Bibcode
Planck Collaboration; Ade, P. A. R.; Arnaud, M.; Ashdown, M.; Aumont, J.; Baccigalupi, C.; Banday, A. J.; Barreiro, R. B.; Battaner, E.; Benabed, K.; Benoit-Lévy, A.; Bernard, J.-P.; Bersanelli, M.; Bielewicz, P.; Bond, J. R.; Borrill, J.; Bouchet, F. R.; Burigana, C.; Cardoso, J.-F.; Catalano, A.; Challinor, A.; Chamballu, A.; Chiang, H. C.; Christensen, P. R.; Clements, D. L.; Colombi, S.; Colombo, L. P. L.; Couchot, F.; Coulais, A.; Crill, B. P.; Curto, A.; Cuttaia, F.; Danese, L.; Davies, R. D.; Davis, R. J.; de Bernardis, P.; de Rosa, A.; de Zotti, G.; Delabrouille, J.; Désert, F.-X.; Dickinson, C.; Diego, J. M.; Dole, H.; Donzelli, S.; Doré, O.; Douspis, M.; Dupac, X.; Enßlin, T. A.; Eriksen, H. K.; Finelli, F.; Forni, O.; Frailis, M.; Fraisse, A. A.; Franceschi, E.; Galeotta, S.; Ganga, K.; Giard, M.; González-Nuevo, J.; Górski, K. M.; Gratton, S.; Gregorio, A.; Gruppuso, A.; Gudmundsson, J. E.; Hansen, F. K.; Hanson, D.; Harrison, D. L.; Henrot-Versillé, S.; Herranz, D.; Hildebrandt, S. R.; Hivon, E.; Hobson, M.; Holmes, W. A.; Hornstrup, A.; Hovest, W.; Huffenberger, K. M.; Jaffe, A. H.; Jaffe, T. R.; Jones, W. C.; Keihänen, E.; Keskitalo, R.; Knoche, J.; Kunz, M.; Kurki-Suonio, H.; Lagache, G.; Lähteenmäki, A.; Lamarre, J.-M.; Lasenby, A.; Lawrence, C. R.; Leonardi, R.; León-Tavares, J.; Lesgourgues, J.; Liguori, M.; Lilje, P. B.; Linden-Vørnle, M.; López-Caniego, M.; Lubin, P. M.; Macías-Pérez, J. F.; Maino, D.; Mandolesi, N.; Maris, M. et al.
Bibliographical reference
Astronomy and Astrophysics, Volume 571, id.A31, 25 pp.
Advertised on:
11
2014
Journal
Citations
73
Refereed citations
68
Description
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 systematicerrors 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.