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The results we showed are useful for manipulation of plasmon modes in plasmonic nanostructures.
The hybridized modes in plasmonic molecules have been extensively studied.
However, the propagation lengths of the tightly confined modes in plasmonic waveguides are not large enough due to the presence of ohmic losses in the dissipative metal regions.
However, due to ohmic loss of metal [13], the propagation lengths of guided modes in plasmonic waveguides are typically short under tight confinement, which greatly limits the scope for practical applications.
Recently, strong light-matter coupling between the electromagnetic modes in plasmonic metasurfaces with quantum-engineering electronic intersubband transitions in quantum wells has been demonstrated experimentally (Benz et al., [14], Lee et al., [15]).
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Mode hybridization of photonic and plasmonic modes in hybrid plasmonic (HP) waveguide is proposed to achieve low-loss sub-wavelength (nano-scale) optical-confinement with variable optical nonlinearity.
The stack of a half nanoring creates a path for realizing different Fano resonance modes in the plasmonic resonant system.
a Plasmonic modes in different graphene structures: infinite sheet, edge, ribbon and single-walled tube (left), and the corresponding graphene plasmon modes (right).
We study analytically the plasmonic modes in the graphene-coated dielectric nanowire, based on the explicit form of nonlinear surface conductivity of graphene.
So, here, we demonstrate the E y profiles of the symmetric hybrid plasmonic modes in the AHPMW waveguide for the widths of the silver nanowire varying from 5 to 150 nm in Figure 2a.
In order to study the propagation of these surface waves (SPs) and formation of plasmonic modes in the gap distance between metals, we use both numerical and analytical methods.
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