Fig. 4


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The sensitivity of the (b), (d), (f) real and (c), (e), (g) imaginary parts of the eigenfrequencies to (b), (c) gyration resistance, (d), (e) positive capacitance C1 (f), (g) positive inductance L1 perturbation. Solid lines: solution of eigenvalue problem of equatoin (18); green-dashed lines: Puiseux series approximation truncated to its second term. Here, both resonators are unstable, i.e., resonance frequency of resonators is purely imaginary. Voltage v1 (t) under the EPD condition in the (h) time-domain, and (i) frequency-domain. The frequency-domain result is calculated by applying an FFT with 106 samples in the time window of 0 μs to 100 μs.

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