The American Geosciences Institute 4220 King Street, Alexandria, VA 22302-1502, U.S.A. 703-379-2480; Fax: 703-379-7563; [email protected] www.earthmagazine.org Superquakes, Supercycles and Global Earthquake Clustering Chris Goldfinger, Yasutaka Ikeda and Robert S. Yeats EARTH Vol. 58 (No. 1), p. 34 REPRODUCTION: More than one photocopy of an item from EARTH may be made provided that fees are paid directly to the Copyright Clearance Center, 222 Rosewood Dr., Danvers, MA 01923, USA. Phone: (978)750-8400. Fax: (978)646-8600. Any other form of reproduction requires special permission from and is subject to fees by EARTH. Information about obtaining reprints of this article or about obtaining permission to reproduce this article in whole or in part can be found by e-mailing [email protected]. EARTH is published monthly for a base subscription rate of $36.00 a year (single copies $5.99) by the American Geosciences Institute. © 2013 American Geosciences Institute. Standard mail, nonprofit postage paid at Denver, Colo., and at other mailing offices. Claims for missing issues will be honored only up to six months. Issues undelivered through failure to notify EARTH of address change will not be replaced. www.earthmagazine.org recent research and recent quakes reveal surprises in major fault systems damage in honshu, Japan, from the 2011 tsunami. Chris Goldfinger, Yasutaka ikeda and robert s. Yeats A number of recent big earthquakes around the world have humbled many earthquake researchers. The March 2011 magnitude-9 superquake off Tohoku, Japan, and the December 2004 magnitude9-plus temblor off Sumatra were both far larger than what scientists expected those fault systems to produce. Based on these quakes, and on recent research that contradicts long-held paradigms, it is becoming clear that the types and sizes of large earthquakes that a given fault system is capable of producing remain poorly known for most major fault systems. 34 EARTH January 2013 www.earthmagazine.org u.s. navy photo by naval Air Crewman 1st Class Jay okonek/released superquakes, supercycles, and global Earthquake clustering Clockwise from top left: Chris Goldfinger; Jay Patton; U.S. Navy photo by Photographer’s Mate 2nd Class Philip A. McDaniel Oregon State University scientists and Indonesian colleagues recover a piston core from the Sunda trench off northern Sumatra on board the Scripps vessel R/V Roger Revelle. Right: The core shows a long history of earthquakes. The problem is that we are relying on short historical records, and even shorter instrumental records. Basing estimations of maximum earthquake size or models of earthquake recurrence on such records or on the behavior of smaller earthquakes does not encompass the full range of fault behavior. We can no longer hold onto the notion that magnitude-9 earthquakes might be likely to occur in some areas, but not in others. So much remains to be learned about great earthquakes There are a few places with long and detailed enough records to examine long-term behavior of major fault systems: Northeastern Japan and Cascadia, off the coast of Oregon, Washington and British Columbia, are two of the beststudied. And thanks to new research techniques, those two areas are offering new lessons and hints at earthquakes to come. theory that plate age and convergence velocity determine maximum earthquake size. And we have tried to apply recurrence rate models, based on the relationships between time before or after an earthquake, to inform us about the next earthquake. But all of these models are built on the short instrumental and sometimes historical records. As we begin to gather more long records from around the world, we are beginning to see more complex behavior. Strain may accumulate at even very slow rates, sometimes in settings previously considered unlikely, eventually to be released in very large earthquakes. Such long-term cycling is suggested for Cascadia, Hokkaido, northeastern Japan, Chile and Sumatra. In the case of northeastern Japan, earthquakes of the past few hundred years had dimmed the memory of the Jogan superquake of A.D. 869, which produced a tsunami that killed about 1,000 people on the Sendai Plain and was probably similar in size to the Tohoku quake. Models were largely based on more recent quakes. In Cascadia, models showing a limited range of expected quake sizes have A village near the coast of Sumatra after the tsunami that struck Southeast Asia the day after Christmas 2004. Earthquakes Reveal Model Shortcomings Scientists have developed detailed conceptual models of quake behavior and recurrence rates. We have the characteristic earthquake