Abstract

We analyze the experimental data on the evolution of the microwave (MW) response of the whispering gallery mode (WGM) resonator. The focus is on the thickness $d_{f}$ variation of the conducting endplates (CEPs) from $d_{f}$ exceeding skin layer thickness $\delta _{s}$ to $d_{f}\ll \delta _{s}$ down to $d_{f} = 0$ , i.e., with no CEPs. The analysis was performed by comparing the numerical simulation results obtained using COMSOL software with the authors’ experimental data on the response of the Ka -band sapphire WGM resonator. The nonmonotonic change in the WGM resonator response with decreasing thickness $d_{f}$ is explained using the metal–insulator percolation model proposed by Krupka et al. We use a different resonator (quasi-optical) technique and different mode polarization, namely, the HE $_{14~1~\delta }$ mode. The artificially introduced discontinuity of the ultrathin film, resulting in a sharp growth of the ${Q}$ -factor is analogous with the percolation material structure. The revealed effect may be useful for the development of MW devices with dynamically controlled properties of metamaterials.

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