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Inflation in Energy-Momentum Squared Gravity in Light of Planck2018

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arxiv 2107.13547 v1 pith:VRKAU4I7 submitted 2021-07-29 gr-qc astro-ph.COhep-phhep-th

classification gr-qcastro-ph.COhep-phhep-th
keywords zetaenergy-momentumtextbfgravityinflationmodelsquaredtensor
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abstract

We study cosmological dynamics of the energy-momentum squared gravity. By adding the squared of the matter field's energy-momentum tensor ($\zeta\, \textbf{T}^{2}$) to the Einstein Hilbert action, we obtain the Einstein's field equations and study the conservation law. We show that the presence of $\zeta\, \textbf{T}^{2}$ term, breaks the conservation of the energy-momentum tensor of the matter fields. However, an effective energy-momentum tensor in this model is conserved in time. By considering the FRW metric as the background, we find the Friedmann equations and by which we explore the cosmological inflation in $\zeta\,\textbf{T}^{2}$ model. We perform numerical analysis on the perturbation parameters and compare the results with Planck2018 different data sets at $68\%$ and $95\%$ CL, to obtain some constraints on the coupling parameter $\zeta$. We show that \textbf{ for $0< \zeta \leq 2.1\times 10^{-5}$, the $\zeta\, \textbf{T}^{2}$ gravity is an observationally viable model of inflation.

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  1. Baryon asymmetry from higher-order matter contributions in gravity

    gr-qc 2025-04 conditional novelty 6.0 of 10

    A T^2-dependent coupling between the derivative of T_mu nu T^mu nu and the baryon current can generate the observed baryon asymmetry in GR and f(R,T^2) gravity, at the cost of fitted parameters.

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