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1999
DOI: 10.1016/s1387-6473(99)00009-3
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Introduction to microwave background polarization

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Cited by 49 publications
(44 citation statements)
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“…We then introduce the quantity C E;B = 0.5 · (C E + C B ), which will be used in the following best-fit analysis. On the contrary, the E and B modes of the primordial CMB anisotropies differ largely as they are induced by different mechanisms (e.g., Seljak & Zaldarriaga 1997;Kosowsky 1999). In the case of C TI , C synch e −(σ b ) 2 and c src e −(σ b ) 2 are also displayed.…”
Section: Selected Areas and Data Analysismentioning
confidence: 99%
“…We then introduce the quantity C E;B = 0.5 · (C E + C B ), which will be used in the following best-fit analysis. On the contrary, the E and B modes of the primordial CMB anisotropies differ largely as they are induced by different mechanisms (e.g., Seljak & Zaldarriaga 1997;Kosowsky 1999). In the case of C TI , C synch e −(σ b ) 2 and c src e −(σ b ) 2 are also displayed.…”
Section: Selected Areas and Data Analysismentioning
confidence: 99%
“…In addition, a linearly polarized component of the CMB arises from any quadrupolar variation in the photons scattered from electrons at the last scattering surface (Rees 1968;Hu & White 1997). Polarization data will complement other CMB data (e.g., Kosowsky 1999). Current cosmological models predict that polarization anisotropies are 10-20 times smaller than temperature anisotropies.…”
Section: Introductionmentioning
confidence: 99%
“…The CMB radiation can be polarized due to the gravitational waves called the B-mode of CMB [43][44][45]. The angular power spectrum of the B-mode of CMB is given by [46,47] …”
Section: Bb-mode Angular Power Spectrum Of Cmbmentioning
confidence: 99%