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CMB Broad-Band Power Spectrum Estimation

Astrophysics 2009-09-25 v1

Abstract

The natural outcome of theoretical calculations of microwave background anisotropy is the angular power spectrum C{\cal C}_\ell as a function of multipole number \ell. Experimental C{\cal C}_\ell's are needed for direct comparison. Estimation procedures using statistics linear in the pixel amplitudes as well as the conventional but less useful quadratic combinations are described. For most current experiments, a single broad-band power amplitude is all that one can get with accuracy. Results are given for the Capri-meeting detections. Mapping experiments, sensitive to many base-lines, can also give spectral ``colour'' information, either with a series of contiguous narrow-band powers or as parameterized by a local ``colour'' index nΔTn_{\Delta T} (scale invariant is -2, white noise is 0). Bayesian analyses of the full first year DMR and FIRS maps give very similar band-powers (\eg Qrms,PS=17.9±2.9μKQ_{rms,PS}=17.9 \pm 2.9 \mu K {\it c.f.} 18.6±4.7μK18.6 \pm 4.7 \mu K for nΔT=2n_{\Delta T}=-2) and colour indices (with 1 and 2 sigma error bars) nΔT+3=2.00.4;1.0+0.4;+0.7n_{\Delta T}+3=2.0^{+0.4;+0.7}_{-0.4;-1.0} and 1.80.8;1.3+0.6;+0.9 1.8^{+0.6;+0.9}_{-0.8;-1.3} ({\it c.f.} the value 1.15 for a ``standard'' scale invariant CDM model). The 53 and 90 GHz DMR maps, as well as the FIRS map, have residual short-distance noise which steepens nΔTn_{\Delta T}. Allowing the pixel error bars to increase absorbs much of the residual, but further exploration is needed to see if a second residual evident in the data which is responsible for the high nΔTn_{\Delta T} is from systematic errors or is physical.

Keywords

Cite

@article{arxiv.astro-ph/9402043,
  title  = {CMB Broad-Band Power Spectrum Estimation},
  author = {J. Richard Bond},
  journal= {arXiv preprint arXiv:astro-ph/9402043},
  year   = {2009}
}

Comments

11 pages, LaTeX, uses revtex; 3 postscript figs, capri_powf*.eps, via anonymous ftp to ftp.cita.utoronto.ca, cd to /pub/dick/capri; CITA-94-5

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