2020
DOI: 10.1007/s12648-020-01877-2
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Cosmological models with variable anisotropic parameter in f(R, T) gravity

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Cited by 31 publications
(8 citation statements)
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“…Furthermore, Maurya et al [69] have demonstrated the existence of strange star candidates beyond the standard maximum mass limit by employing the gravitational decoupling method within 5D Einstein-Gauss-Bonnet formalism. In this connection, some more solutions including cosmological models have been investigated in f (R, T ), f (T ), and f (T, T ) gravity theories [78][79][80][81].…”
Section: Jcap10(2022)003mentioning
confidence: 99%
“…Furthermore, Maurya et al [69] have demonstrated the existence of strange star candidates beyond the standard maximum mass limit by employing the gravitational decoupling method within 5D Einstein-Gauss-Bonnet formalism. In this connection, some more solutions including cosmological models have been investigated in f (R, T ), f (T ), and f (T, T ) gravity theories [78][79][80][81].…”
Section: Jcap10(2022)003mentioning
confidence: 99%
“…Nevertheless, the nature and origin for the violation of the homogeneity and isotropy has yet resolved [14]. In view of this, in the present work, we are motivated to take up this bouncing issue in a homogeneous and anisotropic background of the metric in the framework of an extended theory of gravity [15,16].…”
Section: Introductionmentioning
confidence: 99%
“…In recent times, the bouncing scenario has been extensively studied in the curvature and torsion based modified gravity and in the scalar tensor models. [15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%
“…The antisymmetry of the linked geometrical objects is presumptively respected by the Lagrange multipliers. Therefore, vanishing curvature R μ βαγ = 0 and torsion T μ αβ = 0 are imposed, as is expected in the symmetric teleparallel framework, by the equations λ scalar-curvature case the action does not preserve its form under the local conformal rescaling of the metric.gμν = e − √ 2/3 (ϕ) g μν(27)…”
mentioning
confidence: 98%