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Wide-angle refraction experiments in the Daito Ridges region at the northwestern end of the Philippine Sea plate
© Nishizawa et al.; licensee Springer. 2014
Received: 2 July 2013
Accepted: 5 November 2013
Published: 30 April 2014
Three large bathymetric highs (from north to south: the Amami Plateau, the Daito Ridge, and the Oki-Daito Ridge) originating from paleo-island arcs characterize the northwestern end of the Philippine Sea plate. We obtained 10 seismic refraction and multi-channel seismic reflection profiles across and along these bathymetric highs and obtained P wave velocity (Vp) models of the crust and the uppermost mantle. Although there are large variations in the crustal structure throughout this region, these bathymetric highs usually have a middle crust with Vp of 6.3 to 6.8 km/s, a lower crust with Vp of 6.8 to 7.2 km/s, a Pn velocity of 7.6 to 7.8 km/s, and a total crustal thickness of 15 to 25 km. These features are similar to those of the Izu-Ogasawara (Bonin)-Mariana island arc and the Kyushu-Palau Ridge, which are immature paleo-island arcs. However, the crust at the southwestern part of the Oki-Daito Ridge contains a relatively thin middle crust and a smaller total crustal thickness compared with other ridges in this region. In addition, we identified a deep reflector beneath the ridge, with these properties indicating a different origin, such as intraplate volcanism.
The topographic highs of the Amami Plateau consist of three east-west-oriented ridges that extend for approximately 300 km, with the middle ridge being both the largest and the shallowest in depth (less than 2,000 m). The northwestern end of the plateau is currently subducting beneath the Ryukyu (Nansei-Shoto) Trench (Nishizawa et al. 2009). Igneous rocks obtained from the plateau suggest that its pedestal is Cretaceous in age, and the ridge portion situated on the pedestal formed in the Middle Eocene (Tokuyama et al. 1986;Ishizuka and Yuasa 2007). Hickey-Vargas (2005) described basalt and tonalite from the Amami Plateau that have geochemical characteristics of intra-oceanic island arc rocks and which formed at 70 to 118 Ma during the Cretaceous. Based on these data, Tokuyama (2007) concluded that the Amami Plateau was an active island arc before the Eocene.
Further south, the Oki-Daito Ridge, in the broad sense, has a total length of approximately 700 km and is topographically divided into three parts: the Oki-Daito Rise in the southwest, the Oki-Daito Plateau in the northwest, and the Oki-Daito Ridge in the strict sense hereafter referred to simply as the Oki-Daito Ridge in the east (Figure 1). The Oki-Daito Plateau connects with the Daito Ridge at its northwestern end. The Oki-Daito Ridge is characterized by two rows of linear bathymetric highs that have a V-shaped topographic depression between them. Volcanic edifices on the Oki-Daito Ridge and the Minami-Daito Basin to the north have geochemical characteristics similar to ocean island basalt (OIB) and have an estimated age of 44 to 48 Ma (Ishizuka et al. 2013). By contrast, alkali basalt dredged at the southeastern bathymetric high on the Oki-Daito Ridge has an age of 65 Ma and formed through undetermined volcanic activity (Okino and Kato 1992). As a result, these data indicate that volcanic activity has occurred on at least two separate occasions in this region.
Kasuga et al. (1986) analyzed gravitational and geomagnetic data from the region around the Daito Ridge and the northern Oki-Daito Ridge, and reported that free air and Bouguer gravity anomalies indicate that the crust below the ridges is thick. Furthermore, magnetic anomalies suggest that these ridges have a magnetic basement with properties characteristic of intermediate and acidic rock types, combined with several intrusive rocks that have intermediate and basic rock properties (Kasuga et al. 1986). They concluded that the two ridges are remnants of island arcs, on the basis of previous results from rock samples and other geological features.
Ishihara and Koda (2007) gravimetrically estimated the crustal thickness of the Philippine Sea plate using a simple four-layer model, which comprised seawater, sediments, crust, and lithospheric mantle, with respective densities of 1,030, 2,300, 2,800, and 3,300 kg/m3. Their results show that the Amami Plateau, the Daito Ridge, and the Oki-Daito Ridge (in the broad sense) have crusts of 15- to 20-km thickness. However, they could not constrain its overall constitution (i.e., the relative proportions of the upper, middle, and lower crusts). Furthermore, there is insufficient information about densities and sediment distribution to obtain a more thorough image of the crustal structure in this region.
