all physically sensible...

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Main Author: Sergey A. Pavluchenko
Format: Article
Language:English
Published: SpringerOpen 2019-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-6624-8
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spelling doaj-9bfd6435b8fa443ba2424e0c090c547b2020-11-25T02:51:52ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-02-0179212110.1140/epjc/s10052-019-6624-8Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional caseSergey A. Pavluchenko0Programa de Pós-Graduação em Física, Universidade Federal do Maranhão (UFMA)Abstract In this paper we performed investigation of the spatially-flat cosmological models whose spatial section is product of three- (“our Universe”) and extra-dimensional parts. The matter source chosen to be the perfect fluid which exists in the entire space. We described all physically sensible cases for the entire range of possible initial conditions and parameters as well as brought the connections with vacuum and $$\Lambda $$ Λ -term regimes described earlier. In the present paper we limit ourselves with $$D=1, 2$$ D=1,2 (number of extra dimensions). The results suggest that in $$D=1$$ D=1 there are no realistic compactification regimes while in $$D=2$$ D=2 there is if $$\alpha > 0$$ α>0 (the Gauss–Bonnet coupling) and the equation of state $$\omega < 1/3$$ ω<1/3 ; the measure of the initial conditions leading to this regime is increasing with growth of $$\omega $$ ω and reaches its maximum at $$\omega \rightarrow 1/3 - 0$$ ω→1/3-0 . We also describe some pecularities of the model, distinct to the vacuum and $$\Lambda $$ Λ -term cases – existence of the isotropic power-law regime, different role of the constant-volume solution and the presence of the maximal density for $$D = 2$$ D=2 , $$\alpha < 0$$ α<0 subcase and associated features.http://link.springer.com/article/10.1140/epjc/s10052-019-6624-8
collection DOAJ
language English
format Article
sources DOAJ
author Sergey A. Pavluchenko
spellingShingle Sergey A. Pavluchenko
Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
European Physical Journal C: Particles and Fields
author_facet Sergey A. Pavluchenko
author_sort Sergey A. Pavluchenko
title Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
title_short Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
title_full Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
title_fullStr Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
title_full_unstemmed Dynamics of the cosmological models with perfect fluid in Einstein–Gauss–Bonnet gravity: low-dimensional case
title_sort dynamics of the cosmological models with perfect fluid in einstein–gauss–bonnet gravity: low-dimensional case
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-02-01
description Abstract In this paper we performed investigation of the spatially-flat cosmological models whose spatial section is product of three- (“our Universe”) and extra-dimensional parts. The matter source chosen to be the perfect fluid which exists in the entire space. We described all physically sensible cases for the entire range of possible initial conditions and parameters as well as brought the connections with vacuum and $$\Lambda $$ Λ -term regimes described earlier. In the present paper we limit ourselves with $$D=1, 2$$ D=1,2 (number of extra dimensions). The results suggest that in $$D=1$$ D=1 there are no realistic compactification regimes while in $$D=2$$ D=2 there is if $$\alpha > 0$$ α>0 (the Gauss–Bonnet coupling) and the equation of state $$\omega < 1/3$$ ω<1/3 ; the measure of the initial conditions leading to this regime is increasing with growth of $$\omega $$ ω and reaches its maximum at $$\omega \rightarrow 1/3 - 0$$ ω→1/3-0 . We also describe some pecularities of the model, distinct to the vacuum and $$\Lambda $$ Λ -term cases – existence of the isotropic power-law regime, different role of the constant-volume solution and the presence of the maximal density for $$D = 2$$ D=2 , $$\alpha < 0$$ α<0 subcase and associated features.
url http://link.springer.com/article/10.1140/epjc/s10052-019-6624-8
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