model, which suggests that faults have “typical” repeatable ruptures. We also have the seismic gap theory, which suggests we should look to holes in the instrumental record for future events. We have relied on a www.earthmagazine.org EARTH January 2013 35 144° 146° 0 -5 Japan Sea Hok kai do 44° -10 1 1961 Mw 7.0 2 42° 2004 Mw 7.0 2.5 2003 Mw 8.3 1952 Mw8.1 0 -1 1901 Mw 7.5 1989 Mw 7.4 1896 Mw 8.2 1915 Mw 7.5 1978 Mw 7.6 6 1936 Mw 7.1 2011 Mw 9.0 1938 Mw 7.7 1933 Mw 8.4 1897 Mw 7.8 Trench 3 4 Long-term Cycling in the Northeast Japan Trench 82 mm/yr Japan 7 hu 1938 Mw 7.8 Pacific Plate 1938 Mw 7.9 -2.5 Tokyo 5 Sendai 8 36° lT ri u K 1968 Mw 7.8 ch ren 1968 Mw 8.3 Ho ns NF M to Ue ts 40° 1994 Mw 7.7 -5 uf o ld and th rust belt 1931 Mw 7.7 38° 1973 Mw 7.8 140° 142° 144° 146° Map showing recent vertical crustal movements and source areas of large intraplate earthquakes. Blue line contours indicate rates of subsidence in millimeters per year, as revealed by tide gauge observations from 1955 to 1981. Orange lines indicate source areas of subduction earthquakes of magnitude 7 or greater since 1896. The epicenter and source area of the 2011 Tohoku earthquake (magnitude 9) are indicated by a star and orange shading, respectively. 36 EARTH January 2013 been based on excellent but relatively short paleoseismic records onshore. However, recent research on undersea deposits indicates that a wide range of earthquake sizes has occurred there, including quakes larger than previously thought possible and smaller ones limited to southern Cascadia. In Sumatra, models suggest that plate convergence was so oblique that the plates were moving parallel to each other, and that a subduction-type earthquake like the one that occurred in 2004 was unlikely. In general, relationships — such as that between plate age and convergence rate — were appealing but had never really been tested. They were based on dubious physical concepts and the short instrumental record. These modeled relationships were on shaky ground in terms of both statistics and the unknown nature of long-term energy storage and release in subduction zones. Scientists are now working to rewrite these models based on new evidence. There are a couple of ways to look at the seismic hazard in northeastern Japan, near where the Tohoku quake struck. Using the historical record, especially of the most recent earthquakes in the Sendai area — a magnitude 8.4 in 1933, a magnitude 7.1 in 1936, and a magnitude 7.6 in 1978 — most scientists considered the largest likely quake in the region to be about 8.4. Those earlier quakes did not leave widespread tsunami records. More numerous and perhaps better remembered are the smaller events in recent decades and centuries that make up the majority of the historical record; it was these smaller events that drove the underestimation of the seismic and tsunami hazard in northeastern Japan. The historical record can be helpful, however, if you look far enough back in time; and if you include paleoseismic and paleotsunami evidence, the picture changes. The older historical record in the Tohoku region, for example, reveals a number of large earthquakes and www.earthmagazine.org Chris Goldfinger 142° -2.5 140° Clockwise from bottom left: Chris Goldfinger; Chris Goldfinger; Masato yamada; Chris Goldfinger above: chris goldfinger digs a pit on the sendai plain in 2011 after the tohoku quake to sample tsunami deposits. left: tsunami deposits from the a.d. 869 Jogan superquake can be seen in the shallow subsurface on the sendai plain. such deposits help create a more complete record of past quakes. high tide in ishinomaki (shown in June 2011), a coastal town that was affected by the march 2011 tsunami. permanent subsidence put most streets in this neighborhood underwater at high tide. www.earthmagazine.org associated tsunamis, including large events in A.D. 869, 1611 and 1896. The largest of these events was the A.D. 869 Jogan tsunami, based on the presence of tsunami deposits in a coastal lake and across the Sendai and Ishinomaki plains. The landward inundation of the March 2011 tsunami penetrated 3.5 to 4 kilometers inland on the Sendai Plain, similar to the Jogan tsunami (although at the time of the Jogan event, the shoreline was approximately 1 kilometer inland of where it presently is). The paleotsunami evidence also includes two predecessors to the Jogan event, which also penetrated approximately 4 kilometers inland. That evidence supports the existence of “outsized” events — those about magnitude 9 or so — along the Tohoku coast with recurrence times in the range of 800 to 1,200 years. Looking at both long-term