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Nanoscale Fabry–Pérot Interferometer using channel plasmon-polaritons in triangular metallic grooves
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10.1063/1.1905799
/content/aip/journal/apl/86/16/10.1063/1.1905799
http://aip.metastore.ingenta.com/content/aip/journal/apl/86/16/10.1063/1.1905799
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Figures

Image of FIG. 1.
FIG. 1.

(a) The structures with a V-groove subwavelength waveguide with two metallic membranes (mirrors) forming a Fabry–Pérot interferometer of length . CPP modes are generated by the end-fire excitation using a bulk plane wave incident at the angle of 45° to the axis. The incident wave is generated by the component of the magnetic field. (b), (c) The dependencies of the amplitudes of the electric field: (b) in the middle of the cavity, and (c) in the wave transmitted through the cavity on cavity length for the silver-vacuum structure at the vacuum wavelength in the absence of dissipation (the dielectric permittivity of the metal is real: ) at three different moments of time (dotted curves), (dashed curves), and (solid curves). The thickness of the cavity mirrors , . The electric field amplitudes are normalized to the amplitude of the incident wave at the point of consideration in the absence of the cavity.

Image of FIG. 2.
FIG. 2.

The steady-state dependencies of the amplitudes of the electric field: (a) in the middle of the cavity and (b) in the wave transmitted through the cavity on cavity length in the presence of dissipation at different thicknesses of the cavity mirrors: (1) , (2) , (3) , (4) . , . The electric field amplitudes are normalized to the amplitude of the incident wave at the point of consideration in the absence of the cavity (membranes).

Image of FIG. 3.
FIG. 3.

(a) The time dependencies of the normalized amplitude of the electric field in front of the cavity (solid curve), in the middle of the cavity (dashed curves), and behind the cavity (dotted curves) at two different cavity lengths: (curves 1–3), and (b) (curves 1, 4, 5). , and the other structural parameters are the same as for Fig. 2. (b) The distribution of the magnitude of the electric field in the plane inside the groove, cavity and the mirrors at the resonant cavity length and . The scale along the axis in the mirrors and the cavity is five and ten times larger than outside of the cavity. These regions are indicated by four dashed vertical lines. The end-fire excitation occurs at .

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/content/aip/journal/apl/86/16/10.1063/1.1905799
2005-04-11
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Nanoscale Fabry–Pérot Interferometer using channel plasmon-polaritons in triangular metallic grooves
http://aip.metastore.ingenta.com/content/aip/journal/apl/86/16/10.1063/1.1905799
10.1063/1.1905799
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