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The completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: BAO and RSD measurements from anisotropic clustering analysis of the quasar sample in configuration space between redshift 0.8 and 2.2

AutorHou, Jiamin; Sánchez, Ariel G.; Ross, Ashley J.; Smith, Alex; Neveux, Richard; Burtin, Etienne; Zhao, Cheng; Scoccimarro, Román CSIC; Dawson, Kyle; Mattia, Arnaud de; Macorra, Axel de la; Bourboux, H.d.M.d.; Eisenstein, Daniel J.; Gil-Marín, Héctor CSIC; Lyke, Brad W.; Mohammad, Faizan G.; Mueller, Eva-Maria; Percival, Will J.; Rossi, Graziano; Vargas Magaña, Mariana; Zarrouk, Pauline; Zhao, Gong-Bo; Brinkmann, Jonathan; Brownstein, Joel R.; Chuang, Chia-Hsun; Myers, Adam D.; Newman, Jeffrey A.; Schneider, Donald P.; Vivek, Mariappan
Palabras claveMethods: data analysis
Quasars: general
Cosmology: observations
Cosmology: dark energy
Cosmology: distance scale
Fecha de publicación23-oct-2020
EditorOxford University Press
CitaciónMonthly Notices of the Royal Astronomical Society 500(1): 1201-1221 (2021)
ResumenWe measure the anisotropic clustering of the quasar sample from Data Release 16 (DR16) of the Sloan Digital Sky Survey IV extended Baryon Oscillation Spectroscopic Survey (eBOSS). A sample of 343 708 spectroscopically confirmed quasars between redshift 0.8 < z < 2.2 are used as tracers of the underlying dark matter field. In comparison with DR14 sample, the final sample doubles the number of objects as well as the survey area. In this paper, we present the analysis in configuration space by measuring the two-point correlation function and decomposing it using the Legendre polynomials. For the full-shape analysis of the Legendre multipole moments, we measure the baryon acoustic oscillation (BAO) distance and the growth rate of the cosmic structure. At an effective redshift of zeff = 1.48, we measure the comoving angular diameter distance DM(zeff)/rdrag = 30.66 ± 0.88, the Hubble distance DH(zeff)/rdrag = 13.11 ± 0.52, and the product of the linear growth rate and the rms linear mass fluctuation on scales of $8 \, h{-1}\, {\rm Mpc}$, f?8(zeff) = 0.439 ± 0.048. The accuracy of these measurements is confirmed using an extensive set of mock simulations developed for the quasar sample. The uncertainties on the distance and growth rate measurements have been reduced substantially (?45 and ?30 per cent) with respect to the DR14 results. We also perform a BAO-only analysis to cross check the robustness of the methodology of the full-shape analysis. Combining our analysis with the Fourier-space analysis, we arrive at $D{{\bf c}}-{\rm M}(z-{\rm eff})/r-{\rm drag} = 30.21 \pm 0.79$, $D{{\bf c}}-{\rm H}(z-{\rm eff})/r-{\rm drag} = 13.23 \pm 0.47$, and $f\sigma-8{{\bf c}}(z-{\rm eff}) = 0.462 \pm 0.045$.
Versión del editorhttp://doi.org/10.1093/mnras/staa3234
URIhttp://hdl.handle.net/10261/249679
DOI10.1093/mnras/staa3234
Identificadoresdoi: 10.1093/mnras/staa3234
issn: 1365-2966
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