geology and new instrument-based research also provides a new view of the seismic hazard in this region. For at least the past 5 million years, the Japan arc has been subjected to east-west compression due to convergence of the Pacific Plate at a rate of 80 millimeters per year. Investigating the structural geology of northeastern Japan reveals that a foldand-thrust belt permanently relieves an unsecured petroleum storage tank swept across ishinomaki Bay by the march 2011 tsunami. some of this compression, but only at a rate of about approximately 3 to 5 millimeters per year. Including other active faults and folds, the total rate of permanent horizontal shortening over the Northeast Japan arc is about 5 to 7 millimeters per year. Permanent uplift of northeastern Japan occurs at a rate that is in agreement with the permanent shortening. This indicates that less than 10 percent of plate convergence is accommodated in the Japan arc as permanent deformation. In the short term, however, triangulation, trilateration and GPS observations show that the Japan arc has been shortening at a rate as high as several tens of millimeters per year over the last century, much higher than geological rates. At the same time, abnormally high rates (up to 10 millimeters per year) of subsidence along the coast have been observed by tide gauges during the last 80 years or so. Despite the fact that marine terraces along the Pacific coast of northeastern Japan show permanent uplift, the best explanation is that in the short term, it is being dragged downward by the subducting Pacific Plate. The difference between short-term and long-term deformation rates indicates that most of the plate convergence is not deforming northeastern Japan. Instead, that energy is elastic and is being stored in the way that a spring stores energy. Eventually, this energy must be released by slip on the subducting plate EARTH January 2013 37 the 2011 tsunami swept up this canyon to more than 60 meters above sea level. the canyon leads to one of the hundreds of “tsunami stones” (right), some more than 600 years old, that are found along the coast of Japan. the inscription on this stone, near the village of aneyoshi, warns against building houses in areas lower than where the stone is set and describes destruction caused by past tsunamis. boundary as giant earthquakes. Yet in recent times, earthquakes with magnitudes of only 7 to 8.4 have occurred in the same region, and did not result in the release of very much of the accumulated energy. To release the excess energy and balance plate motion, much larger earthquakes must occur. Thus, the Tohoku magnitude-9 earthquake should not have been unexpected with longer-term information taken into consideration. Nonetheless, very few geologists accurately forecasted the size of the Tohoku earthquake. 38 EARTH January 2013 In Hokkaido, north of Sendai, a similar relationship has been observed between the shorter historical and instrumental records and the paleoseismic record along the Kuril Trench. Prehistoric tsunamis that most likely were generated from long ruptures along the Kuril Trench were significantly larger than those existing in the historical and instrumental records. Over the past 2,000 to 7,000 years, such outsized events occurred on average about every 500 years, with the most recent event approximately 350 years ago. The best-known large earthquake along the Cascadia Subduction Zone occurred in 1700. The magnitude of the earthquake is estimated to be approximately 9, based on the arrival of an “orphan tsunami” — meaning there is a tsunami record without a corresponding local earthquake — along the Japanese coast. The perception of Cascadia quickly underwent a paradigm shift, from a place thought to host no earthquakes at all to a region capable of great earthquakes, based largely on this quake. More recently, the view of Cascadia’s hazard has been changing again due to new paleoseismic work. Because there haven’t been any large quakes along Cascadia in recent history, the entire earthquake record is based on several decades of paleoseismic work. New evidence from onshore subsidence and tsunami deposits and offshore turbidites (submarine slope failure records) has yielded an unprecedented record of great earthquakes along the Cascadia Subduction Zone. The offshore records www.earthmagazine.org Bottom: Chris Goldfinger; top: kyodo via Ap Images palEosEisMic rEcord in cascadia suBduction ZonE scientists can use turbidites (submarine slope failure deposits) collected from the ocean floor to understand past earthquakes. turbidites provide clues to the timing and magnitude