- Research article
- Open Access
Punctuated growth of an accretionary prism and the onset of a seismogenic megathrust in the Nankai Trough
Progress in Earth and Planetary Science volume 5, Article number: 78 (2018)
Ocean drilling in the Nankai Trough forearc suggests a new scenario for the evolution of the Nankai subduction zone. Continuous subduction since the Late Cretaceous has been a common tectonic scenario, although the plate subduction was transferred from the Pacific Plate to the Philippine Sea Plate during the Miocene. Seismic reflection studies coupled with drilling have demonstrated that two episodes have controlled the recent evolution of the Nankai forearc: a resurgence of subduction at ~ 6 Ma after cessation since ~ 12 Ma and rapid growth of the accretionary prism since ~ 2 Ma because of the influx of large amounts of terrigenous sediments from the Japan Alps in central Japan. Both episodes were synchronous with large-scale plate reorganizations. The westward subduction of the Philippine Sea Plate initiated both in the Ryukyu and the Philippine trenches at ~ 6 Ma. Rifting in the Okinawa and Mariana troughs started at ~ 6 Ma. Compressive tectonics in northeast Japan started at ~ 3–2 Ma, and resultant mountain building with active surface erosion commenced in central Japan at ~ 2 Ma. This recent compressive tectonic phase might be due to the initiation of convergence of the Amurian Plate with the Okhotsk or North American Plate along the eastern margin of the Japan Sea. In addition to this event, the strong collision and indentation of the Izu-Bonin Arc since ~ 2.5 Ma was also enhanced in central Japan.
The Nankai Trough in southwest Japan is among the most thoroughly studied subduction zones with many geological and geophysical investigations. Geological studies have suggested that subduction and accretion have been continuous since the late Cretaceous (e.g., Taira et al. 1988). Meanwhile, several global geologic events have occurred since then, including the early Cenozoic global reorganization of plate motions (e.g., Seton et al. 2015), back-arc spreading in the western Pacific margin (Karig 1971), and intra-continental deformation caused by the India-Asian collision (Tapponnier et al. 1982). Their effects on the subduction processes must be recorded in accretionary complexes, but the resulting phenomena of each event remains unclear. Finding such a causal relationship is difficult for the ancient geological record, but easier for the recent past.
The recent drilling campaign by the Integrated Ocean Drilling Program (IODP) in the Nankai Trough (Tobin and Kinoshita 2006) has provided a clue to its Cenozoic tectonic history (e.g., Strasser et al. 2009; Kimura et al. 2011; Clift et al. 2013; Pickering et al. 2013; Kimura et al. 2014; Moore et al. 2015; Boston et al. 2016;Underwood 2018). These results demonstrate that accretion in the Nankai Trough has not been constant as previously thought (e.g., Kimura et al. 2005) but rather has been episodic even in the recent past. The present tectonic framework was initiated at ~ 2 Ma in southwest Japan in association with the rapid influx of sediment into the Nankai Trough and the Kumano forearc basin from the Japanese islands. Reviewing the in-land geology and the result of the drilling, Kimura et al. (2014) and Tsuji et al. (2017) suggested that subduction in the Nankai Trough resurged at ~ 6 Ma after a long cessation since ~ 12 Ma. Underwood (2018) suggested a switch in subducting plate from the Pacific to the Philippine Sea Plate during ~ 10 to 5 Ma. These recent interpretations challenge the traditional tectonic model of the continuous subduction (e.g., Kimura et al. 2005), which are mainly based on in-land geological information.
In this study, we interpret seismic profiles of the northern edge of the Kumano forearc basin, discuss the Nankai forearc evolution, and propose their regional linkage to the plate tectonic framework.
Nankai Trough geological setting
The Nankai forearc is separated into two tectonic domains: the inner and outer wedges that are separated by a transitional thrust zone of the outer ridge or trench slope break (Kimura et al. 2007), termed the Kumano Basin Edge Fault Zone (KBEFZ: Fig. 1, Martin et al. 2010). The accretionary outer wedge is composed of previous trench-filling turbidites and Shikoku Basin sediments of the Philippine Sea (PS) Plate, now subducting at a rate of ~ 58.4 ± 1.4 mm/a (DeMets et al. 2010). Drilling into the slope sediments and the accretionary prism of the outer wedge has documented the rapid growth of the accretionary prism since ~ 1.95–2.0 Ma (Screaton et al. 2009; Strasser et al. 2009; Kimura et al. 2011). Underplating of the clayey sediments of the Shikoku Basin also appears to have promoted the rapid growth of the lower section of the outer wedge, characterized by a seismic low-velocity zone and slow earthquakes (Kamei et al. 2013; Park et al. 2010).