Various seismic refraction experiments have been conducted in this region in an attempt to reveal more of its crustal structure. Murauchi et al. (1968) revealed that the Oki-Daito Ridge has a continental-type upper crust that is up to 5 km thick and has a P wave velocity (Vp) of 6 km/s. Exploration conducted by Nishizawa et al. (1983) using a small number of ocean bottom seismographs (OBSs) produced similar crustal models for beneath the Amami Plateau, which indicate an upper crust up to 4 km thick with Vp of 5.4 to 5.6 km/s. However, they did not obtain the precise depth of the Moho due to a lack of seismic energy and insufficient travel time data. There was also little available information to image the entire paleo-island arc crust region of the Daito Ridges.
Recently, Calvert (2011) reviewed island arc seismic velocity models and discussed two examples as evolutionary end members: the Aleutian arc, initiated in the Eocene and not significantly affected by extension and rifting, and the Izu-Ogasawara (Bonin)-Mariana (IBM) arc-backarc system, also initiated in the Eocene but variably affected by localized extension and two episodes of arc rifting and backarc spreading. Calvert (2011) divided both arc crusts into three parts based on their Vp and crustal thickness proportions and showed that their middle and lower crusts have higher seismic velocities than those of typical continental crust. Moreover, the Aleutian middle crust has Vp of 6.5 to 7.3 km/s, which is significantly higher than that of the IBM middle crust (6.0 to 6.8 km/s). Thus, comparing the arc crustal structure of the Daito Ridges with these arc models will provide important insight into their evolution.
From 2004 to 2006, we carried out extensive wide-angle seismic and multi-channel seismic (MCS) explorations in the Daito Ridges region as part of the Japanese Continental Shelf Survey Project. This paper presents the first seismic images of the deeper structures beneath the bathymetric highs in this region and aims to contribute to future research into the early history of the Philippine Sea plate.
The locations of our seismic profiles in relation to known bathymetric, Bouguer gravity anomaly, and magnetic anomaly data are shown in Figure 2. In this seismic experiment, we shot a tuned array of air guns with a volume of 8,040 in.3 (132 L) at intervals of 200 m (90 s) for the wide-angle seismic profiles and at intervals of 50 m for the MCS profiles (480 channels, 60-folds). OBSs were deployed at an average interval of 5 km, except for ODr1, where the interval was 3 km.
We used pop-up type OBSs equipped with a three-component 4.5-Hz geophone and a hydrophone. Sensor outputs were continuously recorded on a hard disc at a sampling rate of 200 Hz with a resolution of 24 bits. Each OBS has an acoustic release unit for retrieval. The OBS locations were determined using acoustic waves from a ship with GPS navigation and direct water waves from an air gun array to the OBS.
OBS record sections were produced by 4- to 16-Hz bandpass filtering, predictive deconvolution (first zero crossing, operator length of 660 ms), and a local slant stack to enhance the signal-to-noise ratio. We read out the arrival times of the refraction and reflection signals from these record sections. Using these data, we produced Vp models by a combination of tomographic inversion and two-dimensional forward modeling. An initial velocity model was produced with the upper sedimentary layer constrained by the MCS data. First arrival data were inverted for a two-dimensional velocity model using the tomo2d tomographic inversion code of Korenaga et al. (2000). We constructed the model from shallower to deeper crust by increasing the offset limits of the input travel time data. In the velocity models derived for all profiles, the horizontal grid spacing is 0.5 km, and the vertical grid spacing gradually increases with depth according to the relation 0.05 + (0.01 × depth (km))1/2 km.
Tomographic inversion misfits were less than 50 ms for almost all velocity models, and the resolution and reliability of our models were examined using checkerboard tests. We built a reference model by adding sinusoidal anomalies with a horizontal dimension of 10 km, a vertical dimension of 2.5 km, and a velocity perturbation of ±5% to the upper crust of our preferred final model. The vertical cells in the middle and lower crusts were 5 and 10 km, respectively, in the vertical direction and 5 km in the horizontal direction. We used ray coverage in addition to checkerboard test results to represent model reliability. Better recovery of the checkerboard pattern and higher ray density indicate higher resolution.
To utilize reflection arrivals and low-amplitude refraction signals at distant offsets, we carried out forward modeling using a two-dimensional ray-tracing algorithm (Fujie et al. 2000;Kubota et al. 2009). We used the tomographic model as an initial ray-tracing model and then improved it through trial and error. Where the final result needed to be confirmed, additional tomographic inversion was conducted using the ray-tracing model as an initial model of inversion. The final velocity models in this study are the results of forward modeling, except for DAr5. The total length of DAr5 is 1,185 km, the longest line in our exploration, and thus, we did not examine the model by forward modeling due to time limitations. In the last step, two-dimensional synthetic seismograms were calculated by the finite difference method, using the E3D code of Larsen and Schultz (1995), and compared with the observed amplitude variation in the record sections.
