Wilkinson Microwave Anisotropy Probe
The main and near-sidelobe response of each of the 20 WMAP antenna feeds
has been mapped in-flight using observations of Jupiter. The 7-year release
is comprised of 13 Jupiter observing seasons:
Oct/Nov 2001
Feb/Mar 2002
Nov/Dec 2002
Mar/Apr 2003
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Dec 2003/Jan 2004
Apr/May 2004
Jan/Feb 2005
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May/Jun 2005
Feb/Mar 2006
Jun/Jul 2006
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Mar/Apr 2007
Jul/Aug 2007
Apr/May 2008
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As a prelude to beam analysis, an archive of calibrated time-ordered observations is constructed,
consisting of Jupiter passages within roughly 7.0, 5.5, 5.0, 4.0 and 3.5 degrees of either the
A- or B-side beam center for K, Ka, Q, V and W bands respectively.
The time-ordered observations are corrected to a fiducial Jupiter distance of 5.2 AU, background
subtracted and corrected for aberration. To constrain low signal-to-noise beam pedestals,
a hybrid TOD archive is then constructed in which model predictions (Hill et al. 2008) are
substituted for data at the 3,4,6,7 and 10 dBi levels of K,Ka,Q,V and W respectively.
This hybrid beam archive serves as the basis for beam map and window function analysis.
For purposes of constructing beam maps,
the data in the hybrid beam TOD archive are assigned to 2.4 arcminute bins on a coordinate grid
centered on either the A or B-side focal plane axis. The beam response for each
feed is computed from the average temperature in each bin. No correction
has been made for the side-A vs. side-B input transmission imbalance.
These beam maps are convenient for some applications, but are not used in the computation of
the flight beam transfer functions. The 2.4 arcminute binning acts as a smoothing kernel which
filters high frequency spatial content. The pixelization transfer function
may be estimated from the Legendre transform of the symmetrized radial profile of the
binning kernel. Assuming a square pixel of 0.04 degrees on a side centered on
the origin, the symmetrized radial profile of the binning function may be represented as
| f(r) | = 1.0 | for r < R |
| = 1.0 - (4/pi)*acos(R/r) | for R <= r <= R*sqrt2 |
where R = 0.02 deg.
Both the pixelization profile and pixelization transfer function are
provided as a useful reminder of the limitations of the 2.4 arcminute binning.
Beam maps are provided in 10 FITS image format files, one file for each
differencing assembly. Each file contains:
- the beam map for the A side, in mK (antenna temperature)
- the statistical error of each bin of the A side beam map, in mK (antenna temperature).
The statistical error is based on the number of observations in each bin.
Model points are assigned 100% error.
- the beam map for the B side, in mK (antenna temperature)
- the statistical error of each pixel of the B side beam map, in mK (antenna temperature)
Model points are assigned 100% error.
The beam coordinates form an equal area rectangular coordinate system centered on
the optic axis of the spacecraft. They are related to coordinates theta (elevation from optic
axis) and phi (azimuth about optic axis) as follows:
- Xbeam = 2*sin(theta/2) * cos(phi)
- Ybeam = 2*sin(theta/2) * sin(phi)
The "optic axis" of the spacecraft is elevated by 19.5 degrees from the S/C XY
plane and lies within the S/C YZ plane. Although this vector
is close to the S/C Y axis (+ or - depending on A or B side), it
becomes the Z axis of the focal plane coordinate system.
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For each differencing assembly, an azimuthally symmetrized radial beam
profile is computed by binning the ensemble of individual A- and B- side
hybridized Jupiter observations. A constant bin size of 0.25 arcmin is used,
and the straight mean of all hybrid samples within a radial bin represents
the value for that bin.
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Beam transfer functions are computed from the Legendre transform of the
binned hybrid radial beam profile. The window function applicable to power
spectra is the square of the beam transfer function.
Beam transfer functions are presented as ASCII tables, with the first
column being multipole moment l and the second column the transfer
function (amplitude) normalized to 1.0 at l=1.
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Additional Information