Spatial and Temporal Patterns of Deformation Through the Seismic Cycle Jeff Freymueller University of Alaska Fairbanks.

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Presentation transcript:

Spatial and Temporal Patterns of Deformation Through the Seismic Cycle Jeff Freymueller University of Alaska Fairbanks

Outline A very simple earthquake cycle model Some complications we think we understand (sort of) A complication we don’t understand Summary of questions

A Simple “Earthquake Cycle” Model Based on the 1D spring-slider analogue model Two “modes”: interseismic and coseismic Between earthquakes (interseismic): – Shallow fault is locked – Deeper fault is creeping at long-term slip rate – Stress builds up: elastic strain energy stored in crust During earthquake, shallow fault slips – Stress on fault reduced Cycle repeats forever

Deformation At Subduction Zone Horizontal Vertical Trench-normal distance (km) Vertical Backslip model (Savage, 1983) – Shallow part of fault slips only in earthquakes – Deeper part slips steadily at long-term rate – Superposition of steady slip on entire interface and backslip (slip deficit) – Earth deforms as elastic body

Along-Strike Variation Trench relative plate motion

Example: Alaska Peninsula  SW arc translation of 4 mm/yr  Updip limit is poorly constrained by land-based data  But, moment rate deficit is well constrained Subduction strain Measured vel. What is the Arc velocity? Cross and Freymueller (2008)

Some Complications We Think We Understand (sort of) Postseismic deformation – Afterslip (on the plate interface) – Viscoelastic relaxation (in mantle wedge) Along-strike variations – Extent of slip deficit varies along strike: why? Slow slip events – The locked to creeping transition is dynamic Common theme: slip along interface varies with time – not just interseismic + coseismic.

Postseismic Deformation Large and great earthquakes cause postseismic deformation, mostly due to: – Afterslip/focused shear on the plate interface – Viscoelastic relaxation within mantle wedge But variable from earthquake to earthquake Wang et al. (2007)

Q– Why are the amounts of afterslip and viscoelastic relaxation so variable? EarthquakeAfterslipViscoelastic Relaxation 1960 Chile (M9.5)??Large, lasted for decades 1964 Alaska (M9.3)~6 meters (25-30% of coseismic), decades Large, lasted for decades 2004 Sumatra-Andaman (M9.2) Large, lasting > several years 2005 Sumatra (M8.7)Large, both updip and downdip Clearly present in far-field data 1995 Antofagasta (M8.1)Small, gone within ~3 yearsNone? 2007 Kurils (M 8.1)Ended within 0.5 yearLarge, will last ~ decade 1994 Sanriku (M 7.7)Equal to coseismicminimal We have not been successful in making advance predictions of postseismic deformation following large or great earthquakes.

Along-Strike Variations are Nearly Ubiquitous Interseismic contour: Suwa et al. (2006) Coseismic slip patches (Yamanaka and Kikuchi, 2002) NE Japan Hikurangi McCaffrey et al. (2008)

Along-Strike Variations are Nearly Ubiquitous Freymueller et al. (2008) Q– What controls along-strike variations in the extent of slip deficit?

Slow Slip and Downdip Transition The downdip end of the seismogenic zone is particularly dynamic. Slow slip events of various sizes observed in Cascadia, Alaska, Mexico, Japan, Costa Rica, …. – Durations of weeks to a few years Q– What is the relationship of slow slip to the generation of tremor? Q– How do variations in the slip rate affect overall slip budget?

Is Slip Confined to Region of Tremor? Melbourne Similar results from Schmidt and Krogstad Delbridge and Houston Slide from Heidi Houston, UW

A Complication We Don’t Understand Suito and Freymueller (2009) Slow Slip Event

Significant Velocity Change Black: 2004 to present

Significant Velocity Change Black: 2004 to present

Change in Width of Locked Zone Data corrected for 1964 postseismic deformation using Suito and Freymueller [2009]

Interpretations/Speculations A sizable patch on the plate interface that had been creeping abruptly locked? – A long-lived (9+ year) slow slip event came to an end? Pattern of postseismic deformation abruptly changed? Any of these explanations require some kind of “mode switching” behavior – Could the Denali earthquake stress change + ~2 years of postseismic deformation been the trigger?

Accumulated Questions How does deformation across the subduction plate boundary evolve in space and time? Why are the amounts of afterslip and viscoelastic relaxation so variable? What controls along-strike variations in the extent of slip deficit? What is the relationship of slow slip to the generation of tremor? – And how to explain subduction zones with slip but no tremor? How do variations in the slip rate affect overall slip budget? What further dynamics will be observed at the locked to creeping transitions at subduction zones?