On the implementation of perfectly matched layers in a three‐dimensional fourth‐order velocity‐stress finite difference scheme
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[1] J. Virieux,et al. Dynamic faulting studied by a finite difference method : Bull seismol soc am, V72, N2, April 1982, P345–369 , 1982 .
[2] Jian-Ming Jin,et al. Conformal PML-FDTD schemes for electromagnetic field simulations: a dynamic stability study , 2001 .
[3] J. Bérenger. Three-Dimensional Perfectly Matched Layer for the Absorption of Electromagnetic Waves , 1996 .
[4] Kim B. Olsen,et al. Site Amplification in the Los Angeles Basin from Three-Dimensional Modeling of Ground Motion , 2000 .
[5] Robert L. Higdon,et al. Radiation boundary conditions for elastic wave propagation , 1990 .
[6] D. Wald,et al. Spatial and temporal distribution of slip for the 1992 Landers, California, earthquake , 1994, Bulletin of the Seismological Society of America.
[7] E. Husebye,et al. 3-D versus 2-D finite-difference seismic synthetics including real surface topography , 1999 .
[8] Jin-Fa Lee,et al. Stability Analysis for Perfectly Matched Layered Absorbers , 1996 .
[9] C. Randall,et al. Absorbing boundary condition for the elastic wave equation , 1988 .
[10] C. Randall,et al. Absorbing boundary condition for the elastic wave equation: Velocity‐stress formulation , 1989 .
[11] B. Engquist,et al. Absorbing boundary conditions for acoustic and elastic wave equations , 1977, Bulletin of the Seismological Society of America.
[12] O. Ramahi. Stability of absorbing boundary conditions , 1999 .
[13] Jiayuan Fang,et al. Numerical implementation and performance of perfectly matched layer boundary condition for waveguide structures , 1995 .
[14] Qing Huo Liu,et al. PERFECTLY MATCHED LAYERS FOR ELASTODYNAMICS: A NEW ABSORBING BOUNDARY CONDITION , 1996 .
[15] David Gottlieb,et al. A Mathematical Analysis of the PML Method , 1997 .
[16] Qing Huo Liu,et al. The application of the perfectly matched layer in numerical modeling of wave propagation in poroelastic media , 2001 .
[17] Stig Hestholm,et al. Instabilities in applying absorbing boundary conditions to high‐order seismic modeling algorithms , 1998 .
[18] Robert L. Higdon,et al. Absorbing boundary conditions for di erence approxima-tions to the multidimensional wave equation , 1986 .
[19] J. Virieux. P-SV wave propagation in heterogeneous media: Velocity‐stress finite‐difference method , 1986 .
[20] John B. Schneider,et al. Application of the perfectly matched layer (PML) absorbing boundary condition to elastic wave propagation , 1996 .
[21] C. Tsogka,et al. Application of the perfectly matched absorbing layer model to the linear elastodynamic problem in anisotropic heterogeneous media , 2001 .
[22] Moshe Reshef,et al. A nonreflecting boundary condition for discrete acoustic and elastic wave equations , 1985 .
[23] Albert C. Reynolds,et al. Boundary conditions for the numerical solution of wave propagation problems , 1978 .
[24] Robert W. Graves,et al. The seismic response of the Los Angeles basin, California , 1998, Bulletin of the Seismological Society of America.
[25] K. B. Olsen,et al. Constraints on Stress and Friction from Dynamic Rupture Models of the 1994 Northridge, California, Earthquake , 2000 .
[26] K. Olsen,et al. 3D Viscoelastic Wave Propagation in the Upper Borrego Valley, California, Constrained by Borehole and Surface Data , 2000 .
[27] R. Higdon. Absorbing boundary conditions for difference approximations to the multi-dimensional wave equation , 1986 .
[28] Robert W. Graves,et al. The SCEC Southern California Reference Three-Dimensional Seismic Velocity Model Version 2 , 2000 .
[29] Kim B. Olsen,et al. Three-dimensional simulation of earthquakes on the Los Angeles fault system , 1996, Bulletin of the Seismological Society of America.
[30] J. Sochacki. Absorbing boundary conditions for the elastic wave equations , 1988 .
[31] Ellen Gottschämmer,et al. Accuracy of the Explicit Planar Free-Surface Boundary Condition Implemented in a Fourth-Order Staggered-Grid Velocity-Stress Finite-Difference Scheme , 2001 .
[32] R. Madariaga,et al. Dynamic modeling of the 1992 Landers earthquake , 2001 .
[33] F. Hu. A Stable, perfectly matched layer for linearized Euler equations in unslit physical variables , 2001 .
[34] Qing Huo Liu,et al. The perfectly matched layer for acoustic waves in absorptive media , 1997 .
[35] Jean-Pierre Berenger,et al. A perfectly matched layer for the absorption of electromagnetic waves , 1994 .
[36] Robert W. Graves,et al. Three-dimensional finite-difference modeling of the San Andreas fault: Source parameterization and ground-motion levels , 1998, Bulletin of the Seismological Society of America.
[37] R. Madariaga. Dynamics of an expanding circular fault , 1976, Bulletin of the Seismological Society of America.
[38] K. Olsen. THREE-DIMENSIONAL GROUND MOTION SIMULATIONS FOR LARGE EARTHQUAKES ON THE SAN ANDREAS FAULT WITH DYNAMIC AND OBSERVATIONAL CONSTRAINTS , 2001 .
[39] Kim B. Olsen,et al. Three-Dimensional Dynamic Simulation of the 1992 Landers Earthquake , 1997 .
[40] Christopher K. W. Tam,et al. Perfectly Matched Layer as an Absorbing Boundary Condition for the Linearized Euler Equations in Open and Ducted Domains , 1998 .
[41] Qing Huo Liu,et al. Acoustic detection of buried objects in 3-D fluid saturated porous media: numerical modeling , 2001, IEEE Trans. Geosci. Remote. Sens..
[42] L. Trefethen,et al. III‐posedness of absorbing boundary conditions for migration , 1988 .
[43] Kim B. Olsen,et al. Three-Dimensional Simulation of a Magnitude 7.75 Earthquake on the San Andreas Fault , 1995, Science.