A pixelated signal f(p) is the average within each pixel p (with surface
) of the underlying signal
However, complete analysis of a pixelated map with the exact wlm(p)
defined above would be computationally intractable (because of azimutal
variation of pixel shape over the polar caps of the HEALPix grid),
and some simplifying asumptions have to be
made. If the pixel is small compared to the signal correlation length
(determined by the beam size), the exact structure of the pixel can be ignored
in the subsequent analysis and we can assume
|wlm(p) = wl(p) Ylm(p)||(32)|
If we assume all the pixels to be identical, the power spectrum of the
, is related to the hypothetical unpixelated
The pixel window functions are now available for both temperature and polarization.
For , those window functions are computed exactly using Eqs. (33) and (35). For the calculations are too costly to be done exactly at all l. The temperature windows are extrapolated from the case assuming a scaling in l similar to the one exhibited by the window of a tophat pixel. The polarization windows are assumed to be proportional to those for temperature, with a proportionality factor given by the exact calculation of wl at low l.
Because of a change of the extrapolation scheme used, the temperature window functions provided with HEALPix 1.2 and higher for are slighty different from those provided with HEALPix 1.1. For a given , the relative difference increases almost linearly with l, and is of the order of at and at .
Version 3.31, 2017-01-06