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The influences of the gap, outer radius, and rod width are systematically investigated.
For the anti-symmetric mode, the resonance peak red shifts to long wavelength when the rod width decreases.
Clearly, when the rod width is decreased from 120 to 65 nm, the field intensity at the gap center can be further increased.
The near-field intensity can be greatly enhanced by adjusting the rod width and gap distance, promoting the lightning-rod effect and plasmon coupling.
In other words, the optical field can be improved by several orders of magnitude by modifying the gap distance or the rod width of a nanorod dimer.
c Field intensity distributions of the anti-symmetric modes of MINE structures along the x-direction with different rod widths Fig. 11 Schematic illustrations of the instantaneous charge distributions in MINE structures: the influences of rod width.
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b Extinction spectra of the MINE structures with different rod widths for both experiment and simulation.
Fig. 10 a SEM images of the fabricated MINE structures with different rod widths.
The field intensity distributions of the anti-symmetric mode along the x-direction under different rod widths are plotted in Fig. 10c.
The TEM images prove that the nanoscale rods (width: about 3 nm) are aggregated with each other to form nanoscale porosity.
The other two factors B and D, i.e., pole length (L) and radial distance from piston rod to coil width (H), are having 26.97% and 3.05% percentage contribution, respectively.
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