Testing General Relativity with Growth rate measurement from Sloan Digital Sky Survey III Baryon Oscillations Spectroscopic Survey galaxies

preprint2015arXivOpen access

Abstract

The measured redshift (zz) of an astronomical object is a combination of Hubble recession, gravitational redshift and peculiar velocity. The line of sight distance to a galaxy inferred from redshift is affected by the peculiar velocity component of galaxy redshift, which is observed as an anisotropy in the correlation function. This anisotropy allows us to measure the linear growth rate of matter (fσ8fσ_8). We measure the fσ8fσ_8 at z=0.57z=0.57 using the CMASS sample from Data Release 11 of Sloan Digital Sky Survey III (SDSS III) Baryon Oscillations Spectroscopic Survey (BOSS). The galaxy sample consists of 690,826 massive galaxies in the redshift range 0.43-0.7 covering 8498 deg2^2. Here we report the first simultaneous measurement of fσ8fσ_8 and background cosmological parameters using Convolution Lagrangian Perturbation Theory (CLPT) with Gaussian streaming model (GSRSD). We arrive at a constraint of fσ8=0.462±0.041fσ_8=0.462\pm0.041 (9\% accuracy) at effective redshift (zˉ=0.57\bar{z}=0.57) when we include Planck CMB likelihood while marginalizing over all other cosmological parameters. We also measure bσ8=1.19±0.03bσ_8=1.19\pm0.03, H(z=0.57)=89.2±3.6H(z=0.57)=89.2\pm3.6 km s−1^{-1} Mpc−1^{-1} and DA(z=0.57)=1401±23D_A(z=0.57)=1401\pm23 Mpc. Our analysis also improves the constraint on Ωch2=0.1196±0.0009Ω_c h^2=0.1196\pm0.0009 by a factor of 3 when compared to the Planck only measurement(Ωch2=0.1196±0.0031Ω_c h^2=0.1196 \pm 0.0031). Our results are consistent with Planck ΛΛCDM-GR prediction and all other CMASS measurements, even though our theoretical models are fairly different. This consistency suggests that measurement of fσ8fσ_8 from Redshift space distortions at multiple redshifts will be a sensitive probe of the theory of gravity that is largely model independent, allowing us to place model-independent constraints on alternative models of gravity.

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