of past events. the authors have collected turbidites from 6,000 meters below the sea surface off the coast of sumatra and 3,000 meters deep in the cascadia subduction Zone in the pacific northwest. Large earthquakes trigger underwater landslides. Density currents flow into deep water and settle to form turbidite deposits. Repeated layers of turbidites under the seafloor record past earthquake events. are in good agreement with onshore paleoseismology evidence, and both offer consistent information about the relative size of paleoearthquakes, lending confidence that both are recording the same phenomena. The longest records available, those from deep-sea turbidites, reveal information about much longer-term behavior of this subduction zone going back 10,000 years. In 1999, we started looking at turbidite deposits along the Cascadia margin to see what they could tell us about ancient earthquakes. Canadian geologist John Adams had proposed in 1990 that turbidite deposits first discovered along the Ca e ver I sla nd ne Zo WASHINGTON Juan eF u aR id g CANADA Van cou n tio uc bd Su ia ad sc Fra S ctu ov re anc Zo o ne Cascadia margin in the 1960s reliably recorded 13 past great earthquakes. We thought otherwise, and collected numerous cores from Canada to Northern California to test the idea. It turned out that we were wrong, and a decade of work and three coring cruises have led to a detailed earthquake record along the 1,000-kilometer length of Cascadia. We now have a 10,000-year integrated onshore-offshore earthquake record in Cascadia, including 41 probable earthquakes. This long record allows us to c d OREGON Both: kathleen Cantner, AGI Pacific Plate North American Plate Juan de Fuca Plate mantle upwelling subducting plate hydrous melting zone theThe historic seismic record from the from cascadia is no longer limited to instrumental earthquake data (blue historic seismic record thesubduction CascadiaZone subduction zone is no longer limited to instrudots). it has been extended by the association of mega earthquakes with turbidite deposits identified in offshore sediment mental earthquake data (blue dots). It has been extended by the association of mega earthcores (orange dots). quakes with turbidite deposits identified in off-shore sediment cores (orange dots). www.earthmagazine.org EARTH January 2013 39 Dates T12 Dates H 6440 turbidite slanted (6280-6570) T13 T14 T13 H 5810 (5680-5960) T11 H 6440 H (6280-6570) T12 T14 H H 7120 (6990-7250) H T15 7610 (7500-7710) 8050 (7900-8200) T15 7610 T13 (7500-7710) H 6.0 8050 T14 coring (7900-8200) artifact T15 coring artifact T12? H 6.0 T13 7150 (7030-7270) T15 Density Magnetics 5.0 H T17 9330 (9230-9410) H 9530 (9340-9770) H T17a T18 H 7150 (7030-7270) H H 6.0 T15 7.0 T16 H T17 H 10040 (9960-10180) H 9340 (9260-9410) T18 9650 (9460-9860) ge BasinforWest the age. Silt Hemipelagic clay Very fine sand Turbidite silty mud range Channel Rogue Oldest Mazama ash bearing turbidite -128 (5870-6120) Radiocarbon Gamma Density (g/cm T11 3)sample location 5920 (5790-6050) Core break T12 Shell Wood fragment H 4.0 6900 High-resolution point mag. susc (SI) T12a (6780-7030) H 6.0 H 7940 H H T18 46 6590 JUAN DE FUCA PLATE (8 (8150-8350) 42 5.0 T16 8850 (8660-8990) T16a 9070 (8910-9230) T17 8400 (8260-8550) H H 10040 (9960-10180) 9150 (8990-9260) H H 7.0 9340 (9260-9410) 9190 (9070-9300) H T16a 9650 (9460-9860) - 122 H - 124 T17 T18 S Astoria Canyon Hydrate Ridge Basin West core site Burrows Wood fragment 7100 (7090-7260) 22/23 PC 44 7670 (7530-7820) 9830 (9640-9990) Cascadia Channel core site 56 PC - Rogue Channel core site 30/31 PC 42 GORDA PLATE Hydrate Ridge Basin West Eel Canyon 40 OREGON Rogue Canyon Smith Canyon Klamath Canyon Trinidad Canyon Mendocino Channel Noyo www.earthmagazine.org 40 T17a Vancouver Island OCEAN Quinault Canyon Grays Canyon WASHINGTON Willapa Canyon (8 (8 9830 (9640-9990) T18 A RNI 9650 11/12 PC T15 T15a (6440-6750) Mottled clay Above: Correlation of four Cascadia turbidite cores spanT14a (7800-8080) ning 550 kilometers of the Cascadia margin. Every spike with8150 a T and T15 a number shows an earthquake. H individual 8250 (7940-8360) Earthquakes T11-T18 (dates shown above,(8150-8350) with possible 8650 T15a 8460 (8470-8820) ranges based on (8270-8600) different dating 5.0techniques in parentheses) are shown to illustrate the two extreme earthquakes in this record, T11 and T16, which happened roughly T16 years ago, respectively, and are 5,900 and 8,900 both esti8400 8850 H (8260-8550) mated to have been about magnitude 9.1. Dark blue areas (8660-8990) 10040 T16a 9070 light blues show the density of show magnetic