2003
DOI: 10.1051/0004-6361:20031038
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Beam deconvolution in noisy CMB maps

Abstract: Abstract. The subject of this paper is beam deconvolution in small angular scale CMB experiments. The beam effect is reversed using the Jacobi iterative method, which was designed to solved systems of algebraic linear equations. The beam is a non circular one which moves according to the observational strategy. A certain realistic level of Gaussian instrumental noise is assumed. The method applies to small scale CMB experiments in general (cases A and B), but we have put particular attention on P mission … Show more

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Cited by 16 publications
(17 citation statements)
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“…Recently, deconvolution mapmaking algorithms have been developed that can produce maps in which the smoothing of the beam response has been deconvolved. These methods lead to maps that approximate the true sky (Burigana & Sáez 2003, Armitage & Wandelt 2004, Harrison et al 2008). These methods are sufficiently different from the ones considered here that different methods of comparison must be used, and we therefore do not include detailed description of them in this paper.…”
Section: Results Of Mapmakingmentioning
confidence: 99%
“…Recently, deconvolution mapmaking algorithms have been developed that can produce maps in which the smoothing of the beam response has been deconvolved. These methods lead to maps that approximate the true sky (Burigana & Sáez 2003, Armitage & Wandelt 2004, Harrison et al 2008). These methods are sufficiently different from the ones considered here that different methods of comparison must be used, and we therefore do not include detailed description of them in this paper.…”
Section: Results Of Mapmakingmentioning
confidence: 99%
“…So once a suitable basis is chosen, the rest of the analysis can be applied without requiring any major change. It may also be possible to deconvolve only a patch of the sky using a similar method [54].…”
Section: Fig 8 (Color Online)mentioning
confidence: 99%
“…At each observed position of the Leiden survey a) we first assigned the Stokes parameters corresponding to the Synfast simulation pixel in which it would project; and b) the corresponding rms given in the original table; c) we then added to each Stokes parameter a random value extracted from a Gaussian distribution in order to mimic the effect of the instrumental white noise (see, e.g., Burigana & Sáez 2003). The adopted standard deviation of this Gaussian distribution has been chosen equal to the mean error quoted for the considered original data.…”
Section: Interpolation Algorithm Optimization and Accuracymentioning
confidence: 99%