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Figure 30 shows the comparison between the maximum frequency of the four modes as a function of the ω b.
The HHs present strongly localized transmission modes as a function of the design parameters and can be localized over a wide range of frequencies.
Figure 4c also shows the number of lasing modes as a function of the size of the microcavities just above their lasing threshold.
The technique focuses on the response of the material's resonance modes as a function of the driving amplitude by sweeping the frequency at various drive levels.
Figure 7 shows LEE for the TE and TM modes as a function of the refractive index of AlGaN when the rod diameter and height are 260 and 1,000 nm, respectively.
The parameters are γ = 1.03122, Ω ce = 0.04 and ω b = 0.04. Figure 24a shows the comparison between the maximum growth rates of the four modes as a function of the plasma frequency.
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Essentially a second order ordinary differential equation is solved for each mode as a function of the generalised coordinates.
The tunability of defect mode was investigated, as a function of the electric field alongside the incident angle.
Figure 29 shows the comparison between the maximum growth rate of the four modes as a function of ω b.
Figure 7 Eigenvalues of the normal modes as a function of for.
c Peak wavelengths of the two resonance modes as a function of structure angle.
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