properties; (9960-10180) (8910-9230) the sediment. Magnetic and density spikes indicate more 9150 T17 dense sandy material in the turbidites, which correlates to 9340 (8990-9260) H (9260-9410) earthquakes. Right: The location map shows the four cores 9190 shown in large yellow-bordered symbols, with other cores T17a (9070-9300) H as gray and white dots. 40 EARTH January 2013 (9460-9860) H 8460 (8270-8600) SAF H T14 Juan de Fuca Channel core site Shell 3 7670 8150 (7530-7820) (7940-8360) 8650 (8470-8820) 8250 H T14 T14a44(7 IFO H 7.0 T15 T15a H T13 CAL H 7220Gamma Density (g/cm ) (7140-7310) T13 7650 (7480-7820) H Barclay Canyon Juan de Fuca Canyon Very fine sand Sand 7100 (7090-7260) PACIFIC Mottled clay High-resolution point mag. ash susc (SI) Burrows Oldest Mazama bearing turbidite H H -126 48 Density MagneticsPurple ages indicate erosion correction applied. Magnetics Sand Radiocarbon sample location Event Dates Dates Blue ages indicate age from benthic species. Silt Dates Coreages breakindicates reversed age. Gray 6000 7650 (7480-7820) 6.0 T13 T18 -130 T12 6590 7220 (6440-6750) (7140-7310) 4.0 6900 T12a (6780-7030) T17a H 48 46 H T17a T18 T11 T12a (6 H T17 7.0 Explanation Turbidite silty mud Purple ages indicate erosion correction applied. 7290 (7220-7380) Blue ages indicate age from benthic species. Radiocarbon ageage. and the error Gray ages indicates reversed Dates T16 T17a T17a Hemipelagic clay Radiocarbon age and the error range for the age. H T17 9900 (9680-9980) H Explanation T16 7.0 T18 7290 (7220-7380) H T14? 8150 (7940-8360) 8650 (8470-8820) H 5920 Magnetics (5790-6050) Density 7650 T15 T14 7940 (7480-7820) T14a (7800-8080) T14? H Dates T11 5920 (5790-6050) T13 T12 7220 (7140-7310) H 9330 T17 (9230-9410) 9530 T17a (9340-9770) 9900 (9680-9980) H T18 8990 T16 (8860-9140) 8990 (8860-9140) Event -13 6000 (5870-6120) T16 T17a 5.0 DatesT12? Event 6530 (6400-6700) H 6530 (6400-6700) T14 Dates Rogue H Channel T11 H T16 H T17 T12 Event T11 7120 (6990-7250) Magnetics 5.0 Hydrate Ridge Basin West Dates T13 H T16 Magnetics H Density Event (5 in core T11 T12 T11 5.0 Dates 5.0 Cascadia Channel 5810 Density Event (5680-5960) Magnetics Chris Goldfinger H Magnetics Density Density turbidite slanted in core Juan T11de Fuca Channel Event Event ICAN PLATE Magnetics NORTH AMER Density Astoria Asto Ast As A sto sst to to orriiaa C Channel haan nne nn n neeell n Event research on the cascadia subduction Zone has caused scientists to raise the earthquake hazard assessment for cities along the zone, like seattle, wash., (above) and portland, ore. (right). Cascadia Supercycles Potential Energy Gain (Plate Motion) 10500 10000 9500 9000 8500 8000 7500 7000 6500 6000 5500 5000 4500 4000 3500 3000 2500 2000 1500 1000 Time (years before present) 500 0 Kinetic energy loss (Earthquakes) From bottom: Chris Goldfinger; ©istockphoto.com/David Birkbeck; ©istockphoto.com/Mark Hatfield energy cycles along the cascadia margin, based on 10,000 years of earthquakes: the sawtooth pattern represents the storage of energy from plate motion (upticks) and energy loss from earthquakes (downticks). the complexity of this pattern suggests that simple models based on the most recent events underestimate earthquake potential, as occurred in tohoku. look more deeply into how this great fault behaves over long periods of time. One thing that is obvious is that the turbidites show an apparent clustering of great earthquakes into groups of four to five events, with 700- to 1,000-year gaps between the clusters. The turbidites also provide clues to the magnitudes of past events, and to the buildup and release of energy over time. In the turbidite record, the benchmark 1700 earthquake is roughly average relative to 19 similar ruptures, in terms of turbidite thickness and mass over the past 10,000 years. About a half dozen turbidites are larger than the 1700 event and a half dozen smaller; the rest are similar. Two obviously larger events are the 11th and 16th events back in time, at about 5,960 and 8,810 years ago. These turbidites are consistently two to five times larger than “average” turbidites at all core sites along the length of Cascadia, and may have been triggered by a magnitude-9.1 quake, which is 44 percent larger than a magnitude-9 quake. Our research shows that, despite the obvious simplifications involved, a www.earthmagazine.org connection between turbidite mass and energy release of the source earthquakes can be made because of consistency in the turbidite records along the length of the margin at multiple sites and multiple depositional environments. We also found a good correlation between turbidite size and