Transition from collision to subduction and its relation to slab seismicity and plate coupling
© Arai and Iwasaki; licensee Springer. 2015
Received: 15 March 2015
Accepted: 14 May 2015
Published: 27 May 2015
The Philippine Sea plate exhibits an along-trench variation in structure, from an eastern volcanic arc to a typical oceanic crust in the west. The regional difference of intra-slab seismicity implies that this transition occurs around the Itoigawa-Shizuoka Tectonic Line (ISTL). However, the nature of the subducting slab in this region has not been studied in detail. Here, we investigate the structure of the Philippine Sea plate subducting beneath the ISTL. Using active source data, we found reflective portions at depths of 14–18 km. An amplitude evaluation for the reflection phases showed that the reflective zone has a P wave velocity as low as 3.0 km/s. Together with its slightly northwestward-dipping geometry, we interpreted that the low-velocity zone is at the plate boundary and can be attributed to high water content supplied by the slab. This feature is in great contrast to the collision zone further east, where the slab top is less reflective and the dehydration process is inactive. This structural difference also correlates well with the regional distribution of slab seismicity. The reflective zones we found are likely located at the down-dip end of the locked zone, where high slip deficit rates are currently observed. This may suggest that changing fluid pressures and the resulting frictional properties in the down-dip direction control the transition from a coseismic rupture zone to a deeper aseismic zone.
KeywordsNankai trough Izu collision zone Philippine Sea plate Plate coupling Frictional property Wide-angle reflections
This systematic variation in fluid distribution correlates well with the regional distribution of intra-slab seismicity; Seno and Yamasaki (2003) pointed out that, unlike the Nankai subduction zone, there is no intraslab seismicity beneath the Izu collision zone and indicated that the dehydration process is a controlling factor for the seismogenic process. This along-trench change in seismicity occurs suddenly at the Itoigawa-Shizuoka Tectonic Line (ISTL), a geological boundary between the northeast Japan and southwest Japan arcs, implying that the ISTL coincides spatially with the structural transition of the Philippine Sea plate from arc-like crust to oceanic crust. On the other hand, onshore seismic surveys and bathymetric features indicate that not oceanic crust but arc-like crust (several kilometers thicker than typical oceanic crust) exists just south of the ISTL (Nakanishi et al. 1998; Nishizawa et al. 2006; Kodaira et al. 2008), leaving the open question of the nature of the Philippine Sea plate subducting beneath the ISTL.
Several seismic experiments were carried out around the southernmost part of the ISTL in the last few decades (Research Group for Explosion Seismology 1988, 1992), and these experiments have the potential to constrain the eastern limit of the subduction system in the western Nankai subduction zone (Fig. 1). However, these seismic data were not fully examined in the context of the transition of the Philippine Sea plate mentioned above. In this paper, we reinterpret them in order to determine the nature of the slab and its relation to intraslab seismicity, especially in relation to the dehydration process within the oceanic lithosphere.
The Nankai subduction zone is also known as a seismogenic zone where large megathrust earthquakes have repeatedly occurred (e.g., Ando 1975). Around the southernmost ISTL, a strongly coupled zone outlined by geodetic measurements and seismic profiles used in this paper cross the zone where large slip deficit rates are currently observed (Suito and Ozawa 2009). Spatial variation in frictional properties along plate boundaries often appear as a difference in the seismic reflectivity of active source data; large-amplitude reflections are found in aseismic (conditionally stable) regions with weak plate coupling, while weakly reflective interfaces correspond to locked zones that rupture during a large earthquake (Kodaira et al. 2004; Nakanishi et al. 2004; Mochizuki et al. 2005). We used this correlation between the intensity of seismic reflections and frictional properties to investigate the structure atop the slab. Our seismic data provide insights on the down-dip end of the rupture zone along the plate interface in the easternmost Nankai subduction zone.
