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Main Authors: Shekh, S. H., Pradhan, Anirudh, Gaikwad, S. P., Mule, K. R.
Format: Preprint
Published: 2024
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Online Access:https://arxiv.org/abs/2408.00022
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author Shekh, S. H.
Pradhan, Anirudh
Gaikwad, S. P.
Mule, K. R.
author_facet Shekh, S. H.
Pradhan, Anirudh
Gaikwad, S. P.
Mule, K. R.
contents The dynamics of perfect fluid as a source in the context of modified gravity, specifically $f(Q,T)$ gravity, are examined within the Friedmann-Lemaître-Robertson-Walker (FLRW) cosmological model. This gravity is a generic function of the non-metricity scalar $Q$ and its trace $T$. We investigate the characteristics of the derived cosmological model using a parameterized form of Hubble's parameter, $H(z) = H_0\left[Ω_{0m}(1+z)^3 + (1-Ω_{0m})\right]^{\frac{1}{2}}$ (Mahmood et al. Int. J. Geom. Methods Mod. Phys., https://doi.org/10.1142/S0219887824502049). Our examination reveals how physical parameters such as energy density, pressure, and the equation of state parameter, among others, in our model accurately describe the physical behavior of the cosmos. Furthermore, we explore the kinematic parameters in our model, which provide valuable insights into the cosmos's expansion history, including its acceleration, deceleration, and the evolution of its large-scale structure. By exploring these aspects, we gain a deeper understanding of the cosmos's dynamics and evolution within the context of modified gravity.
format Preprint
id arxiv_https___arxiv_org_abs_2408_00022
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Cosmography in $f(Q,T)$ gravity with the specific $H(z)$
Shekh, S. H.
Pradhan, Anirudh
Gaikwad, S. P.
Mule, K. R.
General Relativity and Quantum Cosmology
The dynamics of perfect fluid as a source in the context of modified gravity, specifically $f(Q,T)$ gravity, are examined within the Friedmann-Lemaître-Robertson-Walker (FLRW) cosmological model. This gravity is a generic function of the non-metricity scalar $Q$ and its trace $T$. We investigate the characteristics of the derived cosmological model using a parameterized form of Hubble's parameter, $H(z) = H_0\left[Ω_{0m}(1+z)^3 + (1-Ω_{0m})\right]^{\frac{1}{2}}$ (Mahmood et al. Int. J. Geom. Methods Mod. Phys., https://doi.org/10.1142/S0219887824502049). Our examination reveals how physical parameters such as energy density, pressure, and the equation of state parameter, among others, in our model accurately describe the physical behavior of the cosmos. Furthermore, we explore the kinematic parameters in our model, which provide valuable insights into the cosmos's expansion history, including its acceleration, deceleration, and the evolution of its large-scale structure. By exploring these aspects, we gain a deeper understanding of the cosmos's dynamics and evolution within the context of modified gravity.
title Cosmography in $f(Q,T)$ gravity with the specific $H(z)$
topic General Relativity and Quantum Cosmology
url https://arxiv.org/abs/2408.00022