The inner wedge comprises the accretionary prism and overlying sediments (Saffer et al. 2009; Gulick et al. 2010; Moore et al. 2015; Boston et al. 2016). The age of the accretionary prism, just beneath 5.6 m.y. cover sediments, is ~ 7.9–8.1 Ma at the C0009 drill site and 5.0 Ma at the C0002 drill site (Fig. 1; Saffer et al. 2009; Moore et al. 2015). The age increases with depth at C0002 to ~ 10 Ma. These data suggest that accretion started at the timing of the unconformity around ~ 6 Ma (between ~ 7.9 and ~ 5.6 Ma). Slope and forearc basin sediments then began to bury the prism rocks. The forearc basin was rapidly filled after ~ 2.0 Ma with a northward onlapping unconformity and northward migration of the depocenter above the underlying slope sediments (Gulick et al. 2010; Moore et al. 2015; Boston et al. 2016). This swift development of the forearc basin was caused by the rapid KBEFZ uplift which was caused by the accretion of trench-filling sediments supplied by mountain building on land to the trench (Kimura et al. 2008).
The on-land geology of the Kii Peninsula to the north of the Kumano Basin comprises three assemblages: a Jurassic to lower Miocene basement accretionary complex, upper Cretaceous to middle Miocene cover sediments, and middle Miocene igneous rocks (e.g., Suzuki 2012). The southern peninsula constitutes an Eocene–Oligocene to lower Miocene accretionary prism, middle Miocene shallow marine to lagoon sediments partly including coal beds, and middle Miocene igneous rocks. Middle Miocene rapid uplift is well documented from the abrupt change in the depositional environment from submarine to near-shore lagoon deposits (Hisatomi 1981). After the intrusion and eruption of a large caldera acidic volcano at ~ 15–13 Ma (e.g., Kimura et al. 2005; Miura and Wada 2007), magmatic-tectonic activity ceased. Between ~ 12 and ~ 6 Ma, no subduction-related magmatic activity was recorded in southwest Japan, and the forearc region was broadly uplifted (e.g., Kimura et al. 2014).
This event is consistently recorded as the rapid exhumation of the Cretaceous accretionary prism (Tagami et al. 1995). Kimura et al. (2014) suggested that the subduction cessation might have been caused by the collision of the northern extension of the buoyant Izu-Bonin Arc, as first suggested by Marshak and Karig (1977).
To elucidate the initiation of the slope and forearc basins of the Nankai, we reexamined multichannel seismic reflection data and core data acquired by the IODP Nankai Trough Seismogenic Zone Experiments (NantroSEIZE) project in the Nankai Trough off the Kii Peninsula, southwest Japan.
We used multichannel seismic reflection data acquired during cruise ODKM of the R/V Polar Princess in 2003, which employed a tuned airgun array with a total volume of ∼ 70 L fired at 50 m intervals and a streamer 6 km in length with 480 receivers. These seismic data were obtained in a dense orthogonal geometry in the Nankai accretionary prism off Kumano, and the survey lines extended near the coast of the Kii Peninsula (Fig. 1). We focused on three lines: the northeast-trending ODKM-4 and northwest-trending ODKM-M and ODKM-B (Figs. 1 and 2), which were reported by Tsuji et al. (2015). Data processing for the 2D seismic data included filtering, velocity analysis, stacking, deconvolution, and post-stack migration. To extract horizons of the top surface of the accretionary prism and reflectors in the forearc sediments from the intersecting seismic reflection lines, we did not apply depth conversion to the time-domain seismic profiles. The paucity of reflectors within the accretionary prism prevented us from estimating seismic velocities for a depth conversion.
