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Exact lambdavacuum solutions in higher dimensions

I. A. Sarmiento-Alvarado, P. Wiederhold, T. Matos

Abstract

In this work, we obtain exact solutions to the $(n+2)$-dimensional Einstein Field Equations with a non-zero cosmological constant for $n > 1$. These solutions depend on a set $\{ A_a, a=1,2,\ldots , m \}$ of pairwise commuting constant matrices in $\mathfrak{sl} ( n, \mathbb{R} )$ and on a constant matrix $g_0$ in $\mathcal{I} (\{ A_a, a=1,\ldots , m \})$, determined in previous work. Different choices of $\{ A_a, a=1,\ldots , m \}$ and $g_0$ correspond to different solutions. As examples, we show how to obtain the de Sitter metric, the Anti-de Sitter metric, the Birmingham metric, the Nariai metric and the Anti-Nariai metric in higher dimensions. The generalized Nariai and Anti-Nariai solutions are direct topological products of $AdS_{\frac{n}{2} + 1} \times H^{\frac{n}{2} + 1}$, $dS_{\frac{n}{2} + 1} \times S^{\frac{n}{2} + 1}$, $AdS_2 \times H^n$, $AdS_n \times H^2$, $dS_2 \times S^n$ and $dS_n \times S^2$. In addition, we study a solution in the context of cosmology.

Exact lambdavacuum solutions in higher dimensions

Abstract

In this work, we obtain exact solutions to the -dimensional Einstein Field Equations with a non-zero cosmological constant for . These solutions depend on a set of pairwise commuting constant matrices in and on a constant matrix in , determined in previous work. Different choices of and correspond to different solutions. As examples, we show how to obtain the de Sitter metric, the Anti-de Sitter metric, the Birmingham metric, the Nariai metric and the Anti-Nariai metric in higher dimensions. The generalized Nariai and Anti-Nariai solutions are direct topological products of , , , , and . In addition, we study a solution in the context of cosmology.

Paper Structure

This paper contains 6 sections, 85 equations, 1 figure.

Figures (1)

  • Figure 1: Behavior of $H$ and $q$ as function of $a$.

Theorems & Definitions (4)

  • Example 1
  • Example 2
  • Example 3
  • Example 4