Third-order effective permittivities for the 4th-order FDTD method in the 2D TM polarization case

The effective permittivities at dielectric interfaces for the 4th-order finite-difference time-domain (FDTD) method using a symplectic integrator propagator are proposed for the two-dimensional (2-D) TM polarization case. For a given accuracy level, the memory resources required by the 4th-order FDTD method with the effective permittivities are reduced by more than an order of magnitude with comparison to the standard FDTD method. The CPU time is also reduced. The permittivities are derived by matching the numerical reflection and transmission at the interface to the exact ones in 3rd-order accuracy. The accurate performance of the proposed method is demonstrated by various numerical examples.

[1]  Steven G. Johnson,et al.  High-density integrated optics , 1999 .

[2]  Allen Taflove,et al.  Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .

[3]  H Melchior,et al.  General self-imaging properties in N × N multimode interference couplers including phase relations. , 1994, Applied optics.

[4]  Mk Meint Smit,et al.  New small-size single-mode optical power splitter based on multi-mode interference , 1992 .

[5]  Weng Cho Chew,et al.  Modeling of rough-surface effects in an optical turning mirror using the finite-difference time-domain method , 1991 .

[6]  D. R. Wight,et al.  Novel 1‐to‐N way integrated optical beam splitters using symmetric mode mixing in GaAs/AlGaAs multimode waveguides , 1992 .

[7]  E. Turkel,et al.  Fourth order method for Maxwell equations on a staggered mesh , 1997, IEEE Antennas and Propagation Society International Symposium 1997. Digest.

[8]  Sai T. Chu,et al.  A finite-difference time-domain method for the design and analysis of guided-wave optical structures , 1989 .

[9]  Wojciech K. Gwarek,et al.  Higher-Order Modelling of Media Interfaces for Enhanced FDTD Analysis of Microwave Circuits , 1994, 1994 24th European Microwave Conference.

[10]  D.W. Zingg High-order finite-difference methods in computational electromagnetics , 1997, IEEE Antennas and Propagation Society International Symposium 1997. Digest.

[11]  Sai T. Chu,et al.  Simulation and analysis of waveguide based optical integrated circuits , 1991 .

[12]  Amir Yefet,et al.  A staggered fourth-order accurate explicit finite difference scheme for the time-domain Maxwell's equations , 2001 .

[13]  E. R. Thoen,et al.  Ultra-compact Si-SiO2 microring resonator optical channel dropping filters , 1998, IEEE Photonics Technology Letters.

[14]  E.C.M. Pennings,et al.  Optical multi-mode interference devices based on self-imaging: principles and applications , 1995 .

[15]  S.,et al.  Numerical Solution of Initial Boundary Value Problems Involving Maxwell’s Equations in Isotropic Media , 1966 .

[16]  Yuzo Yoshikuni,et al.  The second-order condition for the dielectric interface orthogonal to the Yee-lattice axis in the FDTD scheme , 2000 .

[17]  J. Hesthaven,et al.  Convergent Cartesian Grid Methods for Maxwell's Equations in Complex Geometries , 2001 .

[18]  Jeffrey L. Young,et al.  Toward the construction of a fourth-order difference scheme for transient EM wave simulation: staggered grid approach , 1997 .

[19]  Yuzo Yoshikuni,et al.  A three-dimensional fourth-order finite-difference time-domain scheme using a symplectic integrator propagator , 2001 .

[20]  S. Chu,et al.  A scalar finite-difference time-domain approach to guided-wave optics , 1991, IEEE Photonics Technology Letters.

[21]  R. LeVeque,et al.  The immersed interface method for acoustic wave equations with discontinuous coefficients , 1997 .

[22]  J. Hesthaven,et al.  Staircase-free finite-difference time-domain formulation for general materials in complex geometries , 2001 .

[23]  J. Yamauchi,et al.  Analysis of optical waveguides with high-reflection coatings using the FD-TD method , 1998, IEEE Photonics Technology Letters.

[24]  Yong-Zhen Huang,et al.  Resonant frequencies and quality factors for optical equilateral triangle resonators calculated by FDTD technique and the Pade approximation , 2000, IEEE Photonics Technology Letters.

[25]  Jean-Pierre Berenger,et al.  A perfectly matched layer for the absorption of electromagnetic waves , 1994 .

[26]  A. Koster,et al.  Analysis of integrated optical waveguide mirrors , 1997 .

[27]  S. Seki,et al.  Successful applications of PML-ABC to the symplectic FDTD scheme with 4th-order accuracy in time and space , 1999, 1999 IEEE MTT-S International Microwave Symposium Digest (Cat. No.99CH36282).

[28]  Z. Popovic,et al.  Surface-wave guiding using periodic structures , 2000, IEEE Antennas and Propagation Society International Symposium. Transmitting Waves of Progress to the Next Millennium. 2000 Digest. Held in conjunction with: USNC/URSI National Radio Science Meeting (C.

[29]  W. Tabbara,et al.  A fourth order scheme for the FDTD algorithm applied to Maxwell's equations , 1992, IEEE Antennas and Propagation Society International Symposium 1992 Digest.

[30]  Shanhui Fan,et al.  Optical filters from photonic band gap air bridges , 1996 .

[31]  M. Robertson,et al.  New formula for semiconductor laser facet reflectivity , 1993, IEEE Photonics Technology Letters.

[32]  J. Joannopoulos,et al.  High Transmission through Sharp Bends in Photonic Crystal Waveguides. , 1996, Physical review letters.