We used age data from cores, cuttings, and logs collected at IODP Sites C0002 and C0009 (Ashi et al. 2009; Underwood and Moore 2012; Expedition 316 Scientists 2009; Expedition 319 Scientists 2010). Moore et al. (2015) reviewed the ages from the C0009 and C0002 sites in the Kumano Basin (Fig. 1) and inferred the evolving process of the Nankai forearc basin from a seaward-dipping slope to a basin to a mature modern basin, particularly focusing on the tectono-stratigraphic evolution since ~ 2 Ma. We expanded upon the results of stratigraphic correlation on the seismic profile of ODKM-M—which was nearly the same line as IL2535 of the 3D survey of Moore et al. (2009)—to reflectors on the ODKM-B and those on ODKM-4 (Figs. 2, 3, 4, and 5).
The evolving history of the central to southern Kumano basin is well reconstructed on the basis of seismic data calibrated by data from the C0002 and C0009 drill sites (Saffer et al. 2009; Gulick et al. 2010; Martin et al. 2010; Moore et al. 2015; Boston et al. 2016). Comparing the results of these investigations, we reexamined the northern edge of the Kumano Basin (Figs. 2, 3, 4, and 5) where the oldest section of the slope sediments has been reported above the accretionary prism (Tsuji et al. 2015). The age constraints of the sediments are poor since neither drilling nor coring have been conducted in the region. Although direct evidence of the age of the sediments is not available, an age inference was possible because the geologic setting was similar to that of the drilling site C0009 (Figs. 1 and 2), which was located on a northern piggyback slope basin of a reactivated northeast-trending fault-bend fold (Figs. 1 and 2; Tsuji et al. 2015; Moore and Strasser 2016). The stratigraphy with a clear unconformity of KL (Figs. 3 and 4) separating the upper forearc basin-filling sediments and the lower slope basin deposits (Moore and Strasser 2016) are clearly correlated. However, the KL reflector of the unconformity does not denote a synchronous reflector as documented by drilling (Moore et al. 2015). A continuous reflector of a layer within the forearc basin-filling sediments is possible to correlate as a synchronous surface, as is well documented by coring (e.g., Strasser et al. 2009; Moore et al. 2015).
Figures 3 and 4 show a hypothetical correlation between C0009 and a site on the seismic profile of ODKM-B through ODKM-4. A key reflector is K4 (Figs. 3 and 4), which is a broadly traceable layer within the Kumano Basin sediments and abuts the unconformity surface of US1 (KL of Moore et al. 2015, S2 of Saffer et al. 2009), as shown in Fig. 4. The age of the unconformity of US 1 progressively becomes younger toward the north from ~ 1.6 Ma at C0002 to ~ 0.9 Ma at C0009 (Moore et al. 2015), and the forearc deposits lap onto the unconformity surface. The US1 unconformity progresses to the northern edge of the Kumano Basin, as observed in Fig. 4.
The east-northeast-trending seismic profile of ODKM-4 is orthogonal to the north-northwest-trending profiles of ODKM-M and ODKM-B and parallel to the strike of the Nankai Trough (Figs. 1 and 2). These arrangements are the same in the 3D volume of investigation (Moore et al. 2009). The KL (US1) unconformity on the east-northeast-trending profiles is nearly parallel to the beddings of both the upper and lower sediments (Moore et al. 2015). This fact is the key to correlating the age of the KL unconformity to the US1 unconformity on ODKM-B via ODKM 4 (Figs. 2, 3, and 4) and the US3 unconformity between the slope deposits and basement of the accretionary prism (Figs. 2, 3, and 4). The start of deposition (US3) in the slope basin above the accretionary prism suggests an initiation of accretion, as is well documented in the modern Nankai frontal prism (Screaton et al. 2009; Strasser et al. 2009).
Cover terrigenous sediments and a transparent accretionary prism are recognized as introduced (Figs. 2, 3, and 4). Three sedimentary units (units 1–3) are separated by the unconformities of US1 and 2. The age of US1 might be ~ 1.0 Ma, but it becomes progressively younger northward because unit 1 gradually laps onto US1. Moore et al. (2015) suggested that the onlap unconformity started from the southern margin of the forearc basin at ~ 2 Ma and migrated northward. The profile of ODKM-B shows the presently ongoing US1 location (Fig. 4).
