2012
DOI: 10.1109/jphot.2012.2198914
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A Slot-Based Surface Plasmon-Polariton Waveguide With Long-Range Propagation and Superconfinement

Abstract: A full-vector spectral element method (SEM) is applied to model and simulate surface plasmon-polariton (SPP) waveguides. Gauss-Lobatto-Legendre (GLL) polynomials are used to construct higher-order basis functions to achieve spectral accuracy. A discretization scheme featuring a nonuniform mesh with extra elements near the metal-dielectric interface is proposed to capture the waveguide configuration and dramatical mode field variations of the SPP waveguide. The studies on the accuracy and mode field distributio… Show more

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Cited by 16 publications
(4 citation statements)
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“…The primary design of a high-index GaAs curved waveguide with n GaAS = 3.4 is capable of strong light confinement over a wide RI range. A width and a radius of curvature for the curved waveguide were determined by a conformal transformation 18 and the Helmholtz equation to optimize bending losses 19 . The optimal width and the radius of the curved single mode waveguide are w = 0.25 μm and Rc = 5 μm.…”
Section: Resultsmentioning
confidence: 99%
“…The primary design of a high-index GaAs curved waveguide with n GaAS = 3.4 is capable of strong light confinement over a wide RI range. A width and a radius of curvature for the curved waveguide were determined by a conformal transformation 18 and the Helmholtz equation to optimize bending losses 19 . The optimal width and the radius of the curved single mode waveguide are w = 0.25 μm and Rc = 5 μm.…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, the GLL polynomials bring in an interesting distribution of nodal points, who are denser near the boundary of an discretized element than in the middle of it. This unique property of SEM makes it suitable for the simulation of surface plasmon phenomenon, since the surface plasmon field would dramatically change near the metal-dielectric interface [32].…”
Section: Modeling Methodsmentioning
confidence: 99%
“…Specifically, the energy of a SPP is typically concentrated within approximately one skin depth of the metal-dielectric interface, resulting in large Ohmic losses within the metal layer. Progress has been made in increasing the propagation length of SPP modes through strategic structural designs that move more of the electric field away from the metal film [15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30]. However, this comes at the cost of structural complexity, and the useful range of a typical plasmonic excitation remains in the micrometer range.…”
Section: Introductionmentioning
confidence: 99%