用宽带强震记录估计俯冲带重复地震震源模型的比较

Masaharu Takiguchi, K. Asano, T. Iwata
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引用次数: 22

摘要

在太平洋板块俯冲到北美板块之下的茨城根-崎地区,每隔21年左右就会发生重复的M7级俯冲带地震。利用宽带强震记录估计了两次M7级茨城根树地震的震源破裂过程,并进行了对比,探讨了重复俯冲带地震的震源特征。首先,利用经验格林函数方法,通过强震模拟正演模拟,估计了2008年5月8日(2008MS) MJ 7.0级地震的震源模型。在广阔的区域模拟了强烈的地面运动。频段频率范围(0.3 ~ 10hz)。假设一个矩形强运动生成区域(SMGA)。在距震源150公里范围内测得的合成波形较好地再现了观测波形。然后,我们估计了1982年7月23日(1982MS)发生的另一次MJ7.0级地震的震源模式。我们比较了1982年和2008年在同一台站和同一地点观测到的波形。在1982年ms的初始破裂阶段。我们假设在1982年ms震源之外有一个单一的矩形SMGA。SMGA位于震源以西约33 km处,在震源时间11s后破裂;该地点位于2008年ms震源向北仅7公里处,因此位于其SMGA内。分析了1982MS与2008MS强震记录的频谱比,估计了1982MS的SMGA的大小、应力降和滑移量。估计尺寸与2008MS相同,但应力降和滑移量约为2008MS的1.5倍。当我们假设破裂传播特征与2008MS相同时,合成波形可以很好地再现观察到的波形。该模拟不具备SMGA位置变化数公里的分辨率。我们的结果表明,两个SMGAs可能重叠。它们的尺寸相同,但应力降和滑移量不同。震源位置和初始破裂过程也不同。这些结果显示了该地区发生的重复地震的多样性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Comparison of Source Models of Repeating Subduction-zone Earthquakes Estimated Using Broadband Strong Motion Records
At the Ibaraki-ken-oki region where the Paci.c plate subducts beneath the North American plate, repeating M7 class subduction-zone earthquakes have occurred with an interval of approximately 21 years. We estimated the source rupture processes of two M7 Ibaraki-ken-oki earthquakes from broadband strong motion records and compared them to investigate the source characteristics of repeating subduction-zone earthquakes. First, the source model of MJ 7.0 earthquake occurring on May 8, 2008 (2008MS) was estimated by the forward modeling through strong motion simulations using the empirical Green’s function method. Strong ground motions were simulated in the broad.band frequency range (0.3-10 Hz). A single rectangular Strong Motion Generation Area (SMGA) was assumed. The synthetic waveforms at stations within 150 km from the hypocenter reproduced the observed ones well. Then, we estimated the source model of another MJ7.0 earthquake occurring on July 23, 1982 (1982MS). We compared the observed waveforms of the 1982MS and the 2008MS at the same stations and identi.ed the initial rupture phase for the 1982MS. We assumed a single rectangular SMGA away from the hypocenter of the 1982MS. The SMGA was located about 33 km westward from the hypocenter and ruptured about 11s after the origin time; this location was just 7 km northward to the 2008MS hypocenter and so inside its SMGA. We analyzed the spectral ratio of the strong motion records of the 1982MS to the 2008MS and estimated the size, stress drop, and slip amount of the SMGA of the 1982MS. The estimated size was the same as that of the 2008MS, but the stress drop and slip amount were approximately 1.5 times larger. Synthetic waveforms reproduced the observed ones well when we assumed the rupture propagation characteristics were the same as that of the 2008MS. This simulation did not have the resolution to several kilometers’change of the location of the SMGA. Our results indicate that the two SMGAs may overlap. They were the same size, but had different stress drops and slip amounts. The hypocentral locations and initial rupture processes were also different. These results show the variety of the repeating earthquakes occurring in this region.
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