2011
DOI: 10.1088/0022-3727/44/24/245101
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Implementation of the critical points model in a SFM-FDTD code working in oblique incidence

Abstract: We describe the implementation of the critical points model in a finite-difference-time-domain code working in oblique incidence and dealing with dispersive media through the split field method. Some tests are presented to validate our code in addition to an application devoted to plasmon resonance of a gold nanoparticles grating.

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Cited by 23 publications
(10 citation statements)
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“…The code takes into account the periodicity of the structure in x and y directions via Bloch's boundary conditions [43] and the upper and lower semi-infinite media in z direction through perfectly matched layer (PML) conditions of Berenger [44]. The implemented Critical Points Drude model [45] deals with the dispersive nature of gold and ITO using different fitted parameters to match experimental values. The structure is illuminated, with a plane wave, at normal incidence from the substrate.…”
Section: Methodsmentioning
confidence: 99%
“…The code takes into account the periodicity of the structure in x and y directions via Bloch's boundary conditions [43] and the upper and lower semi-infinite media in z direction through perfectly matched layer (PML) conditions of Berenger [44]. The implemented Critical Points Drude model [45] deals with the dispersive nature of gold and ITO using different fitted parameters to match experimental values. The structure is illuminated, with a plane wave, at normal incidence from the substrate.…”
Section: Methodsmentioning
confidence: 99%
“…The main object studied in this paper is two-dimensional SFM-FDTD, its algorithm prototype can refer to the Ref. [5,6,[8][9][10][11] . Some transformations are made on the original Maxwell equations and overcoming the time bias generated from the time-frequency conversion under oblique incidence [8] .…”
Section: Theory Of Sfm-fdtdmentioning
confidence: 99%
“…6b and their values are given in the caption. The glass substrate optical refractive index is fixed to n s = 1.458 and the dispersion of the silver film is described through a Drude-Critical Points (DCP) model [35] which has been adapted to the studied spectral range (λ ∈[600 nm,1400 nm]).…”
Section: Appendix B: Optimization Of the Geometrymentioning
confidence: 99%