Abstract

The complexity of coseismic slip distributions influences the tsunami hazard posed by local and, to a certain extent, distant tsunami sources. Large slip concentrated in shallow patches was observed in recent tsunamigenic earthquakes, possibly due to dynamic amplification near the free surface, variable frictional conditions or other factors. We propose a method for incorporating enhanced shallow slip for subduction earthquakes while preventing systematic slip excess at shallow depths over one or more seismic cycles. The method uses the classic k−2 stochastic slip distributions, augmented by shallow slip amplification. It is necessary for deep events with lower slip to occur more often than shallow ones with amplified slip to balance the long-term cumulative slip. We evaluate the impact of this approach on tsunami hazard in the central and eastern Mediterranean Sea adopting a realistic 3D geometry for three subduction zones, by using it to model ~ 150,000 earthquakes with M_{w} from 6.0 to 9.0. We combine earthquake rates, depth-dependent slip distributions, tsunami modeling, and epistemic uncertainty through an ensemble modeling technique. We found that the mean hazard curves obtained with our method show enhanced probabilities for larger inundation heights as compared to the curves derived from depth-independent slip distributions. Our approach is completely general and can be applied to any subduction zone in the world.

Highlights

  • A relatively high rate of great seismic events (MwC 8.0) characterized the last two decades

  • We address the importance of such a model through a long-term seismic—probabilistic tsunami hazard assessment (S-PTHA; hazard for tsunamis generated by earthquakes only)

  • We model tsunamigenic earthquakes in a range from Mw 1⁄4 6:0 to Mw 1⁄4 9:0 subdivided into 18 bins

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Summary

Introduction

A relatively high rate of great seismic events (MwC 8.0) characterized the last two decades Most of these events occurred along subduction zones and triggered some of the strongest ever-recorded tsunamis (e.g., 2004 Mw 9:2 Sumatra–Andaman, 2010 Mw 8:8 Maule, and 2011 Mw 9.1 Tohoku). Some of these great earthquakes revealed unprecedented rupture features, for example the Tohoku earthquake that produced an unexpectedly large amount of slip (* 50 m) just at the trench, resulting in a huge tsunami (e.g., Romano et al 2014; Lorito et al 2016; Lay 2018) Before this earthquake, it was commonly stated that the accretionary sedimentary wedges could not accumulate sufficient strain to produce a large co-seismic slip (e.g., Hyndman et al 1997; Moore and Saffer 2001). Some numerically simulated dynamic effects may favor the up-

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