The age of US2 (as shown in Fig. 4) was ~ 3.7 Ma, and the seismic profile showed an angular unconformity with onlapping. Unit 3 was the lowest sediment between US2 and US3, and plant fragments were found at C0009 (Saffer et al. 2009). The age was uppermost Miocene to lower Pliocene. The age of US3 was ~ 6 Ma on the upper Miocene accretionary prism (Saffer et al. 2009; Moore et al. 2015). The age of the sediments of unit 3 above the accretionary prism (shown on the left side of Fig. 4) was unclear because the direct correlation of a synchronous layer was difficult on the profile. However, age inference may be possible since the setting of the basin was similar to that at site C0009, which was a piggyback basin behind the northeast-trending fault-bend anticline (Figs. 1 and 2; Tsuji et al. 2015), and the basin-filling sequences were composed of three units separated by three unconformities similar to those at C0009 (Fig. 5). Thus, we infer US3 may be ~ 6 Ma as well as the others.
Basement and accretionary prism
The lithology of the basement (as shown in the lower left of Fig. 4) may be different from the accretionary prism because the US3 unconformity between the sediments, and the basement was intensively reflective with a positive anomaly suggestive of hard rocks in the basement (Tsuji et al. 2015). Tsuji et al. (2015) suggested the middle Miocene igneous rocks exposed on land or the older Eocene-Lower Miocene accretionary complex for the basement. The composition of the antiformal accretionary prism to the south of the back-thrust was unknown, and the possibility of mud diapir uplift was suggested in the northern edge of the Kumano basin to the east of this region (Morita et al. 2004).
Initiation of accretion, slope deposition, and sedimentation in the forearc basin
The structure of the northern edge of the Kumano Basin (Fig. 5) indicates the initiation of accretion and the Kumano basin as follows:
Accretion of ~ 8 m.y. old sediments started at ~ 6 Ma with the deposition of cover slope sediments. The slope sediments also started to cover the stiff basement of Eocene to early Miocene age or the igneous rocks of the middle Miocene (Fig. 5a).
At ~ 3.7 Ma, a regional sedimentary break (US2) occurred with tectonic tilting in the forearc (Fig. 5b). The growth of the accretionary prism (Fig. 5a) might be related to this unconformity. A back-thrust of the accretionary prism occurred along the northern edge (Fig. 5a).
Slope deposition (unit 2–2) continued without tectonic activity from ~ 3.7 to 1.3 Ma (Fig. 5b) along the northern edge of the forearc. The growth of the outer wedge and forearc deposition around the KBEFZ started at ~ 2 Ma, as noted by Strasser et al. (2009) and Moore et al. (2015).
The reactivated deformation of the accretionary prism with continuous slope deposition occurred later than ~ 1.3 Ma (Fig. 5c). The growth strata might have been associated with uplift of the accretionary prism (Fig. 5c). The anticlinal uplift of the accretionary prism with slope sediments caused erosion in place (US1), and a subsurface slope might have appeared (Fig. 5c).
Kumano Basin deposition started at ~ 2 Ma around the southern margin of the inner wedge and reached to the northern margin of the Kumano Basin at ~ 0.9 Ma; onlap sedimentation still continues along the northern margin (Fig. 5c).
The accretionary prism thrust upwards onto the basement (Fig. 5), and unit 3 intervened along the thrust. On the basis of evolving history, the back-thrusting with ~ 2 km displacement and ~ 1 km uplift was inferred (Fig. 5), assuming P wave velocity of the sediments in such a depth of ~ 2 km s−1, as commonly observed (Moore et al. 2015; Chhun et al. 2018). The thrust changed to a synclinal fault-bend-fold into unit 2 (red line in Fig. 5c). Strata of unit 1 tilt northward gently with ascension, suggesting continuous growth and depocenter migration of the forearc basin since ~ 2 Ma, as Moore et al. (2015) suggested.
We discuss the regional tectonic significance of the well-recorded unconformities and tectonic events previously described and their relationship to the onset of the seismogenic megathrust in the Nankai Trough.
