<p>Foreshocks are sometimes observed before earthquakes<sup><CitationRef AdditionalCitationIDS="CR2 CR3 CR4 CR5 CR6 CR7 CR8 CR9 CR10 CR11 CR12" CitationID="CR1">1</CitationRef>–<CitationRef CitationID="CR13">13</CitationRef></sup>, yet their role in controlling rupture nucleation remains unclear<sup><CitationRef CitationID="CR1">1</CitationRef>,<CitationRef CitationID="CR11">11</CitationRef>,<CitationRef CitationID="CR14">14</CitationRef></sup>. Classical models often assume that nucleation arises from slow, quasi-static slip governed primarily by fault weakening<sup><CitationRef AdditionalCitationIDS="CR16 CR17 CR18 CR19 CR20" CitationID="CR15">15</CitationRef>–<CitationRef CitationID="CR21">21</CitationRef></sup>, typically neglecting impulsive precursory events. Here we show, using laboratory experiments and a rate-and-state-based Griffith-like rupture framework<sup><CitationRef CitationID="CR22">22</CitationRef></sup>, that foreshocks, when they occur at the onset of or during nucleation, can fundamentally regulate earthquake initiation. We find that the slip burst induced by foreshocks imparts a transient sliding velocity, <i>V</i><sub>min</sub>, whose magnitude is set by foreshock size and which robustly predicts both nucleation duration and spatial length. Larger foreshocks generate higher <i>V</i><sub>min</sub> and trigger a more rapid transition to dynamic rupture, whereas smaller foreshocks produce long-duration quasi-static growth and very small impulses lead to ruptures entirely arresting. Extending our theoretical framework to tectonic faults, we show that foreshock and associated slow-slip sequences preceding natural earthquakes seem to follow the same scaling. These observations allow us to constrain realistic characteristic nucleation slip distances of 0.3–3.0 mm, orders of magnitude smaller than those inferred for dynamic rupture<sup><CitationRef CitationID="CR23">23</CitationRef></sup>. Our results demonstrate that foreshock-induced transients set the timing and potential detectability of earthquake nucleation<sup><CitationRef CitationID="CR24">24</CitationRef></sup>.</p>

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Foreshock-induced slip transients set mainshock nucleation timing

  • Barnaby Fryer,
  • Dmitry Garagash,
  • Mathias Lebihain,
  • François Passelègue

摘要

Foreshocks are sometimes observed before earthquakes113, yet their role in controlling rupture nucleation remains unclear1,11,14. Classical models often assume that nucleation arises from slow, quasi-static slip governed primarily by fault weakening1521, typically neglecting impulsive precursory events. Here we show, using laboratory experiments and a rate-and-state-based Griffith-like rupture framework22, that foreshocks, when they occur at the onset of or during nucleation, can fundamentally regulate earthquake initiation. We find that the slip burst induced by foreshocks imparts a transient sliding velocity, Vmin, whose magnitude is set by foreshock size and which robustly predicts both nucleation duration and spatial length. Larger foreshocks generate higher Vmin and trigger a more rapid transition to dynamic rupture, whereas smaller foreshocks produce long-duration quasi-static growth and very small impulses lead to ruptures entirely arresting. Extending our theoretical framework to tectonic faults, we show that foreshock and associated slow-slip sequences preceding natural earthquakes seem to follow the same scaling. These observations allow us to constrain realistic characteristic nucleation slip distances of 0.3–3.0 mm, orders of magnitude smaller than those inferred for dynamic rupture23. Our results demonstrate that foreshock-induced transients set the timing and potential detectability of earthquake nucleation24.