SU(2)CMB at high redshifts and the value of H0
Abstract
We investigate a high-z cosmological model to compute the co-moving sound horizon rs at baryon-velocity freeze-out towards the end of hydrogen recombination. This model assumes a replacement of the conventional CMB photon gas by deconfining SU(2) Yang-Mills thermodynamics, three flavours of massless neutrinos (N=3), and a purely baryonic matter sector (no cold dark-matter (CDM)). The according SU(2) temperature-redshift relation of the CMB is contrasted with recent measurements appealing to the thermal Sunyaev-Zel'dovich effect and CMB-photon absorption by molecular rotations bands or atomic hyperfine levels. Relying on a realistic simulation of the ionization history throughout recombination, we obtain z*=1693.55 6.98 and z drag=1812.66 7.01. Due to considerable widths of the visibility functions in the solutions to the associated Boltzmann hierarchy and Euler equation we conclude that z* and z drag over-estimate the redshifts for the respective photon and baryon-velocity freeze-out. Realistic decoupling values turn out to be z lf,*=1554.89 5.18 and z lf,drag=1659.30 5.48. With rs(z lf,drag)=(137.19 0.45)\,Mpc and the essentially model independent extraction of rs· H0=const from low-z data in arXiv:1607.05617 we obtain a good match with the value H0=(73.24 1.74)\,km\,s-1\,Mpc-1 extracted in arXiv:1604.01424 by appealing to Cepheid calibrated SNe~Ia, new parallax measurements, stronger constraints on the Hubble flow, and a refined computation of distance to NGC4258 from maser data. We briefly comment on a possible interpolation of our high-z model, invoking percolated and unpercolated U(1) topological solitons of a Planck-scale axion field, to the phenomenologically successful low-z cosmology.
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