Dispersive VP-EP conformal mesh algorithm in FDTD for a CCPR model

A dispersive volume-average polarized effective permittivity (D-VP-EP) algorithm is introduced for the analysis of arbitrarily shaped three-dimensional dispersive materials, utilizing the complex-conjugate pole-residue (CCPR) model within the finite-difference time-domain (FDTD) method. The D-VP-EP employs the fitting algorithm as the preprocessor in the frequency domain, followed by an interpolation algorithm in the spatial domain, to avoid conformal-induced changes in the form of the constitutive equations during subsequent conformal mesh generation. The D-VP-EP algorithm maintains the iterative formulation of conventional CCPR-FDTD while enabling conformal meshing between 2 dispersive materials with an arbitrary number of poles. In scattering simulations of metal-dielectric dispersive bilayer nanosphere and transmission spectrum simulations of a dispersive micro-ring, the D-VP-EP effectively reduces mesh mismatch errors at curved interfaces when compared to volume-averaged or staircase, and only needs 1/16 of the computing resources of the comparison group to achieve the same accuracy.

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Publication Details

Journal
Optics Express
Published
2026-01-05
DOI
https://doi.org/10.1364/oe.584767
Primary Topic
Electromagnetic Simulation and Numerical Methods
Type
article
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article

Dispersive VP-EP conformal mesh algorithm in FDTD for a CCPR model

Liuge Du, Y. Zhou, Xiao Xu, Fan Yuan et al.
Optics Express
Electromagnetic Simulation and Numerical Methods
article

Dispersive VP-EP conformal mesh algorithm in FDTD for a CCPR model

Liuge Du, Y. Zhou, Xiao Xu, Fan Yuan, Jia Zhao, Yanan Liu, Han Liu, Fanmin Kong
article en

Abstract

A dispersive volume-average polarized effective permittivity (D-VP-EP) algorithm is introduced for the analysis of arbitrarily shaped three-dimensional dispersive materials, utilizing the complex-conjugate pole-residue (CCPR) model within the finite-difference time-domain (FDTD) method. The D-VP-EP employs the fitting algorithm as the preprocessor in the frequency domain, followed by an interpolation algorithm in the spatial domain, to avoid conformal-induced changes in the form of the constitutive equations during subsequent conformal mesh generation. The D-VP-EP algorithm maintains the iterative formulation of conventional CCPR-FDTD while enabling conformal meshing between 2 dispersive materials with an arbitrary number of poles. In scattering simulations of metal-dielectric dispersive bilayer nanosphere and transmission spectrum simulations of a dispersive micro-ring, the D-VP-EP effectively reduces mesh mismatch errors at curved interfaces when compared to volume-averaged or staircase, and only needs 1/16 of the computing resources of the comparison group to achieve the same accuracy.

Optics ExpressVol. 34(2)
Shandong University (CN), Laser Research Institute (CN)
Openalex Percentile: Top 97%
Electromagnetic Simulation and Numerical Methods
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Dispersive VP-EP conformal mesh algorithm in FDTD for a CCPR model — Liuge Du, Y. Zhou, et al. · Optics Express (2026) | TGRS Research Map | TGRS