利用分布式声学传感和电锤源进行三维近地表 P 波速度结构成像

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摘要

分布式声学传感(DAS)是一种新兴的超密集地震观测技术,为高分辨率次表层地震成像提供了一种新方法。最近,大量线性 DAS 阵列被用于城市地区的二维 S 波近地表成像。为了探索利用 DAS 阵列进行三维(3D)结构成像的可行性,我们在北京国家地球观测站进行了一次主动源实验。我们部署了一条长 1 公里的矩形光缆,光缆被重新铸造成 250 个传感器,通道间距为 4 米。DAS 阵列清晰地记录了锤击源产生的 P 波、S 波和面波。首先用短期平均/长期平均(STA/LTA)法选取首次到达的 P 波行进时间,然后再进行人工检查。DAS 记录的 P 波信号与短周期地震仪水平分量记录的 P 波信号一致。在较短的震源-接收器距离上,DAS 记录的 P 波信号与地震仪垂直分量记录的 P 波信号一致,但在较远的距离上,DAS 记录的 P 波信号明显落后于地震仪垂直分量记录的 P 波信号。这可能是信噪比和入射波的极化共同作用的结果。然后,我们使用 TomoDD 软件反演了最上层 50 米的三维 P 波速度结构,分辨率为 10 米。反演后的 P 波速度结构与之前通过环境噪声层析成像获得的 S 波速度结构非常吻合。我们的研究表明,利用主动源和 DAS 阵列进行三维近地表成像是可行的。然而,在大深度的反演绝对速度值可能存在偏差,这是因为在震源-接收器距离较远时,DAS 记录和地震仪之间可能存在时间偏移。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
3D near-surface P-wave velocity structure imaging with Distributed Acoustic Sensing and electric hammer source

Distributed Acoustic Sensing (DAS) is an emerging technique for ultra-dense seismic observation, which provides a new method for high-resolution sub-surface seismic imaging. Recently a large number of linear DAS arrays have been used for two-dimensional S-wave near-surface imaging in urban areas. In order to explore the feasibility of three-dimensional (3D) structure imaging using a DAS array, we carried out an active source experiment at the Beijing National Earth Observatory. We deployed a 1 ​km optical cable in a rectangular shape, and the optical cable was recast into 250 sensors with a channel spacing of 4 ​m. The DAS array clearly recorded the P, S and surface waves generated by a hammer source. The first-arrival P wave travel times were first picked with a Short-Term Average/Long-Term Average (STA/LTA) method and further manually checked. The P-wave signals recorded by the DAS are consistent with those recorded by the horizontal components of short-period seismometers. At shorter source-receiver distances, the picked P-wave arrivals from the DAS recording are consistent with vertical component recordings of seismometers, but they clearly lag behind the latter at greater distances. This is likely due to a combination of the signal-to-noise ratio and the polarization of the incoming wave. Then, we used the TomoDD software to invert the 3D P-wave velocity structure for the uppermost 50 ​m with a resolution of 10 ​m. The inverted P-wave velocity structures agree well with the S-wave velocity structure previously obtained through ambient noise tomography. Our study indicates the feasibility of 3D near-surface imaging with the active source and DAS array. However, the inverted absolute velocity values at large depths may be biased due to potential time shifts between the DAS recording and seismometer at large source-receiver distances.

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