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 provide complementary figures to those of the 2017 HFI DPC paper ({{PlanckPapers|planck2016-l03}}).
  
<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>
 
  
Those masks are provided in the PLA.
+
 
+
<!--
{| 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:center" width=800px
 
|+ '''CO and dust templates '''
 
|+ '''CO and dust templates '''
 
|- bgcolor="ffdead"
 
|- bgcolor="ffdead"
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|}
 
|}
  
 +
-->
  
<span style="font-size:150%">'''[Complementary of Fig. 11:]''' </span>
 
  
{| border="1" cellpadding="3" cellspacing="0" align="center" style="text-align:left" width=800px
 
|+ '''Comparaison of 2015 and 2017 I, Q and U maps and their difference. '''
 
|- bgcolor="ffdead"
 
!
 
!colspan="3"| 2015 maps
 
!colspan="3"| 2017 maps
 
!colspan="3"| difference
 
|-
 
!
 
!I
 
!Q
 
!U
 
!I
 
!Q
 
!U
 
!I
 
!Q
 
!U
 
|-
 
| 100 GHz
 
|[[File:100GHz_DX11_I.pdf.pdf]]
 
|[[File:100GHz_DX11_Q.pdf.pdf]]
 
|[[File:100GHz_DX11_U.pdf.pdf]]
 
|[[File:100GHz_I.pdf]]
 
|[[File:100GHz_Q.pdf]]
 
|[[File:100GHz_U.pdf]]
 
|[[File:100GHz_diff_I.pdf.pdf]]
 
|[[File:100GHz_diff_Q.pdf.pdf]]
 
|[[File:100GHz_diff_U.pdf.pdf]]
 
|-
 
| 143 GHz
 
|[[File:143GHz_DX11_I.pdf.pdf]]
 
|[[File:143GHz_DX11_Q.pdf.pdf]]
 
|[[File:143GHz_DX11_U.pdf.pdf]]
 
|[[File:143GHz_I.pdf]]
 
|[[File:143GHz_Q.pdf]]
 
|[[File:143GHz_U.pdf]]
 
|[[File:143GHz_diff_I.pdf.pdf]]
 
|[[File:143GHz_diff_Q.pdf.pdf]]
 
|[[File:143GHz_diff_U.pdf.pdf]]
 
|-
 
| 217 GHz
 
|[[File:217GHz_DX11_I.pdf.pdf]]
 
|[[File:217GHz_DX11_Q.pdf.pdf]]
 
|[[File:217GHz_DX11_U.pdf.pdf]]
 
|[[File:217GHz_I.pdf]]
 
|[[File:217GHz_Q.pdf]]
 
|[[File:217GHz_U.pdf]]
 
|[[File:217GHz_diff_I.pdf.pdf]]
 
|[[File:217GHz_diff_Q.pdf.pdf]]
 
|[[File:217GHz_diff_U.pdf.pdf]]
 
|-
 
| 353 GHz
 
|[[File:353GHz_DX11_I.pdf.pdf]]
 
|[[File:353GHz_DX11_Q.pdf.pdf]]
 
|[[File:353GHz_DX11_U.pdf.pdf]]
 
|[[File:353GHz_I.pdf]]
 
|[[File:353GHz_Q.pdf]]
 
|[[File:353GHz_U.pdf]]
 
|[[File:353GHz_diff_I.pdf.pdf]]
 
|[[File:353GHz_diff_Q.pdf.pdf]]
 
|[[File:353GHz_diff_U.pdf.pdf]]
 
|-
 
| 545 GHz
 
|[[File:545GHz_DX11_I.pdf.pdf]]
 
| .
 
| .
 
|[[File:545GHz_I.pdf]]
 
| .
 
| .
 
|[[File:545GHz_diff_I.pdf.pdf]]
 
| .
 
| .
 
|-
 
| 857 GHz
 
|[[File:857GHz_DX11_I.pdf.pdf]]
 
| .
 
| .
 
|[[File:857GHz_I.pdf]]
 
| .
 
