Complex space approach to perfectly matched layers: a review and some new developments
By Fernando Lisboa Teixeira, Weng Cho Chew. 2000
147 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering
View Paper: https://www.semanticscholar.org/paper/31c2312c66b7b365385612bea3f44e72a6c3815b
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
- David S. Bindel
- Sanjay Govindjee
- U. Basu
- Fernando Lisboa Teixeira
- Yang Shen
- Wei Zhang
- Jeroen Tromp
- Dimitri Komatitsch
In Atomic and Molecular Physics, and Optics
- U. Basu
- A. Chopra
- Fernando Lisboa Teixeira
- Yang Shen
- David S. Bindel
- Wei Zhang
- Sanjay Govindjee
- Dimitri Komatitsch
In Electrical and Electronic Engineering
- U. Basu
- David S. Bindel
- Sanjay Govindjee
- A. Chopra
- Fernando Lisboa Teixeira
- Yang Shen
- Wei Zhang
- Dimitri Komatitsch
Citations in the corpus
- Unsplit complex frequency-shifted PML implementation using auxiliary differential equations for seismic wave modeling (2010, background): “…of the PML as an artificial anisotropic medium Sacks et al., 1995; Gedney, 1996 or complex coordinate stretching Chew and Weedon, 1994; Teixeira and Chew, 2000 have led to unsplit-field PML implementations involving convolution terms Wang and Tang, 2003; Komatitsch and Martin, 2007 ,…”
- Perfectly matched layers for time-harmonic elastodynamics of unbounded domains : Theory and finite-element implementation (2003, background): “These observations––especially the third––mirror similar ones made in the context of electromagnetic waves [34,36,49], where PMLs have been formulated for anisotropic, inhomogeneous media [36], underscoring the possibility of extending these elastodynamic PML formulations to anisotropic, continuousl”
- Elastic PMLs for resonator anchor loss simulation (2005, background): “3 linear wave equation [13, 32, 30 ]. Not only do these layers rapidly attenuate waves, they also \perfectly match" the rest of the domain; that is, there are no spurious reections at the interface due to perfect impedance matching.”
- Time-Domain Finite-Difference and Finite-Element Methods for Maxwell Equations in Complex Media (2008, background): “The most versatile ABC for complex media is the perfectly matched layer (PML) [263]–[268], which can be implemented for either FDTD [263], [264], [269]–[274], or FETD [275]–[279].”