Abstract

We study Modified Gravity (MG) theories by modelling the redshifted matter power spectrum in a spherical Fourier-Bessel (sFB) basis. We use a fully non-linear description of the real-space matter power-spectrum and include the lowest-order redshift-space correction (Kaiser effect), taking into account some additional non-linear contributions. Ignoring relativistic corrections, which are not expected to play an important role for a shallow survey, we analyse two different modified gravity scenarios, namely the generalised Dilaton scalar-tensor theories and the f(R)f({R}) models in the large curvature regime. We compute the 3D power spectrum Cℓs(k1,k2){\cal C}^s_{\ell}(k_1,k_2) for various such MG theories with and without redshift space distortions, assuming precise knowledge of background cosmological parameters. Using an all-sky spectroscopic survey with Gaussian selection function φ(r)∝exp⁡(−r2/r02)φ(r)\propto \exp(-{r^2 / r^2_0}), r0=150 h−1 Mpcr_0 = 150 \, h^{-1} \, {\textrm{Mpc}}, and number density of galaxies Nˉ=10−4  Mpc−3\bar {\textrm{N}} =10^{-4}\;{\textrm{Mpc}}^{-3}, we use a χ2χ^2 analysis, and find that the lower-order (ℓ≤25)(\ell \leq 25) multipoles of Cℓs(k,k′){\cal C}^s_\ell(k,k') (with radial modes restricted to k<0.2 h Mpc−1k < 0.2 \, h \,{\textrm{Mpc}}^{-1}) can constraint the parameter fR0f_{R_0} at a level of 2×10−5(3×10−5)2\times 10^{-5} (3\times 10^{-5}) with 3σ3 σ confidence for n=1(2)n=1(2). Combining constraints from higher ℓ>25\ell > 25 modes can further reduce the error bars and thus in principle make cosmological gravity constraints competitive with solar system tests. However this will require an accurate modelling of non-linear redshift space distortions. Using a tomographic β(a)β(a)-m(a)m(a) parameterization we also derive constraints on specific parameters describing the Dilaton models of modified gravity.

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