Difference between revisions of "Galactic stray light removal"
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The polarized signal from synchrotron and thermal emission from dust was included in the computation. | The polarized signal from synchrotron and thermal emission from dust was included in the computation. | ||
− | The convolution was performed transforming the maps into spherical harmonics using | + | The convolution was performed transforming the maps into spherical harmonics using HEALPix Anafast {{BibCite|gorski2005}} with <math>l_{max}= 2048</math>, and combining the spherical harmonic coefficients <math>a_{lm}</math> using the LevelS totalconvolver.cxx. For each sample in the timeline the straylght was computed with a linear |
interpolation on the straylight ringset, given the corresponding pointing coordinates <math>(θ, φ)</math> and the orientation <math>ψ</math> of the beam. | interpolation on the straylight ringset, given the corresponding pointing coordinates <math>(θ, φ)</math> and the orientation <math>ψ</math> of the beam. |
Revision as of 10:55, 15 December 2014
The pickup of the Galactic signal through the sidelobes causes two kinds of systematic errors:
1. It introduces a bias in the calibration process.
2. It leaves a spurious signal in the calibrated map.
The first error is corrected including an estimate of the Galactic sidelobe pickup alongside the convolved dipole in the fit with the measured voltages. The beam pattern is decomposed into
- ,
and our estimate the gain
is given through a linear least-squares fit between the voltages and , defined as- .
The term
is neglected in the fit because during the calibration we mask the Galactic plane, and we assume that the contribution to the fit given by the terms with is negligible.The second error is corrected subtracting the residual signal caused by Galactic pickup through the sidelobes from the timelines immediately after voltages have been calibrated into temperatures.
was estimated using temperature and polarization maps from the Full Focal Plane simulation 7.
The included components were:
1. Synchrotron diffuse emission
2. Thermal and anomalous diffuse emission from dust
3. Thomson scattering diffuse emission
4. Faint and strong radio sources
5. Thermal and kinetic SZ sources
The polarized signal from synchrotron and thermal emission from dust was included in the computation.
The convolution was performed transforming the maps into spherical harmonics using HEALPix Anafast [1] with , and combining the spherical harmonic coefficients using the LevelS totalconvolver.cxx. For each sample in the timeline the straylght was computed with a linear
interpolation on the straylight ringset, given the corresponding pointing coordinates
and the orientation of the beam.- ↑ HEALPix: A Framework for High-Resolution Discretization and Fast Analysis of Data Distributed on the Sphere, K. M. Górski, E. Hivon, A. J. Banday, B. D. Wandelt, F. K. Hansen, M. Reinecke, M. Bartelmann, ApJ, 622, 759-771, (2005).
Cosmic Microwave background
Sunyaev-Zel'dovich
(Hierarchical Equal Area isoLatitude Pixelation of a sphere, <ref name="Template:Gorski2005">HEALPix: A Framework for High-Resolution Discretization and Fast Analysis of Data Distributed on the Sphere, K. M. Górski, E. Hivon, A. J. Banday, B. D. Wandelt, F. K. Hansen, M. Reinecke, M. Bartelmann, ApJ, 622, 759-771, (2005).