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Seismicity rate immediately before and after main shock rupture from high-frequency waveforms in Japan

机译:在日本,由高频波形引起的主震破裂前后的地震发生率

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We analyze seismicity rate immediately before and after 82 main shocks with the magnitudes ranging from 3 to 5 using waveforms recorded by the Hi-net borehole array in Japan. By scrutinizing high-frequency signals, we detect ~5 times as many aftershocks in the first 200 s as in the Japan Meteorological Agency catalogue. After correcting for the changing completeness level immediately after the main shock, the aftershock rate shows a crossover from a slower decay with an Omori's law exponent p = 0.58 ± 0.08 between 20 and 900 s after the main shock to a faster decay with p = 0.92 ± 0.04 after 900 s. The foreshock seismicity rate follows an inverse Omori's law with p = 0.73 ± 0.08 from several tens of days up to several hundred seconds before the main shock. The seismicity rate in the 200 s immediately before the main shock appears steady with p = 0.35 ± 0.50. These observations can be explained by the epidemic-type aftershock sequence (ETAS) model, and the rate-and-state model for a heterogeneous stress field on the main shock rupture plane. Alternatively, nonseismic stress changes near the source region, such as episodic aseismic slip, or pore fluid pressure fluctuations, may be invoked to explain the observation of small p values immediately before and after the main shock.
机译:我们使用日本Hi-net钻孔阵列记录的波形分析了82次主震前后的地震活动率,震级范围为3至5。通过检查高频信号,我们发现在200 s之内余震的数量是日本气象厅目录中的〜5倍。在校正了主震后立即变化的完整性水平后,余震速率显示出从主震后20到900 s内,以大森定律指数p = 0.58±0.08的较慢衰减到p = 0.92的较快衰减的过渡。 900 s后为±0.04。前震的地震活动率在大震前的几十天到几百秒内遵循大森逆定律,p = 0.73±0.08。紧接主震之前200 s内的地震活动率稳定,p = 0.35±0.50。这些观察结果可以通过流行型余震序列(ETAS)模型以及主震破裂面上非均质应力场的速率和状态模型来解释。或者,可以调用震源区附近的非地震应力变化,例如偶发性地震滑动或孔隙流体压力波动,以解释在主震之前和之后立即观察到的小p值。

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