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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

Jiamin HouMax-Planck-Institut für Extraterrestrische Physik, Postfach 1312, Giessenbachstrasse 1, D-85748 Garching bei München, GermanyAriel G. SánchezMax-Planck-Institut für Extraterrestrische Physik, Postfach 1312, Giessenbachstrasse 1, D-85748 Garching bei München, GermanyA.J. RossCenter for Cosmology and Astro-Particle Physics, Ohio State University, Columbus, Ohio 43210, USAA. G. SmithIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceRichard NeveuxIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceJulian BautistaInstitute of Cosmology & Gravitation, Dennis Sciama Building, University of Portsmouth, Portsmouth PO1 3FX, UKE. BurtinIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceCheng ZhaoInstitute of Physics, Laboratory of Astrophysics, École Polytechnique Fédérale de Lausanne (EPFL), Observatoire de Sauverny, CH-1290 Versoix, SwitzerlandRomán ScoccimarroCenter for Cosmology and Particle Physics, Department of Physics, New York University, New York, NY 10003, USAKyle DawsonDepartment Physics and Astronomy, University of Utah, 115 S 1400 E, Salt Lake City, UT 84112, USAArnaud de MattiaIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceAxel de la MacorraInstituto de Física, Universidad Nacional Autónoma de México, Apdo. Postal 20-364, MéxicoHélion du Mas des BourbouxDepartment Physics and Astronomy, University of Utah, 115 S 1400 E, Salt Lake City, UT 84112, USADaniel J. EisensteinHarvard-Smithsonian Center for Astrophysics, 60 Garden St, MS-20, Cambridge, MA 02138, USAHéctor Gil-MarínInstitut de Ciències del Cosmos, Universitat de Barcelona, ICCUB, Mart’i i Franquès 1, E-08028 Barcelona, SpainBrad W. LykeUniversity of Wyoming, Department of Physics and Astronomy, 1000 E. University Ave., Laramie, WY 82071, USAFaizan G MohammadDepartment of Physics and Astronomy, University of Waterloo, Waterloo, ON N2L 3G1, CanadaEva-Maria MuellerSub-department of Astrophysics, Department of Physics, University of Oxford, Denys Wilkinson Building, Keble Road, Oxford OX1 3RH, UKWill J. PercivalDepartment of Physics and Astronomy, University of Waterloo, Waterloo, ON N2L 3G1, CanadaGraziano RossiDepartment of Physics and Astronomy, Sejong University, Seoul 143-747, KoreaM. Vargas-MagañaInstituto de Física, Universidad Nacional Autónoma de México, Apdo. Postal 20-364, MéxicoPauline ZarroukIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceGong‐Bo ZhaoInstitute of Cosmology & Gravitation, Dennis Sciama Building, University of Portsmouth, Portsmouth PO1 3FX, UKJ. BrinkmannApache Point Observatory and New Mexico State University, PO Box 59, Sunspot, NM 88349, USAJoel R. BrownsteinDepartment Physics and Astronomy, University of Utah, 115 S 1400 E, Salt Lake City, UT 84112, USAChia-Hsun ChuangKavli Institute for Particle Astrophysics and Cosmology, Stanford University, 452 Lomita Mall, Stanford, CA 94305, USAAdam D. MyersUniversity of Wyoming, Department of Physics and Astronomy, 1000 E. University Ave., Laramie, WY 82071, USAJeffrey A. NewmanPITT PACC, Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA 15260, USADonald P. SchneiderDepartment of Astronomy and Astrophysics, The Pennsylvania State University, University Park, PA 16802, USAM. VivekDepartment Physics and Astronomy, University of Utah, 115 S 1400 E, Salt Lake City, UT 84112, USA
2020en
ABI

Аннотация

ABSTRACT We 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 $8 \, h^{-1}\, {\rm Mpc}$, fσ8(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 $f\sigma _8^{{\bf c}}(z_{\rm eff}) = 0.462 \pm 0.045$.

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