Abstract

We use cosmic microwave background data from the WMAP, SPT, BICEP, and QUaD experiments to obtain constraints on the dark matter particle mass ${m}_{\ensuremath{\chi}}$, and show that the combined data requires ${m}_{\ensuremath{\chi}}>7.6\text{ }\text{ }\mathrm{GeV}$ at the 95% confidence level for the $\ensuremath{\chi}\ensuremath{\chi}\ensuremath{\rightarrow}b\overline{b}$ channel assuming $s$-wave annihilation and a thermal cross section $⟨{\ensuremath{\sigma}}_{\mathrm{a}}v⟩=3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}26}\text{ }\text{ }{\mathrm{cm}}^{3}/\mathrm{s}$. We examine whether the bound on ${m}_{\ensuremath{\chi}}$ is sensitive to ${\ensuremath{\sigma}}_{8}$ measurements made by galaxy cluster observations. The large uncertainty in ${\ensuremath{\sigma}}_{8}$ and the degeneracy with ${\ensuremath{\Omega}}_{\mathrm{m}}$ allow only small improvements in the dark matter mass bound. Increasing the number of effective neutrinolike degrees of freedom to ${N}_{\mathrm{eff}}=3.85$ improves the mass bound to ${m}_{\ensuremath{\chi}}>8.6\text{ }\text{ }\mathrm{GeV}$ at 95% confidence, for the $\ensuremath{\chi}\ensuremath{\chi}\ensuremath{\rightarrow}b\overline{b}$ channel. We also study models in which dark matter halos at $z<60$ reionize the Universe. We compute the Ostriker-Vishniac power resulting from partial reionization at intermediate redshifts $10<z<60$, but find the effect to be small. We discuss the importance of the large angle polarization as a complementary probe of dark matter annihilation. By performing Monte Carlo simulations, we show that future experiments that measure the $EE$ power spectrum from $20<l<50$ can exclude ${m}_{\ensuremath{\chi}}\ensuremath{\sim}10\text{ }\text{ }\mathrm{GeV}$ at the $2(3)\ensuremath{\sigma}$ level provided the error bars are smaller than $4(3)\ifmmode\times\else\texttimes\fi{}\mathrm{\text{cosmic variance}}$. We show that the Planck experiment will significantly improve our knowledge of dark matter properties.

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