$f(\mathcal{G},T_{\alpha \beta }{T}^{\alpha \beta })$ Theory and Complex Cosmological Structure

Abstract

The basic objective of this investigation is to explore the impact of a novel gravitational modification, specifically, the $f(\mathcal{G},{\mathbf{T}}^2)$ (where ${\mathbf{T}}^2\equiv T_{\alpha \beta }{T}^{\alpha \beta }$, $T^{\alpha \beta }$ denotes the stress-energy tensor) model of gravitation, upon the complexity of time-dependent dissipative as well as non-dissipative spherically symmetric celestial structures. To find the complexity factor $({\mathbb{C}}_{\mathbf{F}})$ from the generic version of the structural variables, we performed Herrera's scheme for the orthogonal cracking of Riemann tensor. In this endeavor, we are mainly concerned with the issue of relativistic gravitational collapse of the dynamically relativistic spheres fulfilling the presumption of minimal ${\mathbb{C}}_{\mathbf{F}}$. The incorporation of a less restrictive condition termed as quasi-homologous $({\mathbb{Q}}_{\mathbf{H}})$ condition together with the zero ${\mathbb{C}}_{\mathbf{F}}$, allows us to formulate a range of exact solutions for a particular choice of $f(\mathcal{G},{\mathbf{T}}^2)$ model. We find that some of the given exact solutions relax the Darmois junction conditions and describe thin shells by satisfying the Israel conditions, while some exhibit voids by fulfilling the Darmois constraints on both boundary surfaces. Eventually, few expected applications of the provided solutions in the era of modern cosmology are debated.

Revision submitted to Physics of the Dark Universe

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Cited by in corpus (1)

• Big Bang Nucleosynthesis constraints on $f(T,T_G)$ gravity