Comparison of PML for TVFEM and FDTD

International Journal of Numerical Modelling: Electronic Networks, Devices and Fields

Volumn 13, Issue 2-3, 2000, Pages 233-244

  Wu, J Y ^a   Nehrbass, J ^a   Lee, R ^a  

^a The Ohio State University   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

BOUNDARY CONDITIONS; COMPUTATIONAL GEOMETRY; CONVERGENCE OF NUMERICAL METHODS; FINITE DIFFERENCE METHOD; FINITE ELEMENT METHOD; ITERATIVE METHODS; TIME DOMAIN ANALYSIS; WAVEGUIDES;

FINITE DIFFERENCE TIME DOMAIN METHOD; PERFECTLY MATCHED LAYER; TANGENTIAL VECTOR FINITE ELEMENT METHOD;

MATHEMATICAL MODELS;

EID: 0034159151     PISSN: 08943370     EISSN: None     Source Type: Journal    
DOI: 10.1002/(sici)1099-1204(200003/06)13:2/3<233::aid-jnm358>3.0.co;2-w     Document Type: Article

References (8)

1. Berenger JP. A perfectly matched layer for the absorption of electromagnetic waves. Journal of Computational Physics 1994; 114:185-200.
2. Mittra R, Pekel U. A new look at the perfectly matched layer (PML) concept for the reflectionless absorption of electromagnetic waves. IEEE Microwave and Guided Wave Letters 1995; 5:84-86.
3. Sacks ZS, Kingsland DM, Lee R, Lee JF. A perfectly matched anisotropic absorber for use as an absorbing boundary condition. IEEE Transactions on Antennas Propagation 1995; AP-43:1460-1463.
4. 3. Numeriche Methamatik 1980; 35:315-341.
5. Webb JP, Forghani B. Hierarchical scalar and vector tetrahedra. IEEE Transactions on Magnetics 1993; 29(2):1495-1498.
6. Lee JF, Sun DK, Cendes ZJ. Full-wave analysis of dielectric waveguides using tangential vector finite elements. IEEE Transactions on Microwave Theory and Techniques 1991; MTT-39:1262-1271.
7. Cendes ZJ. Vector finite elements for electromagnetic field. IEEE Transactions on Magnetics 1991; MAG-27:3958-3966.
8. Wu JY, Kingsland DM, Lee JF, Lee R. A comparison of anisotropic PML to Berenger's PML and its application to the finite element method for EM scattering. IEEE Transactions on Antennas and Propagation 1997; AP-45:40-50.