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[^1]: The notions *polyhedral domain* and *convex domain* are synonymous, i.e., for every convex domain $D$, there exists a polyhedral domain $\Omega$ such that $D\subset\Omega$ and $C(\overline\Omega)\subset C(\overline D)$.

[^2]: $\kappa$ is the Gaussian curvature.

[^3]: The local index of refraction is the ratio between the phase velocity and the wave vector of a plane wave in the medium, $n(\bf{r})=k/\mathcal{K}(\bf{r})$, where $k$ is the wave vector and $\mathcal{K}$ is the wave impedance.

[^4]: In the important references [@HaMaRa1998; @PiVe2003; @LaNa2009; @NaMaSo2011] and in [@JaSt2013] the Hardy inequality holds under an additional assumption on the dimension $n$, the geometric mean of the principal curvatures of $M$ being positive. In our situation it is enough to assume that the principal curvatures are positive and lower-bounded (see (A.1)).

[^5]: Note that this special case was studied in [@St89] and

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