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The phase-space of generalized Gauss-Bonnet dark energy

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
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.

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years

2025 1 2011 1

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UNVERDICTED 2

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representative citing papers

Modified Gravity and Cosmology

astro-ph.CO · 2011-06-13 · unverdicted · novelty 2.0

A comprehensive review of modified gravity theories and their cosmological consequences, including a parameterized post-Friedmannian formalism for constraining deviations from General Relativity.

citing papers explorer

Showing 2 of 2 citing papers.

  • Dynamical system analysis of the cosmological phases in Palatini $k$-essence gravity gr-qc · 2025-11-24 · unverdicted · none · ref 43 · internal anchor

    Dynamical systems analysis of a Palatini k-essence model identifies fixed points for quasi-de-Sitter epochs, scaling solutions, and quintessence phases connected by heteroclinic orbits in flat FLRW cosmology.

  • Modified Gravity and Cosmology astro-ph.CO · 2011-06-13 · unverdicted · none · ref 25

    A comprehensive review of modified gravity theories and their cosmological consequences, including a parameterized post-Friedmannian formalism for constraining deviations from General Relativity.