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Lensing of 21-cm Fluctuations by Primordial Gravitational Waves

Laura Book, Marc Kamionkowski, Fabian Schmidt

TL;DR

Weak-gravitational-lensing distortions to the intensity pattern of 21-cm radiation from the dark ages can be decomposed geometrically into curl and curl-free components, allowing tensor-to-scalar ratios conceivably as small as r~10(-9)-far smaller than those currently accessible-to be probed.

Abstract

Weak-gravitational-lensing distortions to the intensity pattern of 21-cm radiation from the dark ages can be decomposed geometrically into curl and curl-free components. Lensing by primordial gravitational waves induces a curl component, while the contribution from lensing by density fluctuations is strongly suppressed. Angular fluctuations in the 21-cm background extend to very small angular scales, and measurements at different frequencies probe different shells in redshift space. There is thus a huge trove of information with which to reconstruct the curl component of the lensing field, allowing tensor-to-scalar ratios conceivably as small as r ~ 10^{-9} - far smaller than those currently accessible - to be probed.

Lensing of 21-cm Fluctuations by Primordial Gravitational Waves

TL;DR

Weak-gravitational-lensing distortions to the intensity pattern of 21-cm radiation from the dark ages can be decomposed geometrically into curl and curl-free components, allowing tensor-to-scalar ratios conceivably as small as r~10(-9)-far smaller than those currently accessible-to be probed.

Abstract

Weak-gravitational-lensing distortions to the intensity pattern of 21-cm radiation from the dark ages can be decomposed geometrically into curl and curl-free components. Lensing by primordial gravitational waves induces a curl component, while the contribution from lensing by density fluctuations is strongly suppressed. Angular fluctuations in the 21-cm background extend to very small angular scales, and measurements at different frequencies probe different shells in redshift space. There is thus a huge trove of information with which to reconstruct the curl component of the lensing field, allowing tensor-to-scalar ratios conceivably as small as r ~ 10^{-9} - far smaller than those currently accessible - to be probed.

Paper Structure

This paper contains 12 equations, 1 figure.

Figures (1)

  • Figure 1: The power spectrum for the deflection-field curl component for lensing of sources at various redshifts by a scale-invariant spectrum of IGWs of the largest amplitude ($r=0.2$) consistent with current measurements. We also superimpose noise power spectra for lensing reconstruction carried out to various values of $l_{\rm max}$. Also shown is the noise power spectrum we estimate from co-adding the signals from all possible redshifts, assuming an $l_{\rm max} = 10^6$.