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2D Laplace-Domain Waveform Inversion of Field Data Using a Power Objective Function

机译:使用功率目标函数对场数据进行二维拉普拉斯域波形反演

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The wavefield in the Laplace domain has a very small amplitude except only near the source point. In order to deal with this characteristic, the logarithmic objective function has been used in many Laplace domain inversion studies. The Laplace-domain waveform inversion using the logarithmic objective function has fewer local minima than the time- or frequency domain inversion. Recently, the power objective function was suggested as an alternative to the logarithmic objective function in the Laplace domain. Since amplitudes of wavefields are very small generally, a power <1 amplifies the wavefields especially at large offset. Therefore, the power objective function can enhance the Laplace-domain inversion results. In previous studies about synthetic datasets, it is confirmed that the inversion using a power objective function shows a similar result when compared with the inversion using a logarithmic objective function. In this paper, we apply an inversion algorithm using a power objective function to field datasets. We perform the waveform inversion using the power objective function and compare the result obtained by the logarithmic objective function. The Gulf of Mexico dataset is used for the comparison. When we use a power objective function in the inversion algorithm, it is important to choose the appropriate exponent. By testing the various exponents, we can select the range of the exponent from 5 × 10~(-3) to 5 × 10~(-8) in the Gulf of Mexico dataset. The results obtained from the power objective function with appropriate exponent are very similar to the results of the logarithmic objective function. Even though we do not get better results than the conventional method, we can confirm the possibility of applying the power objective function for field data. In addition, the power objective function shows good results in spite of little difference in the amplitude of the wavefield. Based on these results, we can expect that the power objective function will produce good results from the data with a small amplitude difference. Also, it can partially be utilized at the sections where the amplitude difference is very small.
机译:除了仅在源点附近,拉普拉斯域中的波场具有非常小的振幅。为了处理此特征,对数目标函数已在许多Laplace域反演研究中使用。使用对数目标函数的拉普拉斯域波形反演比时域或频域反演具有更少的局部最小值。最近,提出了幂目标函数作为拉普拉斯域中对数目标函数的替代方法。由于波场的幅度通常很小,因此功率<1会放大波场,尤其是在较大偏移处。因此,幂目标函数可以增强Laplace域反演结果。在先前关于合成数据集的研究中,可以证实,与使用对数目标函数的反演相比,使用幂目标函数的反演显示出相似的结果。在本文中,我们将使用幂目标函数的反演算法应用于字段数据集。我们使用功率目标函数执行波形求逆,并比较通过对数目标函数获得的结果。墨西哥湾数据集用于比较。当我们在反演算法中使用幂目标函数时,选择合适的指数很重要。通过测试各种指数,我们可以在墨西哥湾数据集中选择从5×10〜(-3)到5×10〜(-8)的指数范围。从具有适当指数的幂目标函数获得的结果与对数目标函数的结果非常相似。即使我们没有得到比常规方法更好的结果,我们也可以确认将幂目标函数应用于现场数据的可能性。此外,功率目标函数显示出良好的结果,尽管波场的幅度差异很小。基于这些结果,我们可以预期,功率目标函数将从振幅差较小的数据中产生良好的结果。同样,它可以部分地用于幅度差很小的部分。

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