| .
 
|[[File:857GHz_diff_I.pdf.pdf]]
 
| .
 
| .
 
|}
 
  
 +
<br>
 +
----
 +
<span style="font-size:150%">'''Section 5.3.10: for convenience, we reproduce here Figures 6, 7 and 8 of Rosset et al.''' </span>
  
<span style="font-size:150%">'''[Section 5.3.10. For convenience, we reproduce here Figures 6, 7 and 8 of Rosset et al.]''' </span>
+
This paper is published as Rosset et al. Planck pre-launch status: High Frequency Instrument polarization calibration. 2010b, A&A, 520, A13 {{PlanckPapers|rosset2010}}. The figures 6, 7 et 8 reproduced hereunder are given in the version on ArXiv 1004.2595
  
 
+
{| border="1" cellpadding="3" cellspacing="0" align="center" style="text-align:centert" width=800px
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
 
 
 
 
 
{| border="1" cellpadding="3" cellspacing="0" align="center" style="text-align:left" width=800px
 
 
|- bgcolor="ffdead"   
 
|- bgcolor="ffdead"   
 
! gain errors (1)|| polarization efficiency errors (2)|| orientation errors (3)
 
! gain errors (1)|| polarization efficiency errors (2)|| orientation errors (3)
Line 133: Line 45:
 
|}
 
|}
  
(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.
+
(1) <math>\Delta C_{\ell}</math> 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.
+
(2) <math>\Delta C_{\ell}</math> in rms due to polarization efficiency 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.
+
(3) <math>\Delta C_{\ell}</math> 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.
  
  
<span style="font-size:150%">'''[Complementary of Fig. 29:]''' </span>
+
<br>
 +
----
 +
<span style="font-size:150%">'''Section 5.5: complementary figures of Fig. 29''' </span>
  
{| 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:center" width=800px
 
|+ '''Map and power spectra from E2E simulations difference with and without 4K lines. '''
 
|+ '''Map and power spectra from E2E simulations difference with and without 4K lines. '''
 
|- bgcolor="ffdead"   
 
|- bgcolor="ffdead"   
Line 150: Line 64:
 
