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Published November 2014 | public
Journal Article

Planck 2013 results. XXXI. Consistency of the Planck data

Ade, P. A. R. ORCID icon
Arnaud, M.
Ashdown, M.
Aumont, J. ORCID icon
Baccigalupi, C. ORCID icon
Banday, A. J.
Barreiro, R. B. ORCID icon
Battaner, E.
Benabed, K.
Benoit-Lévy, A.
Bernard, J.-P.
Bersanelli, M.
Bielewicz, P.
Bond, J. R. ORCID icon
Borrill, J.
Bouchet, F. R. ORCID icon
Burigana, C. ORCID icon
Cardoso, J.-F.
Catalano, A. ORCID icon
Challinor, A.
Chamballu, A.
Chiang, H. C. ORCID icon
Christensen, P. R. ORCID icon
Clements, D. L. ORCID icon
Colombi, S.
Colombo, L. P. L. ORCID icon
Couchot, F.
Coulais, A.
Crill, B. P. ORCID icon
Curto, A.
Cuttaia, F.
Danese, L.
Davies, R. D.
Davis, R. J.
de Bernardis, P. ORCID icon
De Rosa, A. ORCID icon
de Zotti, G. ORCID icon
Delabrouille, J.
Désert, F.-X. ORCID icon
Dickinson, C. ORCID icon
Diego, J. M. ORCID icon
Dole, H.
Donzelli, S.
Doré, O. ORCID icon
Douspis, M.
Dupac, X.
Enßlin, T. A.
Eriksen, H. K. ORCID icon
Finelli, F. ORCID icon
Forni, O. ORCID icon
Frailis, M. ORCID icon
Fraisse, A. A.
Franceschi, E. ORCID icon
Galeotta, S. ORCID icon
Ganga, K.
Giard, M.
González-Nuevo, J.
Górski, K. M. ORCID icon
Gratton, S.
Gregorio, A.
Gruppuso, A.
Gudmundsson, J. E. ORCID icon
Hansen, F. K.
Hanson, D.
Harrison, D. L. ORCID icon
Henrot-Versillé, S.
Herranz, D.
Hildebrandt, S. R. ORCID icon
Hivon, E. ORCID icon
Hobson, M. ORCID icon
Holmes, W. A.
Hornstrup, A.
Hovest, W.
Huffenberger, K. M. ORCID icon
Jaffe, A. H.
Jaffe, T. R.
Jones, W. C. ORCID icon
Keihänen, E. ORCID icon
Keskitalo, R.
Knoche, J.
Kunz, M. ORCID icon
Kurki-Suonio, H. ORCID icon
Lagache, G. ORCID icon
Lähteenmäki, A. ORCID icon
Lamarre, J.-M.
Lasenby, A.
Lawrence, C. R. ORCID icon
Leonardi, R.
León-Tavares, J.
Lesgourgues, J.
Liguori, M.
Lilje, P. B. ORCID icon
Linden-Vørnle, M.
López-Caniego, M.
Lubin, P. M.
Macías-Pérez, J. F.
Maino, D. ORCID icon
Mandolesi, N.
Maris, M.
Martin, P. G. ORCID icon
Martínez-González, E.
Masi, S. ORCID icon
Matarrese, S.
Mazzotta, P. ORCID icon
Meinhold, P. R.
Melchiorri, A.
Mendes, L.
Mennella, A. ORCID icon
Migliaccio, M.
Mitra, S.
Miville-Deschênes, M.-A. ORCID icon
Moneti, A.
Montier, L.
Morgante, G.
Mortlock, D.
Moss, A.
Munshi, D.
Murphy, J. A.
Naselsky, P.
Nati, F. ORCID icon
Natoli, P.
Nørgaard-Nielsen, H. U.
Noviello, F.
Novikov, D.
Novikov, I.
Oxborrow, C. A.
Pagano, L.
Pajot, F.
Paoletti, D.
Partridge, B.
Pasian, F.
Patanchon, G.
Pearson, D.
Pearson, T. J. ORCID icon
Perdereau, O.
Perrotta, F.
Piacentini, F. ORCID icon
Piat, M.
Pierpaoli, E. ORCID icon
Pietrobon, D.
Plaszczynski, S.
Pointecouteau, E.
Polenta, G. ORCID icon
Ponthieu, N.
Popa, L.
Pratt, G. W.
Prunet, S.
Puget, J.-L.
Rachen, J. P.
Reinecke, M.
Remazeilles, M.
Renault, C.
Ricciardi, S.
Ristorcelli, I.
Rocha, G. ORCID icon
Roudier, G. ORCID icon
Rubino-Martin, J. A. ORCID icon
Rusholme, B. ORCID icon
Sandri, M.
Scott, D.
Stolyarov, V.
Sudiwala, R.
Sutton, D.
Suur-Uski, A.-S.
Sygnet, J.-F.
Tauber, J. A.
Terenzi, L.
Toffolatti, L.
Tomasi, M. ORCID icon
Tristram, M.
Tucci, M.
Valenziano, L. ORCID icon
Valiviita, J. ORCID icon
Van Tent, B.
Vielva, P.
Villa, F.
Wade, L. A. ORCID icon
Wandelt, B. D. ORCID icon
Wehus, I. K. ORCID icon
White, S. D. M. ORCID icon
Yvon, D.
Zacchei, A.
Zonca, A. ORCID icon
Planck Collaboration

