2005
DOI: 10.1364/opex.13.010367
|View full text |Cite
|
Sign up to set email alerts
|

Contour-path effective permittivities for the two-dimensional finite-difference time-domain method

Abstract: Effective permittivities for the two-dimensional Finite- Difference Time-Domain (FDTD) method are derived using a contour path approach that accounts for the boundary conditions of the electromagnetic field at dielectric interfaces. A phenomenological formula for the effective permittivities is also proposed as an effective and simpler alternative to the previous result. Our schemes are validated using Mie theory for the scattering of a dielectric cylinder and they are compared to the usual staircase and the w… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
44
0

Year Published

2007
2007
2023
2023

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 52 publications
(44 citation statements)
references
References 32 publications
0
44
0
Order By: Relevance
“…The conformal FDTD method on non-orthogonal grids [15][16][17], counter path FDTD method [18,19], and subgridding method [20][21][22] can represent curved interfaces suitably, but they are relatively difficult to implement and increase the memory and computation time. A different approach using effective permittivities (EPs), which derives from interface interpolations based on Ampere's and Faraday's integration laws, can reduce the error of the permittivity model on coarse grids in a simple implementation and at low computational cost [23][24][25][26][27][28][29][30][31][32][33][34][35]. The EP method, however, is not effective for plasmonic materials because the SP resonance condition is changed on interfaces due to interpolated values of EPs.…”
Section: Introductionmentioning
confidence: 99%
“…The conformal FDTD method on non-orthogonal grids [15][16][17], counter path FDTD method [18,19], and subgridding method [20][21][22] can represent curved interfaces suitably, but they are relatively difficult to implement and increase the memory and computation time. A different approach using effective permittivities (EPs), which derives from interface interpolations based on Ampere's and Faraday's integration laws, can reduce the error of the permittivity model on coarse grids in a simple implementation and at low computational cost [23][24][25][26][27][28][29][30][31][32][33][34][35]. The EP method, however, is not effective for plasmonic materials because the SP resonance condition is changed on interfaces due to interpolated values of EPs.…”
Section: Introductionmentioning
confidence: 99%
“…If the collision frequency γ = 0, then (31) reduces to the numerical permittivity for lossless LHMs given in [28]. Previously we have used an FDTD cell size of ∆x = λ/100 in simulations.…”
Section: Effects Of Numerical Materials Parametersmentioning
confidence: 99%
“…However, these techniques were mainly related to the non-dispersive FDTD methods, and applications in dispersive FDTD methods have not attracted sufficient attention. In [31][32][33], a dispersive contour-path FDTD method was proposed. Nevertheless, this method could only deal with a single metal-dielectric interface.…”
Section: Introductionmentioning
confidence: 99%