Project Abstract
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Mechanistic studies of short-term earthquake interactions have taken two separate tracks. One is to study farfield triggering (Hill et al., 1993; Brodsky et al., 2000; Gomberg et al., 2001; Prejean et al., 2004). The other is to study aftershocks (Stein, 1999; Kilb et al., 2002; Felzer and Brodsky, 2006). The long-range triggering studies have the advantages of cleanly separating out
the stresses and thus having a well-defined triggering stress. The clear role of the dynamic stress is well-illustrated by phase-locked triggering that tracks the surface waves (West et al., 2005). The long-range approach has the disadvantages that the number of triggered events is often too small for statistical study and the phenomenon may not be representative of common processes. Aftershock studies have the advantages that enormous numbers of triggered events have been recorded and it is clear that aftershock generation is a common, major process that occurs throughout the crust. The disadvantage of studying aftershocks is that the nearfield stress field is complex with potentially significant static and dynamic components.
In this project we connect observationally these two types of triggering. We exploit the understanding that dynamic strain is the dominant triggering agent at large distances and relatively short time scales in order to constrain the contribution of additional triggering agents in the near field. We first determine an empirical relationship between a measure of triggering intensity and peak dynamic strain in the far field based on the waiting time to early triggered earthquakes. Then we compare this far‐field relationship to near‐field observations to assess the proportion of near‐field earth- quakes that can be explained by the far‐field proportionality. We ultimately find that dynamic triggering can account for a significant portion of near‐field aftershocks, but that there is an additional triggering component in the near field. Whether this reflects additional triggering agents (e.g., static strain, afterslip) or the effect of second‐order aspects of the dynamic strain (e.g., duration, frequency) we cannot resolve. |