Abstract

In the presence of a background magnetic field, axion dark matter induces an electric field and can thus excite phonon-polaritons in suitable materials. We revisit the calculation of the axion-photon conversion power output from such materials, accounting for finite volume effects, and material losses. Our calculation shows how phonon-polaritons can be converted to propagating photons at the material boundary, offering a route to detecting the signal. Using the dielectric functions of GaAs, ${\text{Al}}_{2}{\mathrm{O}}_{3}$, and ${\mathrm{SiO}}_{2}$, a fit to our loss model leads to a signal of lower magnitude than previous calculations. We demonstrate how knowledge of resonances in the dielectric function can directly be used to calculate the sensitivity of any material to axion dark matter. We argue that a combination of low losses encountered at $\mathcal{O}(1)\text{ }\text{ }\mathrm{K}$ temperatures and near future improvements in detector dark count allow one to probe the QCD axion in the mass range ${m}_{a}\ensuremath{\approx}100\text{ }\text{ }\mathrm{meV}$. This provides further impetus to examine novel materials and further develop detectors in the THz regime. We also discuss possible tuning methods to scan the axion mass.

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