!colspan="2"| 353 GHz bolometers  
 
!colspan="2"| 353 GHz bolometers  
 
|-
 
|-
|[[File:map_100-1a_lines4K.pdf]]
+
|[[File:map_100-1a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-1a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-1a_sroll.pdf|100px]]
|[[File:map_143-1a_lines4K.pdf]]
+
|[[File:map_143-1a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-1a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-1a_sroll.pdf|100px]]
|[[File:map_217-1_lines4K.pdf]]
+
|[[File:map_217-1_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-1_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-1_sroll.pdf|100px]]
|[[File:map_353-1_lines4K.pdf]]
+
|[[File:map_353-1_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-1_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-1_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-1b_lines4K.pdf]]
+
|[[File:map_100-1b_lines4K.pd|100px]]
|[[File:cl_fsky43_lines4K_100-1b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-1b_sroll.pdf|100px]]
|[[File:map_143-1b_lines4K.pdf]]
+
|[[File:map_143-1b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-1b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-1b_sroll.pdf|100px]]
|[[File:map_217-2_lines4K.pdf]]
+
|[[File:map_217-2_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-2_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-2_sroll.pdf|100px]]
|[[File:map_353-2_lines4K.pdf]]
+
|[[File:map_353-2_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-2_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-2_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-2a_lines4K.pdf]]
+
|[[File:map_100-2a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-2a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-2a_sroll.pdf|100px]]
|[[File:map_143-2a_lines4K.pdf]]
+
|[[File:map_143-2a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-2a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-2a_sroll.pdf|100px]]
|[[File:map_217-3_lines4K.pdf]]
+
|[[File:map_217-3_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-3_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-3_sroll.pdf|100px]]
|[[File:map_353-3a_lines4K.pdf]]
+
|[[File:map_353-3a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-3a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-3a_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-2b_lines4K.pdf]]
+
|[[File:map_100-2b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-2b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-2b_sroll.pdf|100px]]
|[[File:map_143-2b_lines4K.pdf]]
+
|[[File:map_143-2b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-2b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-2b_sroll.pdf|100px]]
|[[File:map_217-4_lines4K.pdf]]
+
|[[File:map_217-4_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-4_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-4_sroll.pdf|100px]]
|[[File:map_353-3b_lines4K.pdf]]
+
|[[File:map_353-3b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-3b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-3b_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-3a_lines4K.pdf]]
+
|[[File:map_100-3a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-3a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-3a_sroll.pdf|100px]]
|[[File:map_143-3a_lines4K.pdf]]
+
|[[File:map_143-3a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-3a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-3a_sroll.pdf|100px]]
|[[File:map_217-5-a_lines4K.pdf]]
+
|[[File:map_217-5-a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-5a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-5a_sroll.pdf|100px]]
|[[File:map_353-4a_lines4K.pdf]]
+
|[[File:map_353-4a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-4a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-4a_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-3b_lines4K.pdf]]
+
|[[File:map_100-3b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-3b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-3b_sroll.pdf|100px]]
|[[File:map_143-3b_lines4K.pdf]]
+
|[[File:map_143-3b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-3b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-3b_sroll.pdf|100px]]
|[[File:map_217-5b_lines4K.pdf]]
+
|[[File:map_217-5b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-5b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-5b_sroll.pdf|100px]]
|[[File:map_353-4b_lines4K.pdf]]
+
|[[File:map_353-4b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-4b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-4b_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-4a_lines4K.pdf]]
+
|[[File:map_100-4a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-4a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-4a_sroll.pdf|100px]]
|[[File:map_143-4a_lines4K.pdf]]
+
|[[File:map_143-4a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-4a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-4a_sroll.pdf|100px]]
|[[File:map_217-6a_lines4K.pdf]]
+
|[[File:map_217-6a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-6a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-6a_sroll.pdf|100px]]
|[[File:map_353-5a_lines4K.pdf]]
+
|[[File:map_353-5a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-5a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-5a_sroll.pdf|100px]]
 
|-
 
|-
|[[File:map_100-4b_lines4K.pdf]]
+
|[[File:map_100-4b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_100-4b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_100-4b_sroll.pdf|100px]]
|[[File:map_143-4b_lines4K.pdf]]
+
|[[File:map_143-4b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-4b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-4b_sroll.pdf|100px]]
|[[File:map_217-6b_lines4K.pdf]]
+
|[[File:map_217-6b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-6b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-6b_sroll.pdf|100px]]
|[[File:map_353-5b_lines4K.pdf]]
+
|[[File:map_353-5b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-5b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-5b_sroll.pdf|100px]]
 
|-
 
|-
 
| .
 
| .
 
| .
 
| .
|[[File:map_143-5_lines4K.pdf]]
+
|[[File:map_143-5_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-5_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-5_sroll.pdf|100px]]
|[[File:map_217-7a_lines4K.pdf]]
+
|[[File:map_217-7a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-7a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-7a_sroll.pdf|100px]]
|[[File:map_353-6a_lines4K.pdf]]
+
|[[File:map_353-6a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-6a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-6a_sroll.pdf|100px]]
 
|-
 
|-
 
| .
 
| .
 
| .
 
| .
|[[File:map_143-6_lines4K.pdf]]
+
|[[File:map_143-6_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-6_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-6_sroll.pdf|100px]]
|[[File:map_217-7b_lines4K.pdf]]
+
|[[File:map_217-7b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-7b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-7b_sroll.pdf|100px]]
|[[File:map_353-6b_lines4K.pdf]]
+
|[[File:map_353-6b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-6b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-6b_sroll.pdf|100px]]
 
|-
 
|-
 
| .
 
| .
 
| .
 
