2008/11/30 by Savvas Nesseris · 122 citations
Physics and Astronomy · #Astrophysics #Big Bang nucleosynthesis #Black Holes and Theoretical Physics #Classical mechanics #Cosmology #Cosmology and Gravitation Theories #Coupling (piping) #Coupling constant #Dark energy #Dark matter #Friedmann equations #Galaxies: Formation, Evolution, Phenomena #Gravitation #Mathematical physics #Nucleosynthesis #Perturbation (astronomy) #Perturbation theory (quantum mechanics) #Phenomenology (philosophy) #Physics #Quantum mechanics #Sigma #Stars #Theoretical physics #astro-ph #gr-qc
paper · pdf · doi:10.1103/physrevd.79.044015
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 79(4) (American Physical Society) · 9 pages, 3 figures, uses revtex4, added Appendix and references, minor changes, accepted in Phys. Rev. D (to appear)
arxiv created 2009/02/10 · openalex publication_date 2009/02/12 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We consider theories with an arbitrary coupling between matter and gravity and obtain the perturbation equation of matter on subhorizon scales. Also, we derive the effective gravitational constant Geff and two parameters \ensuremathΣ and \ensuremathη, which along with the perturbation equation of the matter density are useful to constrain the theory from growth factor and weak lensing observations. Finally, we use a completely solvable toy model which exhibits nontrivial phenomenology to investigate specific features of the theory. We obtain the analytic solution of the modified Friedmann equation for the scale factor a in terms of time t and use the age of the oldest star clusters and the primordial nucleosynthesis bounds in order to constrain the parameters of our toy model.