tsunami size at Bradley Lake along the southern Oregon coast, where an excellent 4,600-year tsunami record is found. This suggests that when paleoseismic records are long enough and of sufficient quality, we may be able to tease out more information about past earthquakes than just their timing. We have also done further research on long-term patterns, looking at the energy balance between the Juan de Fuca and North American plates in Cascadia. Because the turbidite size is so consistent among sites, the size of the turbidites can be used as a crude measure of energy release and balanced against the energy gain from plate motion. Plotting the energy gain against energy loss, it is possible to generate a 10,000-year energy time series for Cascadia, showing how energy is stored and released by the fault over time. What this plot and a similar one created for the Sumatran subduction zone show is that not only are earthquakes clustered in time, but there appears to be a long-term cycle of energy storage and release. The resulting sawtooth pattern reveals what we interpret as long-term energy cycling on the subduction zone, with some events releasing less energy and others releasing more energy than is generated from plate convergence alone. Earthquakes that are larger than the energy available from plate convergence may have “borrowed” stored energy from previous cycles; at other times, energy is stored when less energy is released than is available. The plots also show that when a fault is in a high- or low-energy state, its behavior can vary. For example, when Cascadia (and perhaps other faults) is at a high-energy state, it appears equally likely to rupture in single very large (maybe magnitude-9.1) earthquake or in a series of somewhat smaller (but still giant) magnitude-8.8 to -9 earthquakes to relieve stress. When at a very lowenergy state, Cascadia may go for long periods without any quakes, or it may EARTH January 2013 41 othEr proBlEMs With short oBsErvation tiMEs the university of washington’s r/v thomas g. thompson leaving the dock in seattle, as researchers head out to study the cascadia subduction Zone. shake in a series of earthquakes that only release a little of the accumulated energy over time — something that also clearly occurred for the 1,000 years prior to the 2011 Tohoku earthquake. The plots also suggest that the size of an earthquake is not that closely related to the time since the last earthquake. Think of a battery as representing the energy storage of a plate boundary: You can draw energy from it in any increment available at any time, limited only by the total energy available. What this means for Cascadia and other subduction zones is that we cannot say very much about the next earthquake based on the few most recent ones. Long paleoseismic records help get around this problem. Turbidites from deep water in subduction zones and from lakes offer ways to build these long records. They have the advantage of being able to link the records between sites with physical stratigraphy and extend them further back in time. 42 EARTH January 2013 Where long paleoseismic records aren’t available, or in addition to paleoseismic evidence, scientists are frequently turning to geodetic data — data from GPS, strain gauges and tide gauges — to inform assessments of seismic hazards based on how the land is deforming in real time. We now have a wealth of geodetic data that directly provides strain accumulation and slip rates on faults. These geodetic rates are commonly thought to be the best available data. In some cases, geodetic rates over the last few years agree with long-term rates determined from geology, such as slip rates on faults and uplift rates of mountains; at other times, geodetic rates undershoot or overshoot these geologic rates. The reasons for the differences are not always clear, but given the examples of very long-term cycling of earthquake energy release, it’s likely that one cause for the discrepancy in rates is linked to the short time frame of the observations. Not only are the geodetic observations made at random times in the seismic cycle of nearby faults, they may well also be at random times in a long-term multievent “supercycle,” making the data less directly linked to average plate and fault block motions, and more difficult to interpret in terms of size and rates of future earthquakes. With short records, almost every significant earthquake is “new” to geologists. The magnitude-7.7 quake last October in the Queen Charlotte Islands off British Columbia was a thrust earthquake, a type not seen previously on that strike-slip fault, and the