阴影中的地震:为什么余震发生在令人惊讶的地方

J. Hardebeck, R. Harris
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引用次数: 5

摘要

几十年来,关于触发余震的动态应力与静态应力的相对影响一直存在争论。根据静态库仑应力变化假设,在静态库仑应力减小的应力阴影区不应发生余震。我们发现,静态应力阴影对三次M≥7级加利福尼亚主震后的余震发生有很大影响。在模拟的静态库仑应力阴影区内,余震率比模拟的增加区低一个数量级。然而,应力阴影中的地震率并不像库仑应力变化模型预测的那样低于背景率。应力阴影区的余震与应力增加区的余震表现出不同的时空特征。应力阴影中的余震率随与主震的距离呈幂律衰减,与动态应力触发的简单模型一致。这些余震开始于主震后最初几天的活动爆发,也符合动态应力触发。我们的解释是,余震序列是静态和动态应力触发的综合结果,估计有34%的余震是由动态触发引起的,而66%的余震是由静态触发引起的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Earthquakes in the Shadows: Why Aftershocks Occur at Surprising Locations
For decades there has been a debate about the relative effects of dynamic versus static stress triggering of aftershocks. According to the static Coulomb stress change hypothesis, aftershocks should not occur in stress shadows—regions where static Coulomb stress has been reduced. We show that static stress shadows substantially influence aftershock occurrence following three M ≥ 7 California mainshocks. Within the modeled static Coulomb stress shadows, the aftershock rate is an order of magnitude lower than in the modeled increase regions. However, the earthquake rate in the stress shadows does not decrease below the background rate, as predicted by Coulomb stress change models. Aftershocks in the stress shadows exhibit different spatial–temporal characteristics from aftershocks in the stress increase regions. The aftershock rate in the stress shadows decays as a power law with distance from the mainshock, consistent with a simple model of dynamic stress triggering. These aftershocks begin with a burst of activity during the first few days after the mainshock, also consistent with dynamic stress triggering. Our interpretation is that aftershock sequences are the combined result of static and dynamic stress triggering, with an estimated ∼34% of aftershocks due to dynamic triggering and ∼66% due to static triggering.
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