Detecting Primordial Gravitational Waves Signal from BICEP2 and {\it Planck} HFI 353353GHz Dust Polarization

preprint2014arXivOpen access

Abstract

The dust polarization is parameterized as a power law form of the multipole ll: DlXX=AXXl(l+1)lαXX/(2π)D^{XX}_{l}=A^{XX}l(l+1)l^{α_{XX}}/(2π) (XXXX denotes BBBB or EEEE), where AXXA^{XX} is its amplitude with the ratio ABB/AEE=0.52±0.02A^{BB}/A^{EE}=0.52\pm 0.02 and αBB,EE=−2.42±0.02α_{BB,EE}=-2.42\pm 0.02. Extrapolating to 150150GHz from 353353GHz yields a value of Dl=80BB=(1.32±0.29)×10−2μK2D^{BB}_{l=80}=(1.32\pm 0.29)\times 10^{-2}μK^2 (and an additional uncertainty (+0.28,−0.24)×10−2μK2(+0.28,-0.24)\times 10^{-2}μK^2) over the range 40<l<12040<l<120. Based on these data, we report the tensor-to-scalar ratio r=At/Asr=A_{t}/A_{s} defined at k0=0.05Mpc−1k_0=0.05 \text{Mpc} ^{-1} by joining the BICEP2+{\it Planck}2013+WMAP9+BAO+HST and {\it Planck} HFI 353353GHz dust polarization and its implication to the detection of the primordial gravitational waves. Considering the ΛΛCDM+rr model, we found r<0.108r<0.108 at 95%95\% confidence level with σstat=0.29σ_{stat}=0.29 and r<0.129r<0.129 at 95%95\% confidence level with σstat+extr=0.29+0.28σ_{stat+extr}=0.29+0.28. The results imply no significant evidence for the primordial gravitational waves in 1σ1σ regions. However the post probability distribution of rr peaks at a small positive value. And rr moves to larger positive values when the extrapolation error bars are included. This might imply a very weak signal of the primordial gravitational waves. It also implies the crucial fact in calibrating the amplitude of the dust polarizations in detecting the primordial gravitational waves in the future. When the running of the scalar spectral tilt is included, we found r<0.079r<0.079 at 95%95\% confidence level with σstat=0.29σ_{stat}=0.29 and r=0.091−0.069+0.042r=0.091_{-0.069}^{+0.042} at 95%95\% confidence level with σstat+extr=0.29+0.28σ_{stat+extr}=0.29+0.28. The later one implies the detection of the primordial gravitational waves in 1σ1σ regions at the cost of decreasing the value of Dl=80BBD^{BB}_{l=80} to 0.67−0.25+0.250.67_{-0.25}^{+0.25}.

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