## Abstract A new implementation of perfectly matched layer (PML) using the recursive‐convolution technique is introduced for an alternating‐direction implicit (ADI) finite‐difference time‐domain (FDTD) method. Based on a “complex frequency‐shifted (CFS)” scaling function, this PML boundary conditi
An unsplit Berenger-like PML for the ADI-FDTD method
✍ Scribed by R. Godoy Rubio; S. González García; A. Rubio Bretones; R. Gómez Martín
- Publisher
- John Wiley and Sons
- Year
- 2004
- Tongue
- English
- Weight
- 124 KB
- Volume
- 42
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
In this paper, we systematically obtain an unsplit form of Berenger's PML equations using the alternating‐direction‐implicit finite‐difference time‐domain (ADI‐FDTD) method to prevent some instabilities from appearing in the split‐form implementation. © 2004 Wiley Periodicals, Inc. Microwave Opt Technol Lett 42: 466–469, 2004; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.20338
📜 SIMILAR VOLUMES
## Abstract The relationship of the numerical dispersion relation presented in different mathematical expressions (that are independently derived in 1, 2) for the three‐dimensional alternating direction implicit finite‐difference time‐domain (3D ADI‐FDTD) method is investigated. It is found that, u