magnitude-8.6 strike-slip quake off the coast of Sumatra last April was the largest of its type ever recorded. Another issue with short observation periods is the question of global clustering. Many people have noted that we have had a lot of really large earthquakes lately. Tohoku in 2011, Chile in 2010, Sumatra in 2004. Before that, there is a gap of 50 years following the 1964 Alaskan earthquake, with several other giants clustered between 1957 and 1964. These great earthquakes are clearly clustered in time, but is this just a random phenomenon, or does it mean something about global plate dynamics? A couple of recent studies suggest global clustering of magnitude-9 earthquakes doesn’t exist, and can easily be explained as part of a random process. The problem, though, is that because the recurrence times of magnitude-9 earthquakes can be hundreds of years, and for the largest events can be 5,000 to 6,000 years, we mostly don’t have enough data to actually test this idea either way. Absent enough magnitude-9 events, www.earthmagazine.org Both: Chris Aikenhead the oregon state university coring team examines the upper section of a turbidite core recovered off the sumatran margin. recent surprising earthquakes in Japan, sumatra and the Queen charlotte islands (circles), as well as new research along the cascadia subduction Zone (triangle), indicate that most any fault zone could rupture significantly. locations that have previously experienced “superquakes” are shown in orange. locations that researchers are starting to think could potentially experience magnitude-9 quakes are shown in red. smaller earthquakes with higher frequencies from other fault systems are used as proxies, but the comparison is dubious at best. The observation that magnitude-9 events worldwide have clustered twice in the last 100 years is also questionable because no mechanism to produce such clusters is known (of course, observations virtually always exist before explanations are found). It’s likely that this question will remain open for the foreseeable future, until we have long records from enough subduction zones to examine whether this phenomenon really exists, and if so, what it might mean and what mechanism could explain it. kathleen Cantner, AGI thE nEXt Big onE So, where will the next big one be? That’s impossible to say. But the recent surprises from Tohoku and Sumatra, coupled with new evidence of long-term seismic supercycles on faults like Cascadia and Sumatra, imply that other subduction zones and other major fault systems may be capable of massive quakes. www.earthmagazine.org Based on older models, relatively old subduction plate systems have been ignored as potential producers of magnitude-9 earthquakes, but recent quakes show these zones are indeed at risk. Such areas include much of the west coast of South America, the remainder of the Japan Trench, the Himalayan Front, the Kuril Islands and the western Aleutians in the North Pacific, Java, Indonesia, in the South Pacific, the Antilles Islands in the Caribbean, the Makran coastal area in Iran and Pakistan, and the Manila, Sulu, Philippine and Hikurangi trenches, among many others. Finally, the underlying cause of supercycles is unclear. They could be generated by intrinsic properties of the plate boundaries, cycling of energy among segments of an individual fault, transfer of energy between adjacent faults, or even energy transfer acting over larger distances. In addition, there is clear evidence of global clustering of magnitude-9 earthquakes, but we don’t have long enough records from around the world to say for sure whether this phenomenon is real or random, or what it means. The earthquake community has had to take a step back and abandon older models of great earthquake occurrence. Today it’s not clear whether new global models will emerge, or whether local geology has the final say and that there are no universal governing relationships to guide model-based hazard assessments. In either case, hazards can be addressed directly by gathering long earthquake records that don’t depend on models. Such records can answer the societal hazard questions in a straightforward way long before there is consensus on global plate dynamics. Goldfinger and Yeats are geologists in the College of earth, Ocean and atmospheric sciences at Oregon state University. ikeda is a geologist in the department of earth and planetary science at the University of tokyo in Japan. their work on long-term earthquake cycles will appear in an upcoming issue of seismological research Letters. EARTH January 2013 43
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