English

Myrzakulov $F(T,Q)$ gravity: cosmological implications and constraints

General Relativity and Quantum Cosmology 2024-09-05 v1

Abstract

In this paper, we investigate some exact cosmological models in Myrzakulov F(T,Q)F(T,Q) gravity or the Myrzakulov gravity-III (MG-III) proposed in [arXiv:1205.5266], with observational constraints. The MG-III gravity is some kind of unification of two known gravity theories, namely, the F(T)F(T) gravity and the F(Q)F(Q) gravity. The field equations of the MG-III theory are obtained by regarding the metric tensor and the general affine connection as independent variables. We then focus on the particular case in which the F(T,Q)F(T,Q) function characterizing the aforementioned metric-affine models is linear that is F(T,Q)=λT+μQF(T,Q)=\lambda T+\mu Q. We investigate this linear case and consider a Friedmann-Lema\^{i}tre-Robertson-Walker background to study cosmological aspects and applications. We have obtained three exact solutions of the modified field equations in different cases TT and QQ, in the form of Hubble function H(t)H(t) and scale factor a(t)a(t) and placed observational constraints on it through the Hubble H(z)H(z) datasets on it using the MCMC analysis. We have investigated the deceleration parameter q(z)q(z), effective EoS parameters and a comparative study of all three models with Λ\LambdaCDM model has been carried out.

Keywords

Cite

@article{arxiv.2404.09698,
  title  = {Myrzakulov $F(T,Q)$ gravity: cosmological implications and constraints},
  author = {Dinesh Chandra Maurya and K. Yesmakhanova and R. Myrzakulov and G. Nugmanova},
  journal= {arXiv preprint arXiv:2404.09698},
  year   = {2024}
}

Comments

33 pages, 11 figures. arXiv admin note: text overlap with arXiv:2403.11604