The calculated Vp models discussed below are presented from north (the Amami Plateau) to south (the Oki-Daito Ridge). The Amami Plateau was transected by two north-south-oriented seismic lines (DAr2 and DAr5), whereas six lines were run across and along the Daito Ridge (ODr1, DAr2, ODr9, DAr5, DAr3, and DAr4). We also report Vp models for these north-south profiles, except for line DAr4, which does not transect the main body of the Daito Ridge. Seven seismic lines were shot across and along the Oki-Daito Ridge. However, since line ODr2 was too short to resolve the deeper part of the Oki-Daito Ridge, we only show results for OKr4, ODr1, and ODr9 for the northwestern part of the ridge and ODr5, DAr5, and KPr15 for the southwestern part.
Following Calvert (2011), we loosely divide our crustal models into three parts (upper, middle, and lower crusts) based on their velocities, velocity gradients, and thickness proportions, and subsequently describe their characteristics.
PmP travel times infer a maximum depth of 19 km for the Moho discontinuity beneath the middle-plateau bathymetric high (Figure 4), whereas the crust below the southern high is the thinnest of the three rows. The Pn velocity immediately beneath the plateau is approximately 7.6 km/s (significantly lower than 8 km/s), which is verified by both inversion and forward modeling. The synthetic seismograms in Figure 4c also explain both observed travel times and amplitude variation with an offset.
Despite the large heterogeneity among the Vp models for the DAr2, ODr9, DAr5, and DAr3 lines, a common characteristic of these velocity structures is another notable difference between the northern and southern parts of the ridge. A material with Vp ≤ 6.3 km/s and a thickness of 6 to 11 km is present in the southern region, while a material with Vp ≥ 6.3 km/s ascends to approximately 2 km from the seafloor in the northern region.
Figure 8a illustrates three Vp models across the two rows of linear bathymetric highs and a valley between them in the southeastern Oki-Daito Ridge. The three profiles transect a bathymetric high on the northern row, the shallowest portion in the southeastern Oki-Daito Ridge. A common feature is the presence of a thick middle crust with Vp of 6.3 to 6.8 km/s beneath the bathymetric high. The upper crust (with Vp of approximately 3.0 to 6.3 km/s) is slightly thicker beneath the valley. The thickness of the lower crust (with Vp of 6.8 to 7.2 km/s) is 7 to 10 km, and the total crustal thickness is 20 to 30 km. Although the Pn velocity is about 8.6 km/s at the transition from the Oki-Daito Ridge and West Philippine Basin, the velocity below the ridge crest is 7.6 to 7.8 km/s. The high uppermost mantle velocity of about 8.6 km/s seems to belong to the West Philippine Basin, which is horizontally and vertically heterogeneous and has a Pn velocity ranging from approximately 8.0 to 8.6 km/s (Figure 8a, b).
Vp and the thickness of the uppermost sediment layer in the Oki-Daito Plateau are 1.8 to 2.2 km/s and about 1 km, respectively (Figure 9a). The upper crust has Vp of about 3.0 to 6.3 km/s and a thickness of 3 to 7 km. Underlying the upper crust, there is a middle crust with Vp of 6.3 to 6.8 km/s and a thickness of 3 to 5 km, and a lower crust with Vp of 6.8 to 7.2 km/s and a thickness of 10 to 15 km. The Pn velocity here is 7.7 to 7.9 km/s, and the total crustal thickness is 20 to 25 km. These characteristics are similar to those of the Daito Ridge.
The middle crust of the Oki-Daito Rise is thin compared to that at other bathymetric highs in this region (Figure 9a). The Vp distribution in the crust is well-constrained, as shown in Figure 7b, and Vp at the crust bottom is estimated to be 7.2 km/s. The total maximum crustal thickness of 14 km is also thinner compared with other ridges in this region. The Pn velocity is 7.8 km/s in the northern part of the rise along OKr4 (Figure 9a, top), but a higher Pn velocity (≥8.0 km/s) was measured along ODr9 (Figure 9a, center) and the southern rise along OKr4.
