Abstract

Recent elaborated by T. Harko and collaborators, the $f(R,T)$ theories of gravity contemplate an optimistic alternative to dark energy, for which $R$ and $T$ stand for the Ricci scalar and the trace of the energy-momentum tensor, respectively. Although the literature has shown that the $T$ dependence on the gravitational part of the action - which is due to the consideration of quantum effects - may induce some novel features in the scope of late-time cosmological dynamics, in the radiation-dominated universe, when $T=0$, no contributions seem to rise from such theories. Apparently, $f(R,T)$ contributions to a radiation-dominated universe may rise only from the $f(R,T^\varphi)$ approach, which is nothing but the $f(R,T)$ gravity in the case of a self-interacting scalar field whose trace of the energy-momentum tensor is $T^\varphi$. We intend, in this article, to show how $f(R,T^\varphi)$ theories of gravity can contribute to the study of the primordial stages of the universe. Our results predict a graceful exit from inflationary stage to a radiation-dominated era. They also predict a late-time cosmic acceleration after a matter-dominated phase, making the $f(R,T^\varphi)$ theories able to describe, in a self-consistent way, all the different stages of the universe dynamics.

Highlights

  • Plenty of efforts have been made in the theoretical framework with the purpose of explaining the accelerated regime our universe has passed through a fraction of a second after the Big Bang, named the “inflationary era”

  • The late-time acceleration of the universe expansion [13,14,15] has been broadly investigated in such a theory of gravity [16,17,18,19,20,21,22,23,24,25], the inflationary era still presents a lack of examination

  • We have obtained from the first-order formalism applied to f (R, T φ) gravity two models able to describe all the different dynamical stages of the universe, from inflation, to radiation, to matter and dark-energy dominated

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Summary

Introduction

Plenty of efforts have been made in the theoretical framework with the purpose of explaining the accelerated regime our universe has passed through a fraction of a second after the Big Bang, named the “inflationary era”. A priori, it seems reasonable to affirm that the f (R, T ) gravity does not contribute to the study of the radiationdominated universe, since the contribution coming from the trace of the energy-momentum tensor in f (R, T ) vanishes at this stage. Such a shortcoming or incompleteness has attracted attention recently [23,24,25,26].

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First-order formalism
Examples
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Cosmological interpretations
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Discussion and perspectives
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