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首页> 外文期刊>Earth and Planetary Science Letters: A Letter Journal Devoted to the Development in Time of the Earth and Planetary System >Source locations of teleseismic P, SV, and SH waves observed in microseisms recorded by a large aperture seismic array in China
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Source locations of teleseismic P, SV, and SH waves observed in microseisms recorded by a large aperture seismic array in China

机译:中国大口径地震台阵记录的微震中观测到的远震P,SV和SH波的震源位置

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Transversely polarized seismic waves are routinely observed in ambient seismic energy across a wide range of periods, however their origin is poorly understood because the corresponding source regions are either undefined or weakly constrained, and nearly all models of microseism generation incorporate a vertically oriented single force as the excitation mechanism. To better understand the origin of transversely polarized energy in the ambient seismic wavefield we make the first systematic attempt to locate the source regions of teleseismic SH waves observed in microseismic (2.5-20 s) noise. We focus on body waves instead of surface waves because the source regions can be constrained in both azimuth and distance using conventional array techniques. To locate microseismic sources of SH waves (as well as SV and P waves) we continuously backproject the vertical, radial, and transverse components of the ambient seismic wavefield recorded by a large-aperture array deployed in China during 2013-2014. As expected, persistent P wave sources are observed in the North Atlantic, North Pacific, and Indian Oceans, mainly at periods of 2.5-10 s, in regions with the strong ocean wave interactions needed to produce secondary microseisms. SV waves are commonly observed to originate from locations indistinguishable from the P wave sources, but with smaller signal-to-noise ratios. We also observe SH waves with about half or less the signal-to-noise ratio of SV waves. SH source regions are definitively located in deep water portions of the Pacific, away from the sloping continental shelves that are thought to be important for the generation of microseismic Love waves, but nearby regions that routinely generate teleseismic P waves. The excitation mechanism for the observed SH waves may therefore be related to the interaction of P waves with small-wavelength bathymetric features, such as seamounts and basins, through some sort of scattering process. (C) 2016 Elsevier B.V. All rights reserved.
机译:通常在很宽的周期内在环境地震能量中观察到横向极化的地震波,但是由于相应的震源区不确定或受弱约束,并且几乎所有的微震模型都包含垂直定向的单力,因此对它们的起源了解甚少。激励机制。为了更好地了解环境地震波场中横向极化能量的起源,我们进行了首次系统的尝试,以定位在微地震(2.5-20 s)噪声中观测到的远震SH波的源区域。我们专注于体波而不是表面波,因为使用常规阵列技术可以将源区域的方位角和距离限制在一定范围内。为了定位SH波(以及SV波和P波)的微震源,我们连续反投影了2013-2014年在中国部署的大口径阵列记录的环境地震波场的垂直,径向和横向分量。正如预期的那样,在北大西洋,北太平洋和印度洋,主要是在2.5-10 s的时间段内,在产生二次微地震所需的强海浪相互作用的区域中观察到了持久性P波源。通常观察到SV波起源于与P波源无法区分的位置,但信噪比较小。我们还观察到SH波的信噪比约为SV波的一半或更少。 SH震源区确定地位于太平洋深水区,远离倾斜的大陆架,大陆架对产生微震Love波很重要,但附近地区通常会产生远震P波。因此,通过某种散射过程,观测到的SH波的激发机制可能与P波与小波长测深特征(例如海山和盆地)的相互作用有关。 (C)2016 Elsevier B.V.保留所有权利。

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