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The intensity distribution of the leakage light is proportional to the SPP mode profile.
Fabrication, edge polishing and near-field mode profile measurement of the waveguide are carried out.
In more detail, λ B degrades Q factor more weakly than ρ does because an entire geometric change by λ B remains, to a high degree, the mode profile, while a local geometric change by ρ breaks the mode profile.
The shape of the mode profile in x-direction depends on the loading-strip width as shown in Fig. 5b.
The device operation is simulated by numerical calculations of the hole distributions coupled with the optical guided mode profile.
The calculations, including those for silicate, show a decrease in the band strength but the changes in the stretching mode profile of CO ice are not significant.
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The maxima of mode profiles are located below the metallic NWs.
The insets are mode profiles corresponding to different d and substrate thicknesses t.
c Mode profiles for TM00 in y- and x-directions (indicated by arrows on the TM00 power distribution).
Interestingly, mode hybridizations exist between the fundamental mode M1 and the respective PSSW modes N2 and N4, as borne out by the simulated hybridized mode profiles.
Accurate mode profiles and confinement factors are calculated by Finite Difference mode solver, OptiWave [19, 20], in order to avoid ripples due to Gibbs phenomenon inherent to FMM.
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