Abstract
We investigate classes of shear-free cosmological dust models with irrotational fluid flows within the framework of f(T) gravity. In particular, we use the 1 + 3 covariant formalism and present the covariant linearised evolution and constraint equations describing such models. We then derive the integrability conditions describing a consistent evolution of the linearised field equations of these quasi-Newtonian universes in the f(T) gravitational theory. Finally, we derive the evolution equations for the density and velocity perturbations of the quasi-Newtonian universe. We explore the behaviour of the matter density contrast for two models – f(T)= mu T_{0}(T/T_{0})^{n} and the more generalised case, where f(T)= T+ mu T_{0} (T/T_{0})^{n}, with and without the application of the quasi-static approximation. Our numerical solutions show that these f(T) theories can be suitable alternatives to study the background dynamics, whereas the growth of energy density fluctuations change dramatically from the expected Lambda CDM behaviour even for small deviation from the general relativistic limits of the underlying f(T) theory. Moreover, applying the so-called quasi-static approximation yields exact-solution results that are orders of magnitude different from the numerically integrated solutions of the full system, suggesting that these approximations are not applicable here.
Highlights
Dark component to the total energy density [3]
This paper is organised as follows: in Sects. 2–4 respectively, we review the 1 + 3 covariant approach, kinematics quantities in the presence of torsion and we provide the covariant form of the field equations in f (T ) gravity which are required to study the cosmological perturbations
This work presented a detailed analysis of scalar cosmological perturbations in the f (T ) gravity theory using the 1 + 3 covariant gauge-invariant approach
Summary
We consider the covariant form of the field equations of f (T ) gravity to study linear cosmological perturbations [28]. In the 1 + 3 covariant approach, the perturbations are formulated using variables that are covariantly defined in the real universe, and are exactly gauge-invariant by construction [41] This approach has been used recently to study the cosmological perturbations for different contexts of modified gravity and G R [34,40,42]. We consider the covariant form of f (T ) gravity to clearly show the equivalence between teleparallel gravity and General Relativity This form of field equation is very advisable to define the covariant variables in a gauge-invariant formalism for the study of the cosmological perturbations. Where Tab denotes the usual energy-momentum tensor of the matter fluid expressed as
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