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First-Year Wilkinson Microwave Anisotropy Probe (WMAP)* Observations: Determination of Cosmological Parameters

D. N. Spergel et al 2003 ApJS 148 175-194   doi: 10.1086/377226  Help

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D. N. Spergel1, L. Verde1,2, H. V. Peiris1, E. Komatsu1, M. R. Nolta3, C. L. Bennett4, M. Halpern5, G. Hinshaw4, N. Jarosik3, A. Kogut4, M. Limon4,6, S. S. Meyer7, L. Page3, G. S. Tucker4,6,8, J. L. Weiland9, E. Wollack4 and E. L. Wright10
1 Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544
2 Chandra Postdoctral Fellow
3 Department of Physics, Jadwin Hall, Princeton, NJ 08544
4 NASA Goddard Space Flight Center, Code 685, Greenbelt, MD 20771
5 Department of Physics and Astronomy, University of British Columbia, Vancouver, BC V6T 1Z1, Canada
6 National Research Council (NRC) Fellow
7 Departments of Astrophysics and Physics, EFI, and CfCP, University of Chicago, Chicago, IL 60637
8 Department of Physics, Brown University, Providence, RI 02912
9 Science Systems and Applications, Inc. (SSAI), 10210 Greenbelt Road, Suite 600, Lanham, MD 20706
10 Department of Astronomy, UCLA, P.O. Box 951562, Los Angeles, CA 90095-1562

ABSTRACT. WMAP precision data enable accurate testing of cosmological models. We find that the emerging standard model of cosmology, a flat Λ-dominated universe seeded by a nearly scale-invariant adiabatic Gaussian fluctuations, fits the WMAP data. For the WMAP data only, the best-fit parameters are h = 0.72 ± 0.05, Ωbh2 = 0.024 ± 0.001, Ωmh2 = 0.14 ± 0.02, τ = 0.166img1.gif, ns = 0.99 ± 0.04, and σ8 = 0.9 ± 0.1. With parameters fixed only by WMAP data, we can fit finer scale cosmic microwave background (CMB) measurements and measurements of large-scale structure (galaxy surveys and the Lyα forest). This simple model is also consistent with a host of other astronomical measurements: its inferred age of the universe is consistent with stellar ages, the baryon/photon ratio is consistent with measurements of the [D/H] ratio, and the inferred Hubble constant is consistent with local observations of the expansion rate. We then fit the model parameters to a combination of WMAP data with other finer scale CMB experiments (ACBAR and CBI), 2dFGRS measurements, and Lyα forest data to find the model's best-fit cosmological parameters: h = 0.71img2.gif, Ωbh2 = 0.0224 ± 0.0009, Ωmh2 = 0.135img3.gif, τ = 0.17 ± 0.06, ns(0.05 Mpc-1) = 0.93 ± 0.03, and σ8 = 0.84 ± 0.04. WMAP's best determination of τ = 0.17 ± 0.04 arises directly from the temperature-polarization (TE) data and not from this model fit, but they are consistent. These parameters imply that the age of the universe is 13.7 ± 0.2 Gyr. With the Lyα forest data, the model favors but does not require a slowly varying spectral index. The significance of this running index is sensitive to the uncertainties in the Lyα forest.

     By combining WMAP data with other astronomical data, we constrain the geometry of the universe, Ωtot = 1.02 ± 0.02, and the equation of state of the dark energy, w < -0.78 (95% confidence limit assuming w ≥ -1). The combination of WMAP and 2dFGRS data constrains the energy density in stable neutrinos: Ωνh2 < 0.0072 (95% confidence limit). For three degenerate neutrino species, this limit implies that their mass is less than 0.23 eV (95% confidence limit). The WMAP detection of early reionization rules out warm dark matter.

Subject headings: cosmic microwave background; cosmological parameters; cosmology: observations; early universe

* WMAP is the result of a partnership between Princeton University and the NASA Goddard Space Flight Center. Scientific guidance is provided by the WMAP Science Team.

Print publication: Issue 1 (2003 September)
Received 2003 February 11, accepted for publication 2003 May 20

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