Difference between revisions of "Appendix of HFI DPC paper"
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This page is intented to gather figures that are not inserted in the 2017 DPC paper ({{PlanckPapers|planck2016-l03}}) for readability reasons. | This page is intented to gather figures that are not inserted in the 2017 DPC paper ({{PlanckPapers|planck2016-l03}}) for readability reasons. | ||
− | <span style="font-size:150%">'''[Section 3.1.2. | + | <span style="font-size:150%">'''[Section 3.1.2. Mask of the very bright regions where the sub-pixel effect in the foreground templates creates problems and prevent them to be used for cosmology or astrophysics analysis]''' </span> |
− | Mask of the very bright regions where the sub-pixel effect in the foreground templates creates problems and prevent them to be used for cosmology or astrophysics analysis | + | |
{| border="1" cellpadding="3" cellspacing="0" align="center" style="text-align:left" width=800px | {| border="1" cellpadding="3" cellspacing="0" align="center" style="text-align:left" width=800px | ||
|+ '''CO and dust templates ''' | |+ '''CO and dust templates ''' |
Revision as of 09:41, 5 October 2017
This page is intented to gather figures that are not inserted in the 2017 DPC paper (Planck-2020-A3[1]) for readability reasons.
[Section 3.1.2. Mask of the very bright regions where the sub-pixel effect in the foreground templates creates problems and prevent them to be used for cosmology or astrophysics analysis]
100 GHz | 143 GHz | 217 GHz | 353 GHz | |
---|---|---|---|---|
CO template | . | |||
Dust template |
[Complementary of Fig. 11:]
2015 maps | 2017 maps | difference | |||||||
---|---|---|---|---|---|---|---|---|---|
I | Q | U | I | Q | U | I | Q | U | |
100 GHz | |||||||||
143 GHz | |||||||||
217 GHz | |||||||||
353 GHz | |||||||||
545 GHz | . | . | . | . | . | . | |||
857 GHz | . | . | . | . | . | . |
[Section 5.3.10. For convenience, we reproduce here Figures 6, 7 and 8 of Rosset et al.]
This paper is published as Rosset et al. Planck pre-launch status: High Frequency Instrument polarization calibration. 2010b, A&A, 520, A13.
The figures 6, 7 et 8 reproduced hereunder are given in the version on ArXiv 1004.2595
gain errors (1) | polarization efficiency errors (2) | orientation errors (3) |
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(1) Delta Cl in rms due to gain errors from 0.01% to 1% for E-mode (top) and B-mode (bottom) compared to initial spectrum (solid black lines). Cosmic variance for E-mode is plotted in dashed black line.
(2) Delta Cl in rms due to polarization effi?ciency errors from 0.1% to 4% for E-mode (top) and B-mode (bottom) compared to initial spectrum (solid black lines). Cosmic variance for E-mode is plotted in dashed black line.
(3) Delta Cl in rms due to various orientation errors from 0.25 to 2 degrees for E-mode (top) and B-mode (bottom) compared to initial spectrum (solid black lines). Cosmic variance for E-mode is plotted in dashed black line.
[Complementary of Fig. 29:]
100 GHz bolometers | 143 GHz bolometers | 217 GHz bolometers | 353 GHz bolometers | ||||
---|---|---|---|---|---|---|---|
. | . | ||||||
. | . | ||||||
. | . | ||||||
. | . | . | . |
[Complementary of Fig. 47:]
- ↑ Planck 2018 results. III. High Frequency Instrument data processing and frequency maps, Planck Collaboration, 2020, A&A, 641, A3.
Data Processing Center
EMI/EMC influence of the 4K cooler mechanical motion on the bolometer readout electronics.
analog to digital converter