# Stable exponential cosmological solutions with three different   Hubble-like parameters in EGB model with a $\Lambda$-term

**Authors:** K. K. Ernazarov, V. D. Ivashchuk

arXiv: 1906.10391 · 2020-07-15

## TL;DR

This paper explores stable exponential solutions in a higher-dimensional Einstein-Gauss-Bonnet model with a cosmological constant, identifying conditions for solutions with three different Hubble-like parameters and analyzing their stability and physical implications.

## Contribution

It provides explicit conditions for the existence and stability of solutions with three distinct Hubble-like parameters in a D-dimensional EGB model with a cosmological term, including exact solutions in specific cases.

## Key findings

- Solutions exist under specific positivity conditions on parameters.
- Explicit solutions are derived for certain parameter configurations.
- Stable and non-stable subclasses of solutions are identified.

## Abstract

We consider a $D$-dimensional Einstein-Gauss-Bonnet model with a cosmological term $\Lambda$ and two non-zero constants: $\alpha_1$ and $\alpha_2$. We restrict the metrics to be diagonal ones and study a class of solutions with exponential time dependence of three scale factors, governed by three non-coinciding Hubble-like parameters: $H \neq 0$, $h_1$ and $h_2$, obeying $m H + k_1 h_1 + k_2 h_2 \neq 0$ and corresponding to factor spaces of dimensions $m > 1$, $k_1 > 1$ and $k_2 > 1$, respectively ($D = 1 + m + k_1 + k_2$). We analyse two cases: i) $m < k_1 < k_2$ and ii) $1< k_1 = k_2 = k$, $k \neq m$. We show that in both cases the solutions exist if $\alpha = \alpha_2 / \alpha_1 > 0$ and $\alpha \Lambda > 0$ satisfies certain restrictions, e.g. upper and lower bounds. In case ii) explicit relations for exact solutions are found. In both cases the subclasses of stable and non-stable solutions are singled out. For $m > 3$ the case i) contains a subclass of solutions describing an exponential expansion of $3$-dimensional subspace with Hubble parameter $H > 0$ and zero variation of the effective gravitational constant $G$. The case $H = 0$ is also considered.

## Full text

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## Figures

6 figures with captions in the complete paper: https://tomesphere.com/paper/1906.10391/full.md

## References

38 references — full list in the complete paper: https://tomesphere.com/paper/1906.10391/full.md

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Source: https://tomesphere.com/paper/1906.10391