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Kantowski-Sachs Barrow Holographic Dark Energy Model in Saez-Ballester Theory of Gravitation
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In this chapter, we have studied a spatially homogeneous and anisotropic Kantowski-Sachs universe in the presence of Barrow Holographic Dark Energy in the background of Saez-Ballester scalar-tensor theory of gravitation. To find the exact solution of the SB field equations, we have assumed that the shear scalar is directly proportional to the expansion scalar. This assumption leads to relation between metric potentials of the models. We have discussed non-interacting and interacting cosmological models. Moreover, we have discussed several cosmological parameters such as energy densities of DM and DE (ρm & ρb), deceleration q, equation of state (ωb) and skewness (α) parameters, squared sound speed (vs2), ωb-ωb′ plane statefinders and Om-diagnostics parameters through graphical representation for both the interacting models. Also, we have observed that the current values of deceleration and EoS parameters of our constructed models coincide with the recent observational data.
Title: Kantowski-Sachs Barrow Holographic Dark Energy Model in Saez-Ballester Theory of Gravitation
Description:
In this chapter, we have studied a spatially homogeneous and anisotropic Kantowski-Sachs universe in the presence of Barrow Holographic Dark Energy in the background of Saez-Ballester scalar-tensor theory of gravitation.
To find the exact solution of the SB field equations, we have assumed that the shear scalar is directly proportional to the expansion scalar.
This assumption leads to relation between metric potentials of the models.
We have discussed non-interacting and interacting cosmological models.
Moreover, we have discussed several cosmological parameters such as energy densities of DM and DE (ρm & ρb), deceleration q, equation of state (ωb) and skewness (α) parameters, squared sound speed (vs2), ωb-ωb′ plane statefinders and Om-diagnostics parameters through graphical representation for both the interacting models.
Also, we have observed that the current values of deceleration and EoS parameters of our constructed models coincide with the recent observational data.
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