TY - JOUR
T1 - The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey
T2 - Single-probe measurements from CMASS anisotropic galaxy clustering
AU - Chuang, Chia Hsun
AU - Prada, Francisco
AU - Pellejero-Ibanez, Marcos
AU - Beutler, Florian
AU - Cuesta, Antonio J.
AU - Eisenstein, Daniel J.
AU - Escoffier, Stephanie
AU - Ho, Shirley
AU - Kitaura, Francisco Shu
AU - Kneib, Jean Paul
AU - Manera, Marc
AU - Nuza, Sebastián E.
AU - Rodríguez-Torres, Sergio
AU - Ross, Ashley
AU - Rubiño-Martín, J. A.
AU - Samushia, Lado
AU - Schlegel, David J.
AU - Schneider, Donald P.
AU - Wang, Yuting
AU - Weaver, Benjamin A.
AU - Zhao, Gongbo
AU - Brownstein, Joel R.
AU - Dawson, Kyle S.
AU - Maraston, Claudia
AU - Olmstead, Matthew D.
AU - Thomas, Daniel
N1 - Publisher Copyright:
© 2016 The Authors.
PY - 2016/10/1
Y1 - 2016/10/1
N2 - With the largest spectroscopic galaxy survey volume drawn from the SDSS-III Baryon Oscillation Spectroscopic Survey (BOSS), we can extract cosmological constraints from the measurements of redshift and geometric distortions at quasi-linear scales (e.g. above 50 h-1 Mpc). We analyse the broad-range shape of the monopole and quadrupole correlation functions of the BOSS Data Release 12 (DR12) CMASS galaxy sample, at the effective redshift z = 0.59, to obtain constraints on the Hubble expansion rate H(z), the angular- diameter distance DA(z), the normalized growth rate f(z)σ8(z), and the physical matter density Ωm h2.We obtain robust measurements by including a polynomial as the model for the systematic errors, and find it works very well against the systematic effects, e.g. ones induced by stars and seeing. We provide accurate measurements (DA(0.59)rs,fid/rs, H(0.59)rs/rs,fid, f(0.59)σ8(0.59), Ωm h2) = (1427 ± 26 Mpc, 97.3 ± 3.3 kms-1 Mpc-1, 0.488 ± 0.060, 0.135 ± 0.016), where rs is the comoving sound horizon at the drag epoch and rs,fid = 147.66 Mpc is the sound scale of the fiducial cosmology used in this study. The parameters which are not well constrained by our galaxy clustering analysis are marginalized over with wide flat priors. Since no priors from other data sets, e.g. cosmic microwave background (CMB), are adopted and no dark energy models are assumed, our results from BOSS CMASS galaxy clustering alone may be combined with other data sets, i.e. CMB, SNe, lensing or other galaxy clustering data to constrain the parameters of a given cosmological model. The uncertainty on the dark energy equation of state parameter, w, from CMB+CMASS is about 8 per cent. The uncertainty on the curvature fraction, Ωk, is 0.3 per cent. We do not find deviation from flat ΛCDM.
AB - With the largest spectroscopic galaxy survey volume drawn from the SDSS-III Baryon Oscillation Spectroscopic Survey (BOSS), we can extract cosmological constraints from the measurements of redshift and geometric distortions at quasi-linear scales (e.g. above 50 h-1 Mpc). We analyse the broad-range shape of the monopole and quadrupole correlation functions of the BOSS Data Release 12 (DR12) CMASS galaxy sample, at the effective redshift z = 0.59, to obtain constraints on the Hubble expansion rate H(z), the angular- diameter distance DA(z), the normalized growth rate f(z)σ8(z), and the physical matter density Ωm h2.We obtain robust measurements by including a polynomial as the model for the systematic errors, and find it works very well against the systematic effects, e.g. ones induced by stars and seeing. We provide accurate measurements (DA(0.59)rs,fid/rs, H(0.59)rs/rs,fid, f(0.59)σ8(0.59), Ωm h2) = (1427 ± 26 Mpc, 97.3 ± 3.3 kms-1 Mpc-1, 0.488 ± 0.060, 0.135 ± 0.016), where rs is the comoving sound horizon at the drag epoch and rs,fid = 147.66 Mpc is the sound scale of the fiducial cosmology used in this study. The parameters which are not well constrained by our galaxy clustering analysis are marginalized over with wide flat priors. Since no priors from other data sets, e.g. cosmic microwave background (CMB), are adopted and no dark energy models are assumed, our results from BOSS CMASS galaxy clustering alone may be combined with other data sets, i.e. CMB, SNe, lensing or other galaxy clustering data to constrain the parameters of a given cosmological model. The uncertainty on the dark energy equation of state parameter, w, from CMB+CMASS is about 8 per cent. The uncertainty on the curvature fraction, Ωk, is 0.3 per cent. We do not find deviation from flat ΛCDM.
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U2 - 10.1093/mnras/stw1535
DO - 10.1093/mnras/stw1535
M3 - Article
AN - SCOPUS:84988663667
SN - 0035-8711
VL - 461
SP - 3781
EP - 3793
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -