Exploring two-spin internal linear combinations for the recovery of the CMB polarization
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Identificadores
URI: https://hdl.handle.net/10902/34479DOI: 10.1093/mnras/stw670
ISSN: 0035-8711
ISSN: 1365-2966
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Fernández Cobos, Raúl


Fecha
2011-06Derechos
This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society ©: 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.
Publicado en
Monthly Notices of the Royal Astronomical Society, 2016, 459(1), 441-454
Editorial
Oxford University Press
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Palabras clave
Polarization
Methods: data analysis
Cosmic background radiation
Resumen/Abstract
We present a methodology to recover cosmic microwave background (CMB) polarization in
which the quantity P = Q + iU is linearly combined at different frequencies using complex
coefficients. This is the most general linear combination of the Q and U Stokes parameters
which preserves the physical coherence of the residual contribution on the CMB estimation.
The approach is applied to the internal linear combination (ILC) and the internal template
fitting (ITF) methodologies. The variance of P of the resulting map is minimized to compute
the coefficients of the linear combination. One of the key aspects of this procedure is that it
serves to account for a global frequency-dependent shift of the polarization phase. Although
in the standard case, in which no global E-B transference depending on frequency is expected in the foreground components, minimizing |P|² is similar to minimizing Q² and U²
separately (as previous methodologies proceed), multiplying Q and U by different coefficients
induces arbitrary changes in the polarization angle and it does not preserve the coherence
between the spinorial components. The approach is tested on simulations, obtaining a similar
residual level with respect to the one obtained with other implementations of the ILC, and
perceiving the polarization rotation of a toy model with the frequency dependence of the
Faraday rotation.
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