D. N. Spergel et al. 2007 ApJS 170 377 doi:10.1086/513700
D. N. Spergel1,2, R. Bean1,3, O. Doré1,4, M. R. Nolta4,5, C. L. Bennett6,7, J. Dunkley1,5, G. Hinshaw6, N. Jarosik5, E. Komatsu1,8, L. Page5, H. V. Peiris1,9,10, L. Verde1,11, M. Halpern12, R. S. Hill6,13, A. Kogut6, M. Limon6, S. S. Meyer9, N. Odegard6,13, G. S. Tucker14, J. L. Weiland6,13, E. Wollack6 and E. L. Wright15
Show affiliationsA simple cosmological model with only six parameters (matter density, Ωmh2, baryon density, Ωbh2, Hubble constant, H0, amplitude of fluctuations, σ8, optical depth, τ, and a slope for the scalar perturbation spectrum, ns) fits not only the 3 year WMAP temperature and polarization data, but also small-scale CMB data, light element abundances, large-scale structure observations, and the supernova luminosity/distance relationship. Using WMAP data only, the best-fit values for cosmological parameters for the power-law flat Λ cold dark matter (ΛCDM) model are (Ωmh2,Ωbh2,h,ns,τ,σ8) = (0.1277
,0.02229 ± 0.00073,0.732
,0.958 ± 0.016,0.089 ± 0.030,0.761
). The 3 year data dramatically shrink the allowed volume in this six-dimensional parameter space. Assuming that the primordial fluctuations are adiabatic with a power-law spectrum, the WMAP data alone require dark matter and favor a spectral index that is significantly less than the Harrison-Zel'dovich-Peebles scale-invariant spectrum (ns = 1, r = 0). Adding additional data sets improves the constraints on these components and the spectral slope. For power-law models, WMAP data alone puts an improved upper limit on the tensor-to-scalar ratio, r0.002 < 0.65 (95% CL) and the combination of WMAP and the lensing-normalized SDSS galaxy survey implies r0.002 < 0.30 (95% CL). Models that suppress large-scale power through a running spectral index or a large-scale cutoff in the power spectrum are a better fit to the WMAP and small-scale CMB data than the power-law ΛCDM model; however, the improvement in the fit to the WMAP data is only Δχ2 = 3 for 1 extra degree of freedom. Models with a running-spectral index are consistent with a higher amplitude of gravity waves. In a flat universe, the combination of WMAP and the Supernova Legacy Survey (SNLS) data yields a significant constraint on the equation of state of the dark energy, w = -0.967
. If we assume w = -1, then the deviations from the critical density, ΩK, are small: the combination of WMAP and the SNLS data implies Ωk = -0.011 ± 0.012. The combination of WMAP 3 year data plus the HST Key Project constraint on H0 implies Ωk = -0.014 ± 0.017 and ΩΛ = 0.716 ± 0.055. Even if we do not include the prior that the universe is flat, by combining WMAP, large-scale structure, and supernova data, we can still put a strong constraint on the dark energy equation of state, w = -1.08 ± 0.12. For a flat universe, the combination of WMAP and other astronomical data yield a constraint on the sum of the neutrino masses,
mν < 0.66 eV (95%CL). Consistent with the predictions of simple inflationary theories, we detect no significant deviations from Gaussianity in the CMB maps using Minkowski functionals, the bispectrum, trispectrum, and a new statistic designed to detect large-scale anisotropies in the fluctuations.
Issue 2 (2007 June)
Received 2006 March 16, accepted for publication 2007 January 12
D. N. Spergel et al. 2007 ApJS 170 377
R.J. Taylor et al 2005 Nucl. Fusion 45 1634
John D Owens 2007 J. Phys.: Conf. Ser. 78 012055