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首页> 外文期刊>Bulletin of the Seismological Society of America >The SPAC Method for a Finite M-Station Circular Array Using Horizontally Polarized Ambient Noise
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The SPAC Method for a Finite M-Station Circular Array Using Horizontally Polarized Ambient Noise

机译:使用水平极化环境噪声的有限M站圆形阵列的SPAC方法

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摘要

The spatial autocorrelation (SPAC) method is a useful tool for interpreting ambient noise, and several theoretical tools based on this method are available for data collection, processing, and analysis. The method uses the three components of seismic microtremors recorded simultaneously with arrays of different configurations and yields dispersion curves of Rayleigh and Love waves. Existing theories of the SPAC method are based on an idealized circular array with an infinite number of stations (the continuous model). Errors due to the use of a finite number of stations have been derived theoretically for vertically polarized ambient noise. This paper presents an extension of that error theory to horizontally polarized ambient noise so that it is valid for a circular array withMuniformly spaced stations. The quantities that are obtained as the output of the SPAC method, however, depend on the ratio of the power spectral densities (PSDs) of Rayleigh and Lovewaves, which are difficult to identify beforehand. Instead we introduce a quantity, κ, that does not depend on the PSD ratio and therefore is more convenient for separating the properties of Rayleigh and Love waves. We derive an expression of κ for a finite, M-station circular array (κ_M) and compare it with what it should be in the continuous model (κ_T).We illustrate κ_M and κ_T using field data from a site in Tehran and discuss their discrepancies. Finally, we demonstrate how we have estimated Love-wave phase velocities using the calculated κ_M.
机译:空间自相关(SPAC)方法是用于解释环境噪声的有用工具,并且基于此方法的几种理论工具可用于数据收集,处理和分析。该方法利用同时记录有不同构造阵列的地震微震的三个分量,得出瑞利波和洛夫波的频散曲线。 SPAC方法的现有理论基于具有无限台数的理想圆形阵列(连续模型)。对于垂直极化的环境噪声,理论上已经得出了由于使用有限数量的站而导致的误差。本文提出了将该误差理论扩展到水平极化的环境噪声的方法,从而使其对于具有均匀间隔站的圆形阵列有效。但是,作为SPAC方法的输出获得的数量取决于瑞利波和洛夫波的功率谱密度(PSD)的比值,这些比值很难事先确定。取而代之的是,我们引入一个不依赖于PSD比率的量κ,因此更便于分离瑞利波和洛夫波的性质。我们导出一个有限的M站圆阵列(κ_M)的κ表达式,并将其与连续模型(κ_T)中的κ表达式进行比较。差异。最后,我们演示了如何使用计算出的κ_M估算Love-wave相速度。

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