Abstract
In this paper, a specific family of $f(R)$ models that can produce the $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ background expansion history is constrained by using the currently available geometric and dynamic probes. The scale dependence of the growth rate $f(z,k)$ in this specific family of $f(R)$ model is shown. Therefore to eliminate the scale dependence of $f{\ensuremath{\sigma}}_{8}(z)$ in theory, which usually is defined as the product of $f(z,k)$ and ${\ensuremath{\sigma}}_{8}(z)$, we define $f{\ensuremath{\sigma}}_{8}(z)=d{\ensuremath{\sigma}}_{8}(z)/d\mathrm{ln}a$, which is obviously scale independent and reproduces the conventional definition in the standard $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ cosmology. In doing so, under the assumption that future probes having the same best fit values as the current ten data points of $f{\ensuremath{\sigma}}_{8}(z)$, even having 20% error bars enlarged, we find a preliminary constraint ${f}_{R0}=\ensuremath{-}2.5{8}_{\ensuremath{-}0.58}^{+2.14}\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$ in $1\ensuremath{\sigma}$ regions. This indicates the great potential that redshift space distortions have in constraining modified gravity theories. We also discuss the nonlinear matter power spectrum based on different halo fit models.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.