12,448 research outputs found

    Wormholes in R2R^2-gravity within the f(R,T)f(R,T) formalism

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    We propose, as a novelty in the literature, the modelling of wormholes within the particular case of the f(R,T)f(R,T) gravity, namely f(R,T)=R+αR2+λTf(R,T)=R+\alpha R^{2}+\lambda T, with RR and TT being the Ricci scalar and trace of the energy-momentum tensor, respectively, while α\alpha and λ\lambda are constants. Although such a functional form application can be found in the literature, those concern to compact astrophysical objects, such that no wormhole analysis has been done so far. The quadratic geometric and linear material corrections of this theory make the matter content of the wormhole to remarkably be able to obey the energy conditions.Comment: Published versio

    f(R,T)=f(R)+λTf(R,T)=f(R)+\lambda T gravity models as alternatives to cosmic acceleration

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    This article presents cosmological models that arise in a subclass of f(R,T)=f(R)+f(T)f(R,T)=f(R)+f(T) gravity models, with different f(R)f(R) functions and fixed TT-dependence. That is, the gravitational lagrangian is considered as f(R,T)=f(R)+λTf(R,T)=f(R)+\lambda T, with constant λ\lambda. Here RR and TT represent the Ricci scalar and trace of the stress-energy tensor, respectively. The modified gravitational field equations are obtained through the metric formalism for the Friedmann-Lema\^itre-Robertson-Walker metric with signature (+,,,)(+,-,-,-). We work with f(R)=R+αR2μ4Rf(R)=R+\alpha R^2-\frac{\mu^4}{R}, f(R)=R+kln(γR)f(R)=R+k\ln(\gamma R) and f(R)=R+me[nR]f(R)=R+me^{[-nR]}, with α,μ,k,γ,m\alpha, \mu, k, \gamma, m and nn all free parameters, which lead to three different cosmological models for our Universe. For the choice of λ=0\lambda=0, this reduces to widely discussed f(R)f(R) gravity models. This manuscript clearly describes the effects of adding the trace of the energy-momentum tensor in the f(R)f(R) lagrangian. The exact solution of the modified field equations are obtained under the hybrid expansion law. Also we present the Om diagnostic analysis for the discussed models.Comment: 11 pages, 20 figures, Accepted version in EPJ

    Wormholes in exponential f(R,T)f(R,T) gravity

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    Alternative gravity is nowadays an extremely important tool to address some persistent observational issues, such as the dark sector of the universe. They can also be applied to stellar astrophysics, leading to outcomes one step ahead of those obtained through General Relativity. In the present article we test a novel f(R,T)f(R,T) gravity model within the physics and geometry of wormholes. The f(R,T)f(R,T) gravity is a reputed alternative gravity theory in which the Ricci scalar RR in the Einstein-Hilbert gravitational lagrangian is replaced by a general function of RR and TT, namely f(R,T)f(R,T), with TT representing the trace of the energy-momentum tensor. We propose, for the first time in the literature, an exponential form for the dependence of the theory on TT. We derive the field equations as well as the non-continuity equation and solve those to wormhole metric and energy-momentum tensor. The importance of applying alternative gravity to wormholes is that through these theories it might be possible to obtain wormhole solutions satisfying the energy conditions, departing from General Relativity well-known outcomes. In this article, we indeed show that it is possible to obtain wormhole solutions satisfying the energy conditions in the exponential f(R,T)f(R,T) gravity. Naturally, there is still a lot to do with this model, as cosmological, galactical and stellar astrophysics applications, and the reader is strongly encouraged to do so, but, anyhow, one can see the present outcomes as a good indicative for the theory.Comment: 6 pages, 3 figures, To appear in European Physical Journal
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