Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Angular Power Spectra
M. R. Nolta, J. Dunkley, R. S. Hill, G. Hinshaw, E. Komatsu, D. Larson, L. Page, D. N. Spergel, C. L. Bennett, B. Gold, N. Jarosik, N. Odegard, J. L. Weiland, E. Wollack, M. Halpern, A. Kogut, M. Limon, S. S. Meyer, G. S. Tucker, E. L. Wright
TL;DR
The paper reports the 5-year WMAP measurements of the CMB temperature and polarization power spectra, detailing improvements in calibration, beams, and foreground treatment that yield a TT spectrum cosmic-variance limited up to $\ell \approx 530$ and a clearly detected TE signal. A refined unresolved point-source correction with amplitude $A_{ps}=0.011\pm0.001\,\mu{\rm K}^2{\rm sr}$ is applied, and the data favor a six-parameter $\Lambda$CDM model with $\chi^2/\nu \approx 1.06$ over $\ell=33-1000$. The EE spectrum shows a robust reionization signature near $\tau=0.089$, while BB remains consistent with zero, placing a stringent upper limit on primordial B-modes. Overall, the 5-year results tighten cosmological constraints, validate the $\Lambda$CDM framework, and provide publicly accessible data and likelihood tools for the community.
Abstract
We present the temperature and polarization angular power spectra of the cosmic microwave background (CMB) derived from the first 5 years of WMAP data. The 5-year temperature (TT) spectrum is cosmic variance limited up to multipole l=530, and individual l-modes have S/N>1 for l<920. The best fitting six-parameter LambdaCDM model has a reduced chi^2 for l=33-1000 of chi^2/nu=1.06, with a probability to exceed of 9.3%. There is now significantly improved data near the third peak which leads to improved cosmological constraints. The temperature-polarization correlation (TE) is seen with high significance. After accounting for foreground emission, the low-l reionization feature in the EE power spectrum is preferred by Δχ^2=19.6 for optical depth tau=0.089 by the EE data alone, and is now largely cosmic variance limited for l=2-6. There is no evidence for cosmic signal in the BB, TB, or EB spectra after accounting for foreground emission. We find that, when averaged over l=2-6, l(l+1)C^{BB}_l/2π< 0.15 uK^2 (95% CL).
