4.7 Article

The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey: single-probe measurements and the strong power of f(z)Σ8(z) on constraining dark energy

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stt988

关键词

cosmological parameters; cosmology: observations; distance scale; large-scale structure of Universe

资金

  1. Spanish MICINN [MultiDarkCSD2009-00064, AYA201021231- C02-01]
  2. Comunidad de Madrid [HEPHACOS S2009/ESP-1473]
  3. NASA Office of Space Science
  4. ICG
  5. SEPNet
  6. University of Portsmouth
  7. Alfred P. Sloan Foundation
  8. National Science Foundation
  9. U.S. Department of Energy Office of Science
  10. University of Arizona
  11. Brookhaven National Laboratory
  12. University of Cambridge
  13. Carnegie Mellon University
  14. University of Florida
  15. Harvard University
  16. Instituto de Astrofisica de Canarias
  17. Johns Hopkins University
  18. Lawrence Berkeley National Laboratory
  19. Max Planck Institute for Astrophysics
  20. Max Planck Institute for Extraterrestrial Physics
  21. New Mexico State University
  22. New York University
  23. Ohio State University
  24. Pennsylvania State University
  25. Princeton University
  26. University of Tokyo
  27. University of Utah
  28. Vanderbilt University
  29. University of Virginia
  30. University of Washington
  31. Yale University
  32. STFC [ST/K00090X/1] Funding Source: UKRI
  33. Science and Technology Facilities Council [ST/K00090X/1] Funding Source: researchfish

向作者/读者索取更多资源

We present measurements of the anisotropic galaxy clustering from the Data Release 9 (DR9) CMASS sample of the Sloan Digital Sky Survey (SDSS)-III Baryon Oscillation Spectroscopic Survey (BOSS). We analyse the broad-range shape of the monopole and quadrupole correlation functions to obtain constraints, at the effective redshift z = 0.57 of the sample, on the Hubble expansion rate H(z), the angular-diameter distance D-A(z), the normalized growth rate f (z)Sigma(8)(z), the physical matter density (m)h(2), and the biased amplitude of matter fluctuation b Sigma(8)(z). We obtain H(0.57), D-A(0.57), f (0.57)Sigma(8)(0.57), (m)h(2), b Sigma(8)(0.57) = 87.6_-6.8 boolean AND+6.7 kms(-1) Mpc(-1), 1396 +/- 73 Mpc, 0.428 +/- 0.066,0.126_-0.010+0.008, 1.19 +/- 0.14} and their covariance matrix as well. 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 [i.e. 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. We show that the major power on constraining dark energy from the anisotropic galaxy clustering signal, as compared to the angular-averaged one (monopole), arises from including the normalized growth rate f (z)Sigma(8)(z). In the case of the cosmological model assuming a constant dark energy equation of state and a flat universe (wCDM), our single-probe CMASS constraints, combined with CMB (WMAP9+SPT), yield a value for the dark energy equation-of-state parameter of w = -0.90 +/- 0.11. Therefore, it is important to include f (z)Sigma(8)(z) while investigating the nature of dark energy with current and upcoming large-scale galaxy surveys.

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