We consider general curvature-invariant modifications of the Einstein-Hilbert action that become important only in regions of extremely low space-time curvature. We investigate the late-time evolution of the universe in such models, examining the possibilities for cosmic acceleration and other ultimate destinies. The models generically possess de Sitter space as an unstable solution and exhibit an interesting set of attractor solutions which, in some cases, provide alternatives to dark energy models. We show that modifications of the form f( R) are ruled out by solar system tests of gravitation. In addition, we also review the Palatini method of variation for such theories and contrast it with the metric variation approach
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...
We discuss modified gravity which includes negative and positive powers of curvature and provides gr...
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...
I give a short introduction to standard cosmology and a review of what it is meant by the dark ener...
Recent observations arising from a number of sources suggest that the Universe is currently undergoi...
We propose a class of actions for the spacetime metric that introduce corrections to the Einstein-Hi...
We propose a class of actions for the spacetime metric that introduce corrections to the Einstein-Hi...
The late time acceleration of the universe poses a puzzle for modern cosmology. There exist several ...
The future finite-time singularities emerging in alternative gravity dark energy models are classifi...
We use the effective field theory of dark energy to explore the space of modified gravity models whi...
Explanations of the late-time cosmic acceleration within the framework of general relativity are pla...
v1: 28 pages, 20 pdf figures. v2: 29 pages, minor improvements in the text, figures improvedInternat...
v1: 28 pages, 20 pdf figures. v2: 29 pages, minor improvements in the text, figures improvedInternat...
We study spherically symmetric solutions in f(R) theories and its compatibility with local tests of ...
International audienceWe propose, in a heuristic way, a relativistic modified gravity model as an al...
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...
We discuss modified gravity which includes negative and positive powers of curvature and provides gr...
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...
I give a short introduction to standard cosmology and a review of what it is meant by the dark ener...
Recent observations arising from a number of sources suggest that the Universe is currently undergoi...
We propose a class of actions for the spacetime metric that introduce corrections to the Einstein-Hi...
We propose a class of actions for the spacetime metric that introduce corrections to the Einstein-Hi...
The late time acceleration of the universe poses a puzzle for modern cosmology. There exist several ...
The future finite-time singularities emerging in alternative gravity dark energy models are classifi...
We use the effective field theory of dark energy to explore the space of modified gravity models whi...
Explanations of the late-time cosmic acceleration within the framework of general relativity are pla...
v1: 28 pages, 20 pdf figures. v2: 29 pages, minor improvements in the text, figures improvedInternat...
v1: 28 pages, 20 pdf figures. v2: 29 pages, minor improvements in the text, figures improvedInternat...
We study spherically symmetric solutions in f(R) theories and its compatibility with local tests of ...
International audienceWe propose, in a heuristic way, a relativistic modified gravity model as an al...
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...
We discuss modified gravity which includes negative and positive powers of curvature and provides gr...
Modified gravity theories with the Gauss-Bonnet term G=R2−4RμνRμν+RμνρσRμνρσ have recently gained a ...