Abstract
A new finite-difference time-domain (FDTD) algorithm is introduced to solve two dimensional (2D) transverse magnetic (TM) modes with a straight dispersive interface. Driven by the consideration of simplifying interface jump conditions, the auxiliary differential equation of the Debye constitution model is rewritten to form a new Debye-Maxwell TM system. Interface auxiliary differential equations are utilized to describe the transient changes in the regularities of electromagnetic fields across a dispersive interface. The resulting time dependent jump conditions are rigorously enforced in the FDTD discretization by means of a matched interface and boundary scheme. Higher order convergences are numerically achieved for the first time in the literature in 2D FDTD simulations of dispersive inhomogeneous media.
Original language | English |
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Pages (from-to) | 699-707 |
Number of pages | 9 |
Journal | Applied Mathematics and Computation |
Volume | 226 |
DOIs | |
State | Published - 2014 |
Bibliographical note
Funding Information:This work is supported in part by the NSF Grants DMS-1016579 and DMS-1318898 .
Keywords
- Auxiliary differential equation
- Debye dispersive medium
- Finite-difference time-domain (FDTD)
- High order interface treatments
- Matched interface and boundary (MIB)
- Maxwell's equations
ASJC Scopus subject areas
- Computational Mathematics
- Applied Mathematics