OBSs deployed on the Oki-Daito Plateau and Oki-Daito Rise frequently recorded large-amplitude signals over distances of about 180 km. Figure 10 shows examples of the record sections obtained at OBS 58 and 115 on ODr9. When considering these signals as first arrivals, we were unable to construct a Vp model to account for these travel times; thus, we interpreted the travel times as reflection signals and estimated the position of the reflector using the travel time mapping method of Fujie et al. (2006). The reflector was denoted with a white line in Figure 10c. In addition to the mapping, we examined the reflector position and Vp distribution by forward modeling. Assuming a rough estimate of the mantle velocity and a reflector extending for 110 to 290 km along ODr9 (Figure 10c), we were able to explain the observed travel times with an error of less than 0.2 s (except at offset 210 to 240 km for OBS 115, where the error was 0.3 s). Finally, we compared the observed record sections with synthetic seismograms and confirmed large amplitude signals at offsets of over 180 km. That is, a velocity discontinuity at a depth of about 45 km under the plateau is proposed as one of possible interpretations for these signals. Furthermore, similar reflection signals were recorded by several OBSs at OKr4. In the same way, we estimated the position of the interface at a depth of about 50 km with a horizontal width of about 60 km beneath the Oki-Daito Rise.
Discussion and conclusion
We have compiled Vp structural models from ten wide-angle seismic lines in the Daito Ridges region at the northwestern end of the Philippine Sea plate. The crustal models obtained for the Amami Plateau (Figure 3) and the Daito Ridge (Figures 5 and 6a) are similar. In both cases, there is an upper crust with Vp of 3.0 to 6.3 km/s and a middle crust with Vp of 6.3 to 6.8 km/s below the ridges, although their relative proportions vary along the seismic lines. The lower crust and upper mantle seismic velocities are 6.8 to 7.2 and 7.6 to 7.9 km/s, respectively. The maximum crustal thickness beneath the bathymetric highs reaches approximately 20 km.
The Kita-Daito Basin is situated between the Amami Plateau and Daito Ridge (Figure 1) and has a thin crust of 4 to 6 km, as deduced from its seismic structure (Nishizawa et al. 2013). The top of the middle crust of the Amami Plateau (Figure 3) tends to shallow southward of the Kita-Daito Basin, particularly in the mid-row bathymetric high along DAr2. A notable feature of the Daito Ridge crust is that a material with Vp ≤ 6.3 km/s and a thickness of 6 to 11 km is concentrated in the southern part, while a material with Vp ≥ 6.3 km/s ascends closer to the seafloor toward the Kita-Daito Basin in the north. The middle crust beneath both the Amami Plateau and the Daito Ridge shallows towards the Kita-Daito Basin, which may be the result of extension between the two bathymetric highs. However, instead of an ascending middle crust, Canales et al. (2008) report that a deeper crust consisting predominantly of gabbro was exhumed at several oceanic core complexes, which are large-offset normal fault systems commonly referred to as oceanic detachment faults on the Mid-Atlantic Ridge.
A much thinner crust, with a thickness of approximately 3 km and a high Pn velocity of 8.3 km/s, occurs at the transition from the Daito Ridge to the Kita-Daito Basin. This crust shows the same characteristics as that found at the transition between the Kyushu-Palau Ridge and the Shikoku and Parece Vela Basins, where backarc spreading had occurred (Nishizawa et al. 2012). The Vp model of the Kita-Daito Basin suggests the presence of a thinner crust, similar to the backarc basin oceanic crust in the Shikoku and Parece Vela Basins, as revealed by Nishizawa et al. (20112013). These features lend credence to the interpretation of rifting and seafloor spreading between the Amami Plateau and Daito Ridge, which is supported further by roughly east-west aligned magnetic anomalies in the Kita-Daito Basin (Figure 2c) that imply seafloor spreading in the north-south direction. By contrast, Kasuga et al. (1986) interpreted these lineations to be related to topographic relief. Moreover, although Tokuyama et al. (1986) proposed that the backarc spreading of the Kita-Daito Basin was caused by subduction at the southern edge of the Daito Ridge, our seismic profiles do not contain any distinctive features indicative of subduction.
Individually, Vp models for the three sub-regions of the Oki-Daito Ridge in the broad sense reveal different features (Figures 8a and 9a). The Oki-Daito Plateau has the thickest crust (20 to 25 km) of these sub-regions (Figure 9a). This comprises an upper crust with Vp of approximately 3.0 to 6.3 km/s, a middle crust with Vp of 6.3 to 6.8 km/s, and a lower crust with Vp of 6.8 to 7.2 km/s, which is a similar structure to that of the Daito Ridge crust. In contrast, the Oki-Daito Rise in the southwestern part of the ridge has a relatively thin middle crust, reaching a maximum total crustal thickness of 14 km, which is different from other bathymetric highs in the Daito Ridges as well as from typical oceanic crust.
