Figure 2
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(a) Total absorption calculated as 1-reflectivity shows resonant modes in Si3N4–Si and overall lower absorption in the nanostructured sample. (b) Distribution of electric field intensity and absorption density in Si3N4–Si strongly depends on Si behavior at cavity resonant wavelengths. (c) Partial absorption is calculated by integrating absorption density over first 5 μm or 10 μm of Si in Si and Si3N4–Si, and adding the Au part for Au–Si3N4–Si and Nano-Au–Si3N4–Si. (d) Total absorption of Au ENHA on Si3N4 shows resonant absorption peak at 894 nm. (e) Electric field intensity and absorption density in the first 2 μm of depth of the three samples.
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