| .
|[[File:map_143-7_lines4K.pdf]]
+
|[[File:map_143-7_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_143-7_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_143-7_sroll.pdf|100px]]
|[[File:map_217-8a_lines4K.pdf]]
+
|[[File:map_217-8a_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-8a_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-8a_sroll.pdf|100px]]
|[[File:map_353-7_lines4K.pdf]]
+
|[[File:map_353-7_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-7_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-7_sroll.pdf|100px]]
 
|-
 
|-
 
| .
 
| .
Line 253: Line 167:
 
| .
 
| .
 
| .  
 
| .  
|[[File:map_217-8b_lines4K.pdf]]
+
|[[File:map_217-8b_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_217-8b_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_217-8b_sroll.pdf|100px]]
|[[File:map_353-8_lines4K.pdf]]
+
|[[File:map_353-8_lines4K.pdf|100px]]
|[[File:cl_fsky43_lines4K_353-8_sroll.pdf]]
+
|[[File:cl_fsky43_lines4K_353-8_sroll.pdf|100px]]
  
 
|}
 
|}
  
  
<span style="font-size:150%">'''[Complementary of Fig. 47:]''' </span>
+
<br>
 +
----
 +
<span style="font-size:150%">'''Section 5.13: complementary figures of Fig. 47''' </span>
  
{| 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:center" width=800px
 
|+ '''ADCNL induced gain time variation as a function of ring numbers. Blue line shows the solved gain variation for the data and grey ones show 10 realizations drawn within the uncertainties of the ADC model. '''
 
|+ '''ADCNL induced gain time variation as a function of ring numbers. Blue line shows the solved gain variation for the data and grey ones show 10 realizations drawn within the uncertainties of the ADC model. '''
 
|- bgcolor="ffdead"   
 
|- bgcolor="ffdead"   
Line 274: Line 190:
 
|}
 
|}
  
 +
<br>
 
== References ==
 
== References ==
 
<References />
 
<References />
 
   
 
   
 
 
[[Category:HFI data processing|004]]
 
[[Category:HFI data processing|004]]

Latest revision as of 11:31, 28 November 2017

This page is intented to provide complementary figures to those of the 2017 HFI DPC paper (Planck-2020-A3[1]).






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 Planck-PreLaunch-XIII[2]. 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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Error creating thumbnail: convert: unable to extend cache `/tmp/magick-30441hF9Axg5ibRSB': File too large @ error/cache.c/OpenPixelCache/4091.
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(1) [math]\Delta C_{\ell}[/math] 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) [math]\Delta C_{\ell}[/math] in rms due to polarization efficiency 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) [math]\Delta C_{\ell}[/math] 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.




