F(R) gravity and the Hubble parameter

AI Thread Summary
The discussion focuses on the implications of f(R) gravity on the Friedmann equations and the Hubble parameter. The user seeks assistance in solving the modified equations derived from the Einstein field equations, particularly the complexities introduced by the terms involving the scale factor's second derivative. They express difficulty in handling the fourth-order terms and inquire about the solvability of these equations during the matter-dominated era. Additionally, they request references to existing literature on the changes in the Hubble parameter due to f(R) modifications and any potential approximations. The conversation highlights the challenges in applying f(R) gravity to cosmological models.
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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