Abstract

The Planck design and scanning strategy provide many levels of redundancy that can be exploited to provide tests of internal consistency. One of the most important is the comparison of the 70 GHz (amplifier) and 100 GHz (bolometer) channels. Based on different instrument technologies, with feeds located differently in the focal plane, analysed independently by different teams using different software, and near the minimum of diffuse foreground emission, these channels are in effect two different experiments. The 143 GHz channel has the lowest noise level on Planck, and is near the minimum of unresolved foreground emission. In this paper, we analyse the level of consistency achieved in the 2013 Planck data. We concentrate on comparisons between the 70, 100, and 143 GHz channel maps and power spectra, particularly over the angular scales of the first and second acoustic peaks, on maps masked for diffuse Galactic emission and for strong unresolved sources. Difference maps covering angular scales from 8° to 15′ are consistent with noise, and show no evidence of cosmic microwave background structure. Including small but important corrections for unresolved-source residuals, we demonstrate agreement (measured by deviation of the ratio from unity) between 70 and 100 GHz power spectra averaged over 70 ≤ ℓ ≤ 390 at the 0.8% level, and agreement between 143 and 100 GHz power spectra of 0.4% over the same ℓ range. These values are within and consistent with the overall uncertainties in calibration given in the Planck 2013 results. We also present results based on the 2013 likelihood analysis showing consistency at the 0.35% between the 100, 143, and 217 GHz power spectra. We analyse calibration procedures and beams to determine what fraction of these differences can be accounted for by known approximations or systematic errors that could be controlled even better in the future, reducing uncertainties still further. Several possible small improvements are described. Subsequent analysis of the beams quantifies the importance of asymmetry in the near sidelobes, which was not fully accounted for initially, affecting the 70/100 ratio. Correcting for this, the 70, 100, and 143 GHz power spectra agree to 0.4% over the first two acoustic peaks. The likelihood analysis that produced the 2013 cosmological parameters incorporated uncertainties larger than this. We show explicitly that correction of the missing near sidelobe power in the HFI channels would result in shifts in the posterior distributions of parameters of less than 0.3σ except for As, the amplitude of the primordial curvature perturbations at 0.05 Mpc⁻¹, which changes by about 1σ. We extend these comparisons to include the sky maps from the complete nine-year mission of the Wilkinson Microwave Anisotropy Probe (WMAP), and find a roughly 2% difference between the Planck and WMAP power spectra in the region of the first acoustic peak.

Additional Information

The development of Planck has been supported by: ESA; CNES and CNRS/INSU-IN2P3-INP (France); ASI, CNR, and INAF (Italy); NASA and DoE (USA); STFC and UKSA (UK); CSIC, MICINN and JA (Spain); Tekes, AoF and CSC (Finland); DLR and MPG (Germany); CSA (Canada); DTU Space (Denmark); SER/SSO (Switzerland); RCN (Norway); SFI (Ireland); FCT/MCTES (Portugal); and DEISA (EU). A description of the Planck Collaboration and a list of its members, including the technical or scientific activities in which they have been involved, can be found at http://www.rssd.esa.int/Planck. Some of the results in this paper have been derived using the HEALPix package. We acknowledge the use of the Legacy Archive for Microwave Background Data Analysis (LAMBDA), part of the High Energy Astrophysics Science Archive Center (HEASARC); HEASARC/LAMBDA is a service of the Astrophysics Science Division at the NASA Goddard Space Flight Center.

Additional details

Created:
August 22, 2023
Modified:
October 24, 2023