A deep reflector was identified at approximately 45 km below the sea floor between the Oki-Daito Rise and Plateau (Figure 10). The detection of such deep reflectors requires a sufficiently long seismic line as well as closely placed shots and receivers, although we do not presently have sufficient data to discern the spatial distribution of these reflectors in the Daito Ridges region. In addition, most seismic refraction lines performed in previous studies did not reach the required offsets. Kaneda et al. (2010) found deeper reflectors at a depth of 35 to 45 km beneath seamounts with a hot spot origin in the northwestern Pacific Basin. They inferred that these reflectors indicate structures that formed via intraplate igneous activities, such as at the top of a mantle partial melting zone or a remnant of a hot spot plume head. OIB rock samples obtained from the Oki-Daito Ridge in the broad sense were different from the samples collected from the Amami Plateau and Daito Ridge (e.g., Ishizuka et al. 2013). The existence of a deep reflector may therefore indicate intraplate volcanic activity in this region, although further investigation is required in order to confirm this interpretation.
The Oki-Daito Ridge shows a narrower ridge topography compared to the Oki-Daito Plateau and the Oki-Daito Rise; however, it has a thicker crust of 20 to 23 km (Figure 8a). The top of the middle crust, which has Vp of 6.3 to 6.8 km/s, is shallower beneath the northeastern bathymetric high. Slightly thinner crust and a notably higher Pn velocity were measured at the boundary between the ridge and the Minami-Daito Basin to the north along the KPr15 and DAr5 seismic lines. Apparently, a similar structure was found at the north of the Daito Ridge, where rifting is inferred. However, neither thin crust nor high Pn velocities were clearly observed at the transition from the Minami-Daito Basin along ODr5. The Pn velocity obtained beneath the Minami-Daito Basin varies between around 7.7 and 8.2 km/s and is locally higher than 8.0 km/s (Nishizawa et al. 2013). Therefore, the shallower and thicker middle crust beneath the northeastern side of the ridge may be related to the bathymetric high that was presumably produced by OIB activity 44 to 48 Ma ago (Ishizuka et al. 2013). While the linear valley topography suggests rifting along the ridge, the velocity models do not show obvious axial symmetry. To confirm this feature, additional profiles across the ridge with symmetrical seafloor topography are needed.
Although large variations in crustal structure exist across the study area, though the crustal model for the Oki-Daito Rise constitutes an exception, we can summarize our results as follows. The Vp models obtained for the bathymetric highs in the Daito Ridges region generally correspond to a middle crust with Vp of 6.3 to 6.8 km/s, a lower crust with Vp of 6.8 to 7.2 km/s, a Pn velocity of 7.6 to 7.8 km/s, and a total crustal thickness of 15 to 25 km. Rock samples obtained from these Daito Ridges bathymetric highs indicate that most of them have originated from island arcs (e.g., Hickey-Vargas 2005;Ishizuka and Yuasa 2007;Ishizuka et al. 2013).
In contrast, the Vp structure of the IBM island arc (an immature intra-oceanic island arc) is characterized by a middle crust with Vp of 6.0 to 6.8 km/s, a lower crust with Vp ≥ 7.0 km/s at its base, and an uppermost mantle with Vp < 8.0 km/s (e.g., Suyehiro et al. 1996;Nishizawa et al. 2006;Takahashi et al. 2007). We compared our Vp models for the Daito Ridges with those for several intra-oceanic island arcs near Japan (Figure 11). The Vp models of the Daito Ridges show a closer match to those of the IBM arc and Kyushu-Palau Ridge, which are immature paleo-island arcs, than they do to those of the mature Japan island arc. Moreover, the velocities of the middle and lower crusts are not as high as those of the Aleutian arc, which may be a result of extension and rifting in this region (Calvert 2011). Future studies on S wave velocity structure are expected to provide more information about the material properties of these paleo-island arcs.
The authors gratefully acknowledge Prof. Emeritus J. Kasahara, Dr. R. Kubota, and the members of the Continental Shelf Surveys Co. Ltd. for the data processing and analysis. Discussions with Y. Ohara, K. Tani and T. Morishita were valuable. We thank the two anonymous reviewers for their insightful comments. The authors are also grateful to the members of the Hydrographic and Oceanographic Department, JCG for the management of the seismic surveys.
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