Subduction initiation of the PS plate at ~ 6 Ma
An age of ~ 6 Ma for the initiation of accretion with back-thrusting upon the stiff basement (Figs. 4b and 5a) suggests that subduction of the PS Plate resurged after a long cessation since ~ 12 Ma (Fig. 6: Kimura et al. 2014; Tsuji et al. 2015). The main part of the Kii Peninsula appears to be composed of the middle Miocene volcano-plutonic rocks related to the collision of the ancient Izu-Bonin arc and the active Shikoku Basin (Kimura et al. 2014). Simplified profiles at ~ 12 Ma and ~ 6 Ma are shown in Fig. 6.
The subduction cessation at ~ 12 Ma might have been due to the loss of slab pull force resulting from the collision of the buoyant arc and the hot back-arc Sikoku basin. The subduction resurgence at ~ 6 Ma may be related to cooling and densification of the PS Plate, which was once stacked beneath southwest Japan (Fig. 6). Subduction resurgence is also suggested by the resurgence of calc-alkaline igneous activity in southwest Japan (Kamata and Kodama 1999; Kimura et al. 2005). Kimura et al. (2005) inferred that the subduction of the PS Plate continued between 12 and 6 Ma, although the subduction decelerated because the alkaline basalt activity during that period would be ascribed to the subduction. However, Sakuyama et al. (2009) investigated the alkaline basalts in northern Kyushu and concluded that the activity is related to a mantle plume broadly upwelled in eastern Asia rather than subduction, as suggested by Tatsumi et al. (1990). The broad mantle plume upwelling in east Asia was recently thought to be a result of mobilized regional asthenospheric dynamics caused by the India-Asia collision (Jolivet et al. 2018).
The subduction of the PS Plate in the Nankai Trough must be interpreted within a regional plate tectonic framework. Since the late 1990s, new geodetic data using Global Positioning System (GPS) have been incorporated to reconstruct the plate kinematics, although the timescale is different neither from a traditional geological timescale nor an earthquake slip vector with a hypothesized recurrence time. However, combining these different data sets is useful to infer the plate motion, particularly with respect to the Asian continent. The recent revision of plate kinematic models of MORVEL (DeMets et al. 2010) or NNR-MORVEL56 (Argus et al. 2011) is a workable hypothesis.
The relative plate motion from NNR-MORVEL56 (Fig. 7) demonstrates that the PS Plate subducts beneath the Amurian Plate to the northwest in the Nankai Trough, the Yantz Plate to the west along the Ryukyu Trench, and the Sunda Plate along the Philippine Trench at present (Fig. 7). The Okinawa Trough, the active back-arc rift of the Ryukyu arc, landing both on Kyushu and Taiwan, appears to be formed by suction force resulting from trench retreat caused by slab pull force of the old, cold, and dense west Philippine Sea part of the PS Plate (e.g., Kamata and Kodama 1999; Heuret and Lallemand 2005). A recent active rift is inferred to have started at ~ 6 Ma with the clockwise rotation of Ishigaki Island. Rifting in the northern Kyushu also started at ~ 6–5 Ma (Kamata and Kodama 1999). The Taiwan and the Luzon islands on the PS Plate overthrust upon the continental crust, as first noted by Suppe (1981), whereas the PS Plate subducts beneath the Sunda Plate in the Philippine Trench (Fig. 7). Hall (2002) showed that the trench was already established at ~ 5 Ma. Relative PS Plate motion with respect to the Yantz and Sunda plates is currently faster than 90 mm y−1 (Fig. 7; DeMets et al. 2010). These parts of the PS Plate are as old as the late Cretaceous to Eocene and require a sufficient westward and downward driving force of slab pull (Faccenna et al. 2017). The ~ 6 Ma initiation of the PS Plate subduction in the Nankai Trough appears to be derived from and associated with the westward subduction along the Ryukyu and Philippine trenches.
