Construction of cosmologically viable f(G) dark energy models
By Antonio de Felice, S. Tsujikawa. 2008
296 citations recorded by the source corpus.
We derive conditions under which f(G) gravity models, whose Lagrangian densities f are written in terms of a Gauss-Bonnet term G, are cosmologically viable. The most crucial condition to be satisfied is that f_GG, the second derivative of f with respect to G, must be positive, which is required to ensure the stability of a late-time de-Sitter solution as well as the existence of standard radiation/matter dominated epochs. We present a number of explicit f(G) models in which a cosmic acceleration is followed by the matter era. We find that the equation of state of dark energy can cross the phantom divide before reaching the present Universe. The viable models have asymptotic behavior f_GG goes to +0 when |G| goes to infinity, in which case a rapid oscillation of perturbations occurs unless such an oscillating degree of freedom is suppressed relative to a homogeneous mode in the early universe. We also introduce an iterative method to avoid numerical instabilities associated with a large mass of the oscillating mode. Comment: 12 pages, 5 figures, uses ReVTeX. Added references, minor corrections
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/2d696043f42e3c69fc9ea8b26660062b0f223b59
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
- Rafael C. Nunes
- Supriya Pan
- Emmanuel N. Saridakis
- E. Abreu
- S. Vagnozzi
- Tomi Koivisto
- Yi-Fu Cai
- A. Golovnev
In Nuclear and High Energy Physics
- Rafael C. Nunes
- Supriya Pan
- E. Abreu
- Emmanuel N. Saridakis
- S. Vagnozzi
- Yi-Fu Cai
- Salvatore Capozziello
- M. De Laurentis
Citations in the corpus
- New observational constraints on f(R) gravity from cosmic chronometers (2016, background): “However, one can construct many other classes of curvature-based modified gravities, such as f(G) gravity [27, 28], Lovelock gravity [29, 30], Weyl gravity [31, 32], Galileon theory [33–36], or even extend to torsion-based modifications, such as f(T ) gravity [37–42], f(T, TG) gravity [43–45], etc.”