Component separation methods for the PLANCK mission

被引:198
作者
Leach, S. M. [1 ,2 ]
Cardoso, J. -F. [3 ,4 ,5 ,6 ]
Baccigalupi, C. [1 ,2 ]
Barreiro, R. B. [7 ]
Betoule, M. [3 ,4 ]
Bobin, J. [8 ]
Bonaldi, A. [9 ,10 ]
Delabrouille, J. [3 ,4 ]
de Zotti, G. [1 ,9 ]
Dickinson, C. [11 ]
Eriksen, H. K. [12 ,13 ]
Gonzalez-Nuevo, J. [1 ]
Hansen, F. K. [12 ,13 ]
Herranz, D. [7 ]
Le Jeune, M. [3 ,4 ]
Lopez-Caniego, M. [14 ]
Martinez-Gonzalez, E. [7 ]
Massardi, M. [1 ]
Melin, J. -B. [15 ]
Miville-Deschenes, M. -A. [16 ]
Patanchon, G. [3 ,4 ]
Prunet, S. [17 ]
Ricciardi, S. [9 ,18 ]
Salerno, E. [19 ]
Sanz, J. L. [7 ]
Starck, J. -L. [8 ]
Stivoli, F. [1 ,2 ]
Stolyarov, V. [14 ]
Stompor, R. [3 ,4 ]
Vielva, P. [7 ]
机构
[1] SISSA, ISAS, Astrophys Sector, I-34014 Trieste, Italy
[2] Ist Nazl Fis Nucl, Sez Trieste, I-34014 Trieste, Italy
[3] CNRS, F-75205 Paris 13, France
[4] Univ Paris 07, Lab APC, F-75205 Paris 13, France
[5] CNRS, Lab Traitement & Commun Informat, F-75634 Paris, France
[6] Telecom ParisTech, F-75634 Paris, France
[7] CSIC UC, Inst Fis Cantabria, Santander 39005, Spain
[8] CEA Saclay, SEDI Serv Astrophys, F-91191 Gif Sur Yvette, France
[9] INAF Osservatorio Astron Padova, I-35122 Padua, Italy
[10] Dipartimento Astron, I-35122 Padua, Italy
[11] CALTECH, Ctr Infrared Proc & Anal, Pasadena, CA 91125 USA
[12] Univ Oslo, Inst Theoret Astrophys, N-0315 Oslo, Norway
[13] Univ Oslo, Ctr Math Applicat, N-0316 Oslo, Norway
[14] Cavevdish Lab, Astrophys Grp, Cambridge CB3 0HE, England
[15] CEA Saclay, DSM,Irfu,SPP, F-91191 Gif Sur Yvette, France
[16] Inst Astrophys Spatiale, F-91405 Orsay, France
[17] Inst Astrophys, F-75014 Paris, France
[18] Univ Calif Berkeley, Lawrence Berkeley Lab, Computat Cosmol Ctr, Space Sci Lab, Berkeley, CA 94720 USA
[19] CNR, Ist Sci & Technol Informaz, Area Ric, I-56124 Pisa, Italy
基金
英国科学技术设施理事会;
关键词
cosmology: cosmic microwave background; methods: data analysis;
D O I
10.1051/0004-6361:200810116
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Context. The PLANCK satellite will map the full sky at nine frequencies from 30 to 857 GHz. The CMB intensity and polarization that are its prime targets are contaminated by foreground emission. Aims. The goal of this paper is to compare proposed methods for separating CMB from foregrounds based on their different spectral and spatial characteristics, and to separate the foregrounds into "components" with different physical origins (Galactic synchrotron, free-free and dust emissions; extra-galactic and far-IR point sources; Sunyaev-Zeldovich effect, etc.). Methods. A component separation challenge has been organised, based on a set of realistically complex simulations of sky emission. Several methods including those based on internal template subtraction, maximum entropy method, parametric method, spatial and harmonic cross correlation methods, and independent component analysis have been tested. Results. Different methods proved to be effective in cleaning the CMB maps of foreground contamination, in reconstructing maps of diffuse Galactic emissions, and in detecting point sources and thermal Sunyaev-Zeldovich signals. The power spectrum of the residuals is, on the largest scales, four orders of magnitude lower than the input Galaxy power spectrum at the foreground minimum. The CMB power spectrum was accurately recovered up to the sixth acoustic peak. The point source detection limit reaches 100 mJy, and about 2300 clusters are detected via the thermal SZ effect on two thirds of the sky. We have found that no single method performs best for all scientific objectives. Conclusions. We foresee that the final component separation pipeline for planck will involve a combination of methods and iterations between processing steps targeted at different objectives such as diffuse component separation, spectral estimation, and compact source extraction.
引用
收藏
页码:597 / 615
页数:19
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