The phase-space of generalized Gauss-Bonnet dark energy
arXiv:0908.1150 · doi:10.1103/PhysRevD.80.043006
Abstract
The generalized Gauss-Bonnet theory, introduced by Lagrangian F(R,G), has been considered as a general modified gravity for explanation of the dark energy. G is the Gauss-Bonnet invariant. For this model, we seek the situations under which the late-time behavior of the theory is the de-Sitter space-time. This is done by studying the two dimensional phase space of this theory, i.e. the R-H plane. By obtaining the conditions under which the de-Sitter space-time is the stable attractor of this theory, several aspects of this problem have been investigated. It has been shown that there exist at least two classes of stable attractors : the singularities of the F(R,G), and the cases in which the model has a critical curve, instead of critical points. This curve is R=12H^2 in R-H plane. Several examples, including their numerical calculations, have been discussed.
19 pages, 11 figures, typos corrected, a reference added
References in corpus (8)
- Models of f(R) Cosmic Acceleration that Evade Solar-System Tests
- Conditions for the cosmological viability of f(R) dark energy models
- Matter instability in modified gravity
- Cosmological coincidence problem in interacting dark energy models
- Gauss-Bonnet cosmologies: crossing the phantom divide and the transition from matter dominance to dark energy
- The phase space view of f(R) gravity
- On the Stability of a class of Modified Gravitational Models
- Asymptotic behavior of w in general quintom model