Data and methods
Two seismic experiments along the southernmost ISTL carried out by Research Group for Explosion Seismology (RGES) (Fig. 1) are expected to provide important structural constraints on the easternmost part of the area of high intraslab seismicity of the Philippine Sea plate; the eastern profile, laid out almost parallel to the ISTL, was carried out in 1983 (Research Group for Explosion Seismology 1988), and the western profile was performed in 1987 on the western side of the ISTL (Research Group for Explosion Seismology 1990, 1992) (Fig. 1b). Both seismic lines were approximately 60-km-long profiles and 71 (eastern profile) and 77 (western profile) stations were deployed along these lines. As seismic sources, five (eastern profile) and six (western profile) dynamite shots (with a charge of 300–700 kg) were fired. Seismic waves were recorded at a sampling rate of 100 Hz at all stations.
In order to explain these reflection phases, we constructed P wave velocity models for both profiles by forward modeling using a ray tracing method (Iwasaki 1988). The P wave velocity models for the upper 5 km of the crust were constructed from first arrivals. Then, the model was extrapolated to deeper parts using velocity models from other nearby active-source experiments (Arai et al. 2009; Arai and Iwasaki 2014) and regional passive-source tomography (Matsubara et al. 2008). Thereafter, we mapped a reflector using travel times of high-amplitude reflections. Finally, synthetic seismograms were calculated using the code SEIS83 (Červený and Pšenčík 1983) to evaluate the velocity contrast across the reflector.
Results and discussions
A distinct reflector was imaged at 14 km depth in the eastern profile (Fig. 2b) and 18 km depth in the western profile (Fig. 2e). Based on the misfit of travel times (within 0.1 s) and the uncertainty of the velocity model (0.5 km/s), we roughly estimated the error for the depth of the reflector to be less than 2.0 km. To estimate the velocity contrast across the reflective zone, Fig. 2 compares observed seismic records of SP-W1 and SP-E4 with synthetic seismograms calculated by models in which a low-velocity layer with Vp = 2.0–3.0 km/s was assumed at depth. The thickness of the layer was assumed to be 100 m according to previous studies (e.g., Mochizuki et al. 2005). We see that the observed high-amplitude reflections are successfully reproduced by these models. Figure 3 examines other models by assuming different velocity values for the layer. We confirmed that the seismic record of SP-W5 also prefers a model with a low-velocity layer of Vp = 3.0 km/s (Fig. 3a–c). The synthetic seismograms from a model with Vp = 4.0 km/s may also be acceptable (Fig. 3d), implying that the velocity value for the layer includes a large error of up to 1.0 km/s. However, a model with Vp = 6.0 km/s (Fig. 3e) and no low-velocity zone (Fig. 3f) cannot explain the reduced amplitude of observed first arrivals.
Although the depth of the reflector in this study is 5–10 km shallower than the slab depth proposed by passive-source seismic data (e.g., Nakajima et al. 2009), the geometry (gently dipping northwestward) is consistent. This discrepancy may arise from the large uncertainty of the slab location in previous models because of its distorted geometry in this region and lack of deep seismicity in the Izu collision zone to the east. Together with the necessity for a low-velocity zone along the reflector as explained above, this suggests that the reflector is the top of the subducting Philippine Sea slab, forming a thin low-velocity layer. We also examined other interpretations for the reflector, such as the Moho occurring beneath the island arc and a mid-crustal reflector, and excluded both possibilities for the following reasons. First, the reflector we observed is located at 14–18 km depths, which is more than 15 km shallower than the Moho depth estimated in the study area (Kato et al. 2010; Katsumata 2010). Second, the velocity jump across the reflector needs to be more than 2.0 km/s. On the other hand, typical velocity contrasts at a mid-crustal reflector and Moho are less than 1.0 km/s (Arai et al. 2009). Thus, it is unlikely that the reflector is either of these.
