TTI介质中错误伴随对RTM的影响

M. Louboutin, Philipp A. Witte, F. Herrmann
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引用次数: 7

摘要

为了获得准确的地下图像,需要进行各向异性建模和成像。但是,21参数完全波动方程的计算成本太高,不能用于这种情况。横向倾斜的各向同性波动方程是下一个最好的可行的物理表征,用于成像。横向倾斜各向同性成像的主要复杂性是成像条件下的接收波场(数据的反向传播或数据残差)的建模。与各向同性或全物理波方程不同,横向倾斜各向同性波方程不是不自伴随的。这种差异意味着时间反转不能模拟正确的接收器波场,这可能导致不正确的地下图像。在这项工作中,我们推导并实现了伴随波方程,以证明在各向异性建模中精确伴随建模的必要性,并将我们的结果与伴随自由逆时成像进行了比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effects of wrong adjoints for RTM in TTI media
In order to obtain accurate images of the subsurface, anisotropic modeling and imaging is necessary. However, the twenty-one parameter complete wave-equation is too computationally expensive to be of use in this case. The transverse tilted isotropic wave-equation is then the next best feasible representation of the physics to use for imaging. The main complexity arising from transverse tilted isotropic imaging is to model the receiver wavefield (back propagation of the data or data residual) for the imaging condition. Unlike the isotropic or the full physics wave-equations, the transverse tilted isotropic wave-equation is not not self-adjoint. This difference means that time-reversal will not model the correct receiver wavefield and this can lead to incorrect subsurface images. In this work, we derive and implement the adjoint wave-equation to demonstrate the necessity of exact adjoint modeling for anisotropic modeling and compare our result with adjoint-free time-reversed imaging.
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