Abstract

We constrain deviations of the form T∝(1+z)1+εT\propto (1+z)^{1+ε} from the standard redshift-temperature relation, corresponding to modifying distance duality as DL=(1+z)2(1+ε)DAD_L=(1+z)^{2(1+ε)} D_A. We consider a consistent model, in which both the background and perturbation equations are changed. For this purpose, we introduce a species of dark radiation particles to which photon energy density is transferred, and assume ε≥0ε\ge0. The Planck 2015 release high multipole temperature plus low multipole data give the limit ε<4.5×10−3ε<4.5\times 10^{-3} at 95% C.L. The main obstacle to improving this CMB-only result is strong degeneracy between εε and the physical matter densities ωbω_{\rm b} and ωcω_{\rm c}. A constraint on deuterium abundance improves the limit to ε<1.8×10−3ε<1.8\times 10^{-3}. Adding the Planck high-multipole CMB polarisation and BAO data leads to a small improvement; with this maximal dataset we obtain ε<1.3×10−3ε<1.3\times 10^{-3}. This dataset constrains the present dark radiation energy density to at most 12% of the total photon plus dark radiation density. Finally, we discuss the degeneracy between dark radiation and the effective number of relativistic species NeffN_{\rm eff}, and consider the impact of dark radiation perturbations and allowing ε<0ε<0 on the results.

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