2016/08/22 by Sara Jamali, Mahmood Roshan · 16 citations
Physics and Astronomy · #Astrophysics #Black Holes and Theoretical Physics #Cosmological constant #Cosmology #Cosmology and Gravitation Theories #Dark energy #Geometry #Lambda #Mathematical physics #Metric expansion of space #Physics #Quantum #Quantum gravity #Quantum mechanics #Scalar (mathematics) #Scalar field #Scale factor (cosmology) #Solar and Space Plasma Dynamics #Tensor (intrinsic definition) #Theoretical physics #Universe #astro-ph.CO #f(R) gravity #gr-qc
paper · pdf · doi:10.1140/epjc/s10052-016-4336-x
published in The European Physical Journal C 76(9) (Springer Science+Business Media) · To appear in EPJC
arxiv created 2016/08/22 · openalex publication_date 2016/09/01 · arxiv updated 2016/09/13 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We investigate the cosmological consequences of a scalar-vector-tensor theory of gravity known as modified gravity (MOG). In MOG, in addition to metric tensor, there are two scalar fields G(x) and μ (x) , and one vector field φ α (x) . Using the phase space analysis, we explore the cosmological consequences of a model of MOG and find some new interesting features which are absent in Λ CDM model. More specifically we study the possibility that if the extra fields of this theory behave like dark energy to explain the cosmic speedup. More interestingly, with or without cosmological constant, a strongly phantom crossing occurs. Also we find that this theory in its original form ( Λ ≠ 0 ) possesses a true sequence of cosmological epochs. However, we show that, surprisingly, there are two radiation-dominated epochs, f5 and f6 , two matter-dominated phases, f3 and f4 , and two late time accelerated eras, f12 and f7 . Depending on the initial conditions the universe will realize only three of these six eras. However, the matter-dominated phases are dramatically different from the standard matter-dominated epoch. In these phases the cosmic scale factor grows as a(t)∼ t0.46 and t0.52 , respectively, which are slower than the standard case, i.e. a(t)∼ t2/3 . Considering these results we discuss the cosmological viability of MOG.