2012Journal of Geophysics and EngineeringOpen access

An unsplit complex-frequency-shifted PML based on matchedZ-transform for FDTD modelling of seismic wave equations

Rui-Qi Shi, Shangxu Wang, Jianguo Zhao

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Abstract

The perfectly matched layer (PML) is an efficient absorbing boundary condition for mitigating undesired reflections in seismic wave modelling. However, the performance of the conventional split-field PML (S-PML) is severely reduced at grazing incidence. Very low frequency waves and evanescent waves can also cause spurious reflections on the PML interface. Such problems could be circumvented by using the complex-frequency-shifted (CFS) stretching tensor in the PML. However, it is difficult to adopt the CFS stretching tensor in the S-PML. A matched Z-transform PML (MZT-PML) technique applied in electromagnetic modelling results in a complete unsplit-field form. In this paper, we show that the MZT-PML can easily implement the CFS stretching tensor and be adopted for elastic wave finite-difference time-domain modelling. The numerical tests in an elongated model illustrate that the complex-frequency-shifted matched Z-transform perfectly matched layer (CFS MZT-PML) can substantially improve performance by eliminating the spurious reflections at grazing incidence. The numerical stability of the CFS MZT-PML is verified by long time computation of the total energy. Also, we conduct a numerical test in a two-layer heterogeneous model showing that the CFS MZT-PML can also be used to simulate efficiently the wave propagation in more complex structures.

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The perfectly matched layer (PML) is an efficient absorbing boundary condition for mitigating undesired reflections in seismic wave modelling. However, the performance of the conventional split-field PML (S-PML) is severely reduced at grazing incidence. Very low frequency waves and evanescent waves can also cause spurious reflections on the PML interface. Such problems could be circumvented by using the complex-frequency-shifted (CFS) stretching tensor in the PML. However, it is difficult to adopt the CFS stretching tensor in the S-PML. A matched Z-transform PML (MZT-PML) technique applied in electromagnetic modelling results in a complete unsplit-field form. In this paper, we show that the MZT-PML can easily implement the CFS stretching tensor and be adopted for elastic wave finite-difference time-domain modelling. The numerical tests in an elongated model illustrate that the complex-frequency-shifted matched Z-transform perfectly matched layer (CFS MZT-PML) can substantially improve performance by eliminating the spurious reflections at grazing incidence. The numerical stability of the CFS MZT-PML is verified by long time computation of the total energy. Also, we conduct a numerical test in a two-layer heterogeneous model showing that the CFS MZT-PML can also be used to simulate efficiently the wave propagation in more complex structures.

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Available abstract

The perfectly matched layer (PML) is an efficient absorbing boundary condition for mitigating undesired reflections in seismic wave modelling. However, the performance of the conventional split-field PML (S-PML) is severely reduced at grazing incidence. Very low frequency waves and evanescent waves can also cause spurious reflections on the PML interface. Such problems could be circumvented by using the complex-frequency-shifted (CFS) stretching tensor in the PML. However, it is difficult to adopt the CFS stretching tensor in the S-PML. A matched Z-transform PML (MZT-PML) technique applied in electromagnetic modelling results in a complete unsplit-field form. In this paper, we show that the MZT-PML can easily implement the CFS stretching tensor and be adopted for elastic wave finite-difference time-domain modelling. The numerical tests in an elongated model illustrate that the complex-frequency-shifted matched Z-transform perfectly matched layer (CFS MZT-PML) can substantially improve performance by eliminating the spurious reflections at grazing incidence. The numerical stability of the CFS MZT-PML is verified by long time computation of the total energy. Also, we conduct a numerical test in a two-layer heterogeneous model showing that the CFS MZT-PML can also be used to simulate efficiently the wave propagation in more complex structures.

Key concepts: Perfectly matched layer, Finite-difference time-domain method, Spurious relationship, Tensor (intrinsic definition), Boundary value problem, Incidence (geometry), Physics, Mathematical analysis

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