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DOI | 10.1111/j.1365-2478.2008.00748.x |
Comparison between the Fourier finite-difference method and the generalized-screen method | |
Zhang, Jin-Hai; Wang, Wei-Min; Yao, Zhen-Xing | |
通讯作者 | Zhang, JH (通讯作者) |
发表日期 | 2009 |
ISSN | 0016-8025 |
EISSN | 1365-2478 |
起始页码 | 355 |
结束页码 | 365 |
卷号 | 57期号:3 |
英文摘要 | The Fourier finite-difference propagator and the generalized-screen propagator are two general high-order forms of one-way dual-domain methods. We compare these two propagators mainly on phase accuracy, computational efficiency and 3D extension. A comparison of phase accuracy shows that the high-order generalized-screen propagator is preferable to the Fourier finite-difference propagator for heterogeneous media with a weak velocity contrast and wide dip angle. With increasing velocity contrast, the accuracy improvement gained by the high-order generalized-screen propagator declines rapidly. The Fourier finite-difference propagator is more robust and flexible to lateral velocity variations than the generalized-screen propagator. The 2D Fourier finite-difference propagator is superior to the 2D generalized-screen propagator when the velocity contrast is stronger than 23%. Despite the two-way splitting error, the 3D Fourier finite-difference propagator is more accurate than the second-order generalized-screen propagator when the velocity contrast is stronger than 20% and is more accurate than the fourth-order generalized-screen propagator when the velocity contrast is stronger than 40%. Numerical experiments on the SEG/EAGE salt model demonstrate that the Fourier finite-difference propagator behaves better than the generalized-screen propagator when imaging steep salt boundary and faults beneath the salt body. Under the same hardware and software conditions, the computational cost of the Fourier finite-difference propagator in our implementation is greater than that of the second-order generalized-screen propagator but smaller than that of the third-order generalized-screen propagator. Compared with the Fourier finite-difference propagator, the generalized-screen propagator requires fewer grid points per wavelength and has more potential to improve running speed in the presence of a much faster Fourier transform. These analyses are applicable for both forward modelling and depth migration. |
关键词 | DEPTH MIGRATIONONE-WAYEXTRAPOLATIONPROPAGATION |
语种 | 英语 |
WOS研究方向 | Geochemistry & Geophysics |
WOS类目 | Geochemistry & Geophysics |
WOS记录号 | WOS:000264821200004 |
来源期刊 | GEOPHYSICAL PROSPECTING |
来源机构 | 中国科学院青藏高原研究所 |
文献类型 | 期刊论文 |
条目标识符 | http://gcip.llas.ac.cn/handle/2XKMVOVA/257631 |
推荐引用方式 GB/T 7714 | Zhang, Jin-Hai,Wang, Wei-Min,Yao, Zhen-Xing. Comparison between the Fourier finite-difference method and the generalized-screen method[J]. 中国科学院青藏高原研究所,2009,57(3). |
APA | Zhang, Jin-Hai,Wang, Wei-Min,&Yao, Zhen-Xing.(2009).Comparison between the Fourier finite-difference method and the generalized-screen method.GEOPHYSICAL PROSPECTING,57(3). |
MLA | Zhang, Jin-Hai,et al."Comparison between the Fourier finite-difference method and the generalized-screen method".GEOPHYSICAL PROSPECTING 57.3(2009). |
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