Map-making in small field modulated CMB polarisation experiments: approximating the maximum-likelihood method

Details Map-making in small field modulated CMB polarisation experiments: approximating the maximum-likelihood method Map-making in small field modulated CMB polarisation experiments: approximating the maximum-likelihood method

2008-07-23

arxiv.org/abs/0807.3658v2

MNRAS 393, 894-910 (2009)

Astronomy and Astrophysics

Astrophysics

18 pages, 17 figures, MNRAS accepted v2: content added (inc: table 2), typos corrected

Scientific paper

10.1111/j.1365-2966.2008.14195.x

Map-making presents a significant computational challenge to the next generation of kilopixel CMB polarisation experiments. Years worth of time ordered data (TOD) from thousands of detectors will need to be compressed into maps of the T, Q and U Stokes parameters. Fundamental to the science goal of these experiments, the observation of B-modes, is the ability to control noise and systematics. In this paper, we consider an alternative to the maximum-likelihood method, called destriping, where the noise is modelled as a set of discrete offset functions and then subtracted from the time-stream. We compare our destriping code (Descart: the DEStriping CARTographer) to a full maximum-likelihood map-maker, applying them to 200 Monte-Carlo simulations of time-ordered data from a ground based, partial-sky polarisation modulation experiment. In these simulations, the noise is dominated by either detector or atmospheric 1/f noise. Using prior information of the power spectrum of this noise, we produce destriped maps of T, Q and U which are negligibly different from optimal. The method does not filter the signal or bias the E or B-mode power spectra. Depending on the length of the destriping baseline, the method delivers between 5 and 22 times improvement in computation time over the maximum-likelihood algorithm. We find that, for the specific case of single detector maps, it is essential to destripe the atmospheric 1/f in order to detect B-modes, even though the Q and U signals are modulated by a half-wave plate spinning at 5-Hz.

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