Another related event at ~ 6 Ma is the rifting initiation of the Mariana Trough (Hussong and Uyeda 1982; Yamazaki et al. 2003). The rifting has been interpreted as an anchored trench model and westward absolute motion of the PS Plate (Uyeda and Kanamori 1979). Such a relationship is well documented from the relative PS Plate motions with respect to its surroundings (Fig. 7). Recently, Faccenna et al. (2017) suggested that the Izu-Bonin-Mariana Trench switched from trench retreat to trench advance as a result of the slab pull force of the PS Plate along the Ryukyu Trench sometime between 10 and 5 Ma. We suggest that, if the timing of the switch was ~ 6 Ma, geological observations both on land and in the subsea forearc should be consistent with this inference. The investigations of seismic tomography around the PS Plate also present a key role in reconstructing the tectonic history of the Nankai Trough. Wu et al. (2016) presented a precise reconstruction of the subducted slab of the PS Plate in the Nankai Trough and the Ryukyu and Philippine trenches. Considering the reconstructed plate kinematics based on a GPS data set (Argus et al. 2011), a ~ 700 km-long slab of PS Plate beneath the East China Sea (Wu et al. 2016) can be explained largely by convergence between the Yantz and PS plates for ~ 6 Ma with the ~ 90 km my−1 and spreading rate of the Okinawa Trough and a trench retreat of ~ 25 km my−1 in the Ryukyu Trench (Argus et al. 2011). The ~ 300–400 km-long slab of the PS Plate beneath southwest Japan is also consistent with northwestward subduction at a rate of ~ 60 km my−1 between the Amurian and PS plates (Argus et al. 2011).
The reason for the subduction starting at ~ 6 Ma is unclear, but recently Faccenna et al. (2017) suggested that the force of the slab pull of the PS Plate in the West Philippine Sea may have been beyond the gravitational stability caused by the cooling and densification.
Modification of tectonic framework and mountain building in central Japan at ~ 2 Ma
The rapid sediment influx to both the Nankai Trough and forearc Kumano Basin and the resultant fast growth of the Nankai forearc started at ~ 2 Ma. The sediment was supplied from the Japan Alps in central Japan (e.g., Kimura et al. 2008; Moore et al. 2015). The mountain building in central Japan was a result of the collision between southwest and northeast Japan, which is now ascribed to the collision of the Amurian Plate with the Okhotsk or North American Plate (Wei and Seno 1998; Heki et al. 1999; Miyazaki and Heki 2001; Argus et al. 2011). Additionally, the northward indentation and collision of the Izu Peninsula has been enhanced in central Japan (Niitsuma 1989). The convergent boundary zone between the Amurian and the North America or Okhotsk plates is mainly along the eastern margin of the Japan Sea (Tamaki and Honza 1985; Okamura et al. 2007) and started E–W compressive tectonics from ~ 3–2 Ma along the margin (Okamura et al. 2007). This event was synchronous with the initiation of mountain building in central Japan and the sediment influx to the Kumano Basin and Nankai Trough (e.g., Kimura et al. 2008; Strasser et al. 2009; Moore et al. 2015). The appearance of oblique subduction-related tectonics on land, as represented by the dextral Median Tectonic Line (MTL), were also at ~ 2 Ma (Okada 1973). The activity of the KBEFZ as a splay fault started at ~ 2 Ma and the sense of slip of the KBEFZ associates with a dextral component (Tsuji et al. 2014b). The obliquity increased because of the additional eastward motion of southwest Japan associated with the onset of the Amurian/Okhotsk Plate boundary (Fig. 7).
Thus, the tectonic events at ~ 6 and ~ 2 Ma were synchronous in the eastern Asia and Philippine Sea regions. More detailed dating of all the events at a 100–10 Ka timescale and investigation of the quantitative causal relationship are significant targets of geodynamic research in this region.
Onset of the seismogenic megathrust and tectonic history
The control of earthquake rupture areas in a subduction zone megathrust is among the most fundamental questions in geodynamic research. In the case of the Nankai Trough, three major controlling factors have been proposed thus far: the surface topography of the subducting plate, such as seamounts (Kodaira et al. 2000); a locally dense and rigid upper plate because of igneous rock composition (Kodaira et al. 2006) other than an ancient accretionary complex (Taira et al. 1988); and frictional properties of the plate boundary megathrust with abnormal pore fluid pressure (e.g., Moore and Saffer 2001; Tsuji et al. 2014a). Kimura et al. (2018) recently proposed that the middle Miocene igneous rocks of the hanging wall in southwest Japan control the rupture area of the seismogenic megathrust in the Nankai Trough and emphasized the significance of tectonic hysteresis of the upper plate. The accretionary prism that has developed since ~ 6 and ~ 2 Ma works as an upper plate wherein elastic strain energy is stored, perhaps releasing in a great tsunamigenic earthquake. The hanging wall of the inner wedge is composed of rock with an abnormally high seismic velocity (e.g., Kamei et al. 2013). The geologic component of the hanging wall is either old basement or a young but extremely over-consolidated accretionary prism, which will be soon clarified by the deep drilling of the IODP NantroSEIZE program. The accretionary prism of the transition zone between the ~ 6 million year (m.y.) old inner and ~ 2 m.y. old outer wedges and the megathrust—particularly beneath the outer accretionary prism—is the location where shallow slow earthquakes occur (Obara and Kato 2017). The plate boundary megathrust of the slow earthquakes (Araki et al. 2017; Tsuji et al. 2017) is within a low seismic velocity zone (Park et al. 2010; Kamei et al. 2013). The results of the drilling of the IODP NantroSEIZE and the tectonic history described in this study suggest that the component of the megathrust is underthrust sediments with abnormal fluid pressure starting at ~ 2 Ma, as first inferred by Moore and Saffer (2001).