Section 5.5: complementary figures of Fig. 29

Map and power spectra from E2E simulations difference with and without 4K lines.
100 GHz bolometers 143 GHz bolometers 217 GHz bolometers 353 GHz bolometers
Map 100-1a lines4K.pdf Cl fsky43 lines4K 100-1a sroll.pdf Map 143-1a lines4K.pdf Cl fsky43 lines4K 143-1a sroll.pdf Map 217-1 lines4K.pdf Cl fsky43 lines4K 217-1 sroll.pdf Map 353-1 lines4K.pdf Cl fsky43 lines4K 353-1 sroll.pdf
100px Cl fsky43 lines4K 100-1b sroll.pdf Map 143-1b lines4K.pdf Cl fsky43 lines4K 143-1b sroll.pdf Map 217-2 lines4K.pdf Cl fsky43 lines4K 217-2 sroll.pdf Map 353-2 lines4K.pdf Cl fsky43 lines4K 353-2 sroll.pdf
Map 100-2a lines4K.pdf Cl fsky43 lines4K 100-2a sroll.pdf Map 143-2a lines4K.pdf Cl fsky43 lines4K 143-2a sroll.pdf Map 217-3 lines4K.pdf Cl fsky43 lines4K 217-3 sroll.pdf Map 353-3a lines4K.pdf Cl fsky43 lines4K 353-3a sroll.pdf
Map 100-2b lines4K.pdf Cl fsky43 lines4K 100-2b sroll.pdf Map 143-2b lines4K.pdf Cl fsky43 lines4K 143-2b sroll.pdf Map 217-4 lines4K.pdf Cl fsky43 lines4K 217-4 sroll.pdf Map 353-3b lines4K.pdf Cl fsky43 lines4K 353-3b sroll.pdf
Map 100-3a lines4K.pdf Cl fsky43 lines4K 100-3a sroll.pdf Map 143-3a lines4K.pdf Cl fsky43 lines4K 143-3a sroll.pdf Map 217-5-a lines4K.pdf Cl fsky43 lines4K 217-5a sroll.pdf Map 353-4a lines4K.pdf Cl fsky43 lines4K 353-4a sroll.pdf
Map 100-3b lines4K.pdf Cl fsky43 lines4K 100-3b sroll.pdf Map 143-3b lines4K.pdf Cl fsky43 lines4K 143-3b sroll.pdf Map 217-5b lines4K.pdf Cl fsky43 lines4K 217-5b sroll.pdf Map 353-4b lines4K.pdf Cl fsky43 lines4K 353-4b sroll.pdf
Map 100-4a lines4K.pdf Cl fsky43 lines4K 100-4a sroll.pdf Map 143-4a lines4K.pdf Cl fsky43 lines4K 143-4a sroll.pdf Map 217-6a lines4K.pdf Cl fsky43 lines4K 217-6a sroll.pdf Map 353-5a lines4K.pdf Cl fsky43 lines4K 353-5a sroll.pdf
Map 100-4b lines4K.pdf Cl fsky43 lines4K 100-4b sroll.pdf Map 143-4b lines4K.pdf Cl fsky43 lines4K 143-4b sroll.pdf Map 217-6b lines4K.pdf Cl fsky43 lines4K 217-6b sroll.pdf Map 353-5b lines4K.pdf Cl fsky43 lines4K 353-5b sroll.pdf
. . Map 143-5 lines4K.pdf Cl fsky43 lines4K 143-5 sroll.pdf Map 217-7a lines4K.pdf Cl fsky43 lines4K 217-7a sroll.pdf Map 353-6a lines4K.pdf Cl fsky43 lines4K 353-6a sroll.pdf
. . Map 143-6 lines4K.pdf Cl fsky43 lines4K 143-6 sroll.pdf Map 217-7b lines4K.pdf Cl fsky43 lines4K 217-7b sroll.pdf Map 353-6b lines4K.pdf Cl fsky43 lines4K 353-6b sroll.pdf
. . Map 143-7 lines4K.pdf Cl fsky43 lines4K 143-7 sroll.pdf Map 217-8a lines4K.pdf Cl fsky43 lines4K 217-8a sroll.pdf Map 353-7 lines4K.pdf Cl fsky43 lines4K 353-7 sroll.pdf
. . . . Map 217-8b lines4K.pdf Cl fsky43 lines4K 217-8b sroll.pdf Map 353-8 lines4K.pdf Cl fsky43 lines4K 353-8 sroll.pdf




Section 5.13: complementary figures of Fig. 47

ADCNL induced gain time variation as a function of ring numbers. Blue line shows the solved gain variation for the data and grey ones show 10 realizations drawn within the uncertainties of the ADC model.
100 GHz bolometers 143 GHz bolometers 217 GHz bolometers 353 GHz bolometers
DEC16v1 gains 100ghz JG INL.pdf DEC16v1 gains 143ghz JG INL.pdf DEC16v1 gains 217ghz JG INL.pdf DEC16v1 gains 353ghz JG INL.pdf


References[edit]

  1. Planck 2018 results. III. High Frequency Instrument data processing and frequency maps, Planck Collaboration, 2020, A&A, 641, A3.
  2. Planck pre-launch status: High Frequency Instrument polarization calibration, C. Rosset, M. Tristram, N. Ponthieu, et al. , A&A, 520, A13+, (2010).

(Planck) High Frequency Instrument

Data Processing Center

EMI/EMC influence of the 4K cooler mechanical motion on the bolometer readout electronics.

analog to digital converter