2020/04/30 by Thomas J. Clarke, Edmund J. Copeland, Adam Moss · 1 citation
Physics and Astronomy · #astro-ph.CO
paper · pdf · doi:10.1088/1475-7516/2020/10/002
32 pages, 9 figures, 1 appendix (with 1 figure). Prepared for submission to JCAP
arxiv created 2020/07/13 · arxiv updated 2020/10/14
Searches for primordial gravitational waves have resulted in constraints in a large frequency range from a variety of sources. The standard Cosmic Microwave Background (CMB) technique is to parameterise the tensor power spectrum in terms of the tensor-to-scalar ratio, r, and spectral index, n\rm t, and constrain these using measurements of the temperature and polarization power spectra. Another method, applicable to modes well inside the cosmological horizon at recombination, uses the shortwave approximation, under which gravitational waves behave as an effective neutrino species. In this paper we give model-independent CMB constraints on the energy density of gravitational waves, Ω_\textrmgw h2, for the entire range of observable frequencies. On large scales, f \lesssim 10-16 Hz, we reconstruct the initial tensor power spectrum in logarithmic frequency bins, finding maximal sensitivity for scales close to the horizon size at recombination. On small scales, f \gtrsim10-15 Hz, we use the shortwave approximation, finding Ω_\textrmgw h2 < 1.7 ×10-6 for adiabatic initial conditions and Ω_\textrmgw h2 < 2.9 ×10-7 for homogeneous initial conditions (both 2σ upper limits). For scales close to the horizon size at recombination, we use second-order perturbation theory to calculate the back-reaction from gravitational waves, finding Ω_\textrmgw h2 < 8.4 ×10-7, in the absence of neutrino anisotropic stress and Ω_\textrmgw h2 < 8.6 ×10-7 when including neutrino anisotropic stress. These constraints are valid for 10-15 Hz \gtrsim f \gtrsim 3 × 10-16 Hz.