Seismic reflection studies coupled with drilling results have concluded that two episodes have controlled the recent evolution of the Nankai forearc: a resurgence of subduction at ~ 6 Ma after cessation since ~ 12 Ma and the rapid growth of an accretionary prism since ~ 2 Ma caused by a large influx of terrigenous sediments from the Japan Alps in central Japan.
This conclusion is supported by the following observations and considerations:
The geological sequences of the northern margin of the Kumano Basin are composed of unit 1, which is younger than the 0.9 m.y. old, forearc basin-filling sediments; unit 2–1 and unit 2–2, deposited from ~ 3.7 to ~ 1.2 Ma as slope basin sediments; and unit 3, deposited from ~ 6 to 3.75 Ma as the lowest slope basin sediments. Each unit is separated by the unconformities of US1 and US2. Unit 3 unconformably (US3) overlies the accretionary prism at ~ 7 Ma and the old basement of middle Miocene igneous rocks or the early Miocene accretionary complex.
The deposition of the sediments progressed along with the tectonic deformation of the forearc. The start of the slope deposition above the accretionary prism at ~ 6 Ma suggests the start of accretion and subduction. The broad unconformity of US1 suggests the formation of the Kumano Basin since ~ 2 Ma, and deposition reached to the northern margin of the basin at ~ 0.9 Ma as a result of northern onlapping.
Both episodes at ~ 6 and ~ 2 Ma were synchronous with regional plate reorganizations. The westward subduction of the PS Plate initiated both in the Ryukyu and the Philippine trenches at ~ 6 Ma. Rifting in the Okinawa and Mariana troughs started at ~ 6 Ma. Compressive tectonics in Northeast Japan started at ~ 3–2 Ma, and resultant mountain building with active surface erosion commenced in central Japan at ~ 2 Ma. This recent compressive tectonic phase might be a result of the eastward migration of the Amurian Plate and convergence with the Okhotsk or North America plates. In addition to this event, the strong collision and indentation of the Izu-Bonin Arc since ~ 2.5 Ma has also been enhanced in central Japan.
Integrated Ocean Drilling Program before 2012 and International Ocean Discovery Program since 2013
Kumano Basin Edge Fault Zone
Nankai Trough Seismogenic Zone Experiments
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We thank Kyoko Tonegawa for her assistance in this study. We also thank the many scientists who joined the IODP NantroSEIZE experiments both abroad and shore-based for helpful discussions. We appreciate two anonymous reviewers whose comments improved the manuscript.
This work was supported by the Japan Society for the Promotion of Science Grants-in-Aid for Scientific Research (KAKENHI) Grant Number 12345678.
HK was partly funded by ABC project (ABC-123-456).
Original seismic profile (image file) can be shared. If you use the original seismic data, please contact author for data requests.
The authors declare that they have no competing interest.
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Kimura, G., Koge, H. & Tsuji, T. Punctuated growth of an accretionary prism and the onset of a seismogenic megathrust in the Nankai Trough. Prog Earth Planet Sci 5, 78 (2018). https://doi.org/10.1186/s40645-018-0234-1
- Nankai Trough
- Accretionary prism
- Seismogenic zone
- Forearc basin
- Subduction zone
- Amurian Plate
- Okhotsk Plate
- Kumano Basin