F(R) gravity and the Hubble parameter

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SUMMARY

The discussion centers on the modifications to the Friedman equations and the Hubble parameter in f(R) gravity models, specifically using the Einstein Hilbert Lagrangian and the FRW metric. The user derives a complex equation for the Hubble parameter, H, involving terms from the (00) component of the Einstein field equations, including a fourth-order term of the scale factor, a(t). The user seeks guidance on solving these equations, particularly in the matter-dominated era, and inquires about existing literature on the impact of f(R) models on the Hubble parameter.

PREREQUISITES
  • Understanding of Einstein field equations
  • Familiarity with Friedman equations
  • Knowledge of f(R) gravity models
  • Proficiency in using the FRW metric
NEXT STEPS
  • Research the implications of f(R) gravity on cosmological models
  • Study the derivation and solutions of the modified Friedman equations
  • Explore existing literature on approximations for the Hubble parameter in f(R) models
  • Investigate the role of scale factor dynamics in cosmological evolution
USEFUL FOR

Cosmologists, theoretical physicists, and researchers studying modified gravity theories and their implications on cosmic expansion and the Hubble parameter.

shadishacker
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Dear all,

Considering Einstein Hilbert lagrangian, by using Einstein field equations one can get the form of Friedman equations and consequently the Hubble parameter.
I know that in f(R) models, Einstein equations get modified. However, what happens to the Friedman equation and the Hubble parameter?
I tried to solve them and get to the form of H, but it seems such a complicated equation.

Using the (00) component, I get
\begin{equation}
H^2=\frac{8\pi G}{3}\rho -\frac{6\alpha}{c^2}(\frac{\ddot{a}^2}{a^2} + H^4)
\end{equation}
What should I do with the
\begin{equation} \ddot{a}^2\end{equation}
in the first equation?!
The (11) component just makes everything more complicated!
I really appreciate any help or idea.
BTW, I am using FRW metric.
 
Last edited:
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I just realized that the equations consist the forth order of the scale factor (a(t)).
Are these solvable in the matter dominated era? when
\begin{equation}
\rho(z)=\rho_m a^{-3}
\end{equation}
 
Has anybody seen any paper on the change of Hubble parameter with f(R)? Is there at least any approximation?
 

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