The estimated velocity values for the reflector (2.0–4.0 km/s) are consistent with those proposed by other seismic experiments in the Nankai subduction zone (Kodaira et al. 2002; Iidaka et al. 2004). According to Kodaira et al. (2002), a thin low-velocity layer lying between the subducting oceanic plate and the overriding landward plate has a high water content, expelled from the downgoing crust and/or serpentinized mantle. Although the seismic data in this study cannot constrain the internal structure of the slab, we speculate from the similarity in the reflection phases that the interpretation by Kodaira et al. (2002) is also true for the easternmost Nankai trough. Our interpretation of the reflective zone as having a high fluid content is supported by studies of electrical resistivity; a resistivity model by Aizawa et al. (2004) showed that a conductive zone exists just above the subducting Philippine Sea slab on the western side of Mt. Fuji, close to our study area, while such a body is not imaged on the eastern side. Matsubara et al. (2008) pointed out a similar contrast from regional seismic tomography, namely, the slab in the Nankai subduction zone, imaged as a zone with low P wave and S wave velocities and high Vp/Vs ratios, indicates a high water content, while the subducting portion beneath the Izu collision zone is imaged as a high-velocity anomaly.
Our seismic data may provide another important constraint on the frictional property along the plate interface, since the seismic structure is closely correlated to interplate coupling (e.g., Fujie et al. 2013). In the easternmost Nankai subduction zone, a strongly coupled zone is outlined by geodetic measurements (Sagiya 1999; Suito and Ozawa 2009). The estimated slip deficit rate of >20 mm/year, almost equivalent to the convergence rate between the overriding and subducting plates, implies that strain is being steadily accumulated at the contact, and will probably lead to coseismic rupture during a megathrust earthquake (Ando 1975). Our seismic lines in the north–south direction cross the transitional boundary between a strongly coupled zone and a weakly coupled zone along the plate boundary. The reflective zones we found are likely located close to the down-dip end of this locked zone (Fig. 4b). This spatial correlation may suggest that the reflective zone delimits the down-dip end of the coseismic rupture zone. Similar spatial patterns of seismic reflectivity (a shallow coseismic region with low reflectivity and a deeper aseismic region with relatively high reflectivity) are also observed in other areas of the Nankai subduction zone (Kodaira et al. 2002, 2004; Iidaka et al. 2004). In the Tokai region further west of this study, Kodaira et al. (2004) correlated this reflective zone with the distribution of slow slips, and suggested that high-pressure fluids supplied by hydrous minerals within the slab effectively extend a region of stable slips, and consequently generate the slow slip. Changing fluid pressures and the resulting frictional properties in the down-dip direction probably control the transition from a coseismic rupture zone to a deeper aseismic zone.
The reflective zone we observed is 10–15 km wide in the down-dip direction, which is well constrained by the fact that high-amplitude reflections are not observed in shot records other than those shown in Figs. 2 and 3. In the western part of the Tokai region where the slow slips occur, the reflective zone is located at depths of approximately 30 km and is extended over a much broader region in the down-dip direction than in this study (Iidaka et al. 2004). The difference in slab depth must produce the difference in the nature of dehydration from the subducting plate and the frictional property along the plate boundary.
We found a reflective zone at 14–18 km depths at the eastern end of the Nankai subduction zone. An amplitude evaluation of the reflections showed that the layer has a P wave velocity as low as 3.0 km/s, which we interpreted as a low-velocity layer along the plate boundary that is probably enriched in fluids supplied by the subducting slab. The high-amplitude reflection phases are similar to those observed in other regions of the Nankai subduction zone and are in a great contrast to the Izu collision zone further east where the slab top is less reflective and the dehydration process is inactive. This structural difference also agrees well with the sudden increase in slab seismicity across the ISTL. Therefore, we suggest that, similar to the western Nankai subduction zone, the fluid-rich crust is subducting beneath the ISTL, and dehydrated fluids are enhancing the intraslab seismicity. The reflective zones we found are likely located at the down-dip end of the locked zone where high slip deficit rates are currently observed, which may suggest that the reflective zone with high water content delimits the down-dip end of the coseismic rupture zone.
We are grateful to the members of the Research Group for Explosion Seismology for the data acquisition. We also thank the editor and two anonymous reviewers for useful comments and the Japan Meteorological Agency for the hypocentral data. We used the GMT software (Wessel and Smith 1998) to draw the figures.
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