A note on holographic dark energy with varying $c^2$ term
Int J Theor Phys 56 (2017) 1845 We reconsider the holographic dark energy (HDE) model with a slowly time varying $ c^2(z)$ parameter in the energy density, namely $\rho_D=3M_p^2 c^2(z)/L^2$, where $L$ is the IR cutoff and $z$ is the redshift parameter. As the system's IR cutoff we choose the Hu...
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Zusammenfassung: | Int J Theor Phys 56 (2017) 1845 We reconsider the holographic dark energy (HDE) model with a slowly time
varying $ c^2(z)$ parameter in the energy density, namely $\rho_D=3M_p^2
c^2(z)/L^2$, where $L$ is the IR cutoff and $z$ is the redshift parameter. As
the system's IR cutoff we choose the Hubble radius and the Granda-Oliveros (GO)
cutoffs. The latter inspired by the Ricci scalar curvature. We derive the
evolution of the cosmological parameters such as the equation of state and the
deceleration parameters as the explicit functions of the redshift parameter
$z$. Then, we plot the evolutions of these cosmological parameters in terms of
the redshift parameter during the history of the universe. Interestingly
enough, we observe that by choosing $L=H^{-1}$ as the IR cutoff for the HDE
with time varying $ c ^2(z) $ term, the present acceleration of the universe
expansion can be achieved, even in the absence of interaction between dark
energy and dark matter. This is in contrast to the usual HDE model with
constant $c^2$ term, which leads to a wrong equation of state, namely that for
dust $w_D=0$, when the IR cutoff is chosen the Hubble radius. |
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DOI: | 10.48550/arxiv.1612.03040 |