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Erratum: "A Measurement of the Cosmic Microwave Background B-Mode Polarization Power Spectrum at Sub-degree Scales with POLARBEAR" (2014, ApJ, 794, 171)

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Published 2017 October 12 © 2017. The American Astronomical Society. All rights reserved.
, , Citation The Polarbear Collaboration: P. A. R. Ade et al 2017 ApJ 848 73 DOI 10.3847/1538-4357/aa8c70

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This is a correction for 2014 ApJ 794 171

0004-637X/848/1/73

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In preparing our second-season results, we found a simple mathematical error in our calculation of the upper bound for contamination by synchrotron radiation. In this erratum, we do not include any new foreground information, we simply fix the calculation error. This has the effect of changing the confidence of the rejection of no B-mode polarization power from gravitational lensing from 97.2% to 97.1%. Note that, to the precision reported in number of σ, this does not affect the significance of the Polarbear B-mode measurement.

There are four places where this affects the text of the paper.

  • 1.  
    The sentence in the abstract "Including both systematic and statistical uncertainties, the hypothesis of no B-mode polarization power from gravitational lensing is rejected at 97.2% confidence." should read as follows. "Including both systematic and statistical uncertainties, the hypothesis of no B-mode polarization power from gravitational lensing is rejected at 97.1% confidence."
  • 2.  
    In Table 4, the upper bound for contamination by synchrotron radiation should be changed; the corrected values are shown in Table 4 here.
  • 3.  
    The second to last sentence of Section 8 should be changed from "The measurement rejects the hypothesis of no ${C}_{{\ell }}^{{BB}}$ from lensing with a confidence of 97.2%" to read as follows. "The measurement rejects the hypothesis of no ${C}_{{\ell }}^{{BB}}$ from lensing with a confidence of 97.1%."
  • 4.  
    In the summary of the reported Polarbear systematic uncertainties, presented in Table 9, the row for synchrotron should be changed, as shown in the corrected Table 9 here. Note that the total is unchanged, to the precision shown here.

Table 4.  Sources of Foreground Power and Their Predicted Power in ${\ell }({\ell }+1){C}_{{\ell }}^{{BB}}/2\pi $

Foreground Predicted power in ${\ell }({\ell }+1){C}_{{\ell }}^{{BB}}/2\pi $
  (${10}^{-4}$ $\mu {{\rm{K}}}^{2}$)
  500–900 900–1300 1300–1700 1700–2100
Galactic dust 40 28 22 9.7
Galactic synchrotron 2.3 1.8 1.6 1.4
Radio galaxies 6.3 15 28 46
Dusty galaxies 2.8 4.5 6.5 8.7
Total bias 51 49 58 66

Note. All foreground power is small compared to our statistical uncertainties, and we do not subtract it. The total bias on the final line is the linear sum of the individual foreground powers.

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Table 9.  Summary of Possible Contributions to the Amplitude of ABB from Major Sources of Systematic Uncertainty

Type Source of systematics Effect on ABB
Systematic uncertainty: Galactic dust 0.045
astrophysical foreground Galactic synchrotron 0.003
  Radio galaxies 0.011
  Dusty galaxies 0.004
Systematic uncertainty: Differential & Boresight pointing 0.017
instrument Instrument & relative polarization angle 0.014
  Pixel-pair relative gain: HWP-independent 0.002
  Pixel-pair relative gain: HWP-dependent 0.010
  Pixel-pair relative gain: drift 0.001
  Differential beam ellipticity 0.001
  Differential beam size 0.003
  Electrical crosstalk 0.002
Systematic uncertainty: Scan synchronous template 0.002
analysis E-to-B leakage subtraction 0.006 ± 0.037
  Total 0.121 ± 0.037
Multiplicative effect Statistical variance and beam co-variance ±0.041
  Polarization efficiency ±0.036
  Transfer function ±0.039
  Total ±0.06

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10.3847/1538-4357/aa8c70