Cosmology in scalar-tensor <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>f</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mtext> </mml:mtext><mml:mi>T</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math> gravity
Tiago B. Gonçalves, João Luís Rosa, Francisco S. N. Lobo
Abstract
In this work, we use reconstruction methods to obtain cosmological solutions in the recently developed scalar-tensor representation of $f(R,T)$ gravity. Assuming that matter is described by an isotropic perfect fluid and the spacetime is homogeneous and isotropic, i.e., the Friedmann-Lema\^{\i}tre-Robertson-Walker (FLRW) universe, the energy density, the pressure, and the scalar field associated with the arbitrary dependency of the action in $T$ can be written generally as functions of the scale factor. We then select three particular forms of the scale factor: an exponential expansion with $a(t)\ensuremath{\propto}{e}^{t}$ (motivated by the de Sitter solution); and two types of power-law expansion with $a(t)\ensuremath{\propto}{t}^{1/2}$ and $a(t)\ensuremath{\propto}{t}^{2/3}$ (motivated by the behaviors of radiation- and matter-dominated universes in general relativity, respectively). A complete analysis for different curvature parameters $k={\ensuremath{-}1,0,1}$ and equation of state parameters $w={\ensuremath{-}1,0,1/3}$ is provided. Finally, the explicit forms of the functions $f(R,T)$ associated with the scalar-field potentials of the representation used are deduced.