Open Access

A revised spreading model of the West Philippine Basin

Earth, Planets and Space201466:83

https://doi.org/10.1186/1880-5981-66-83

Received: 7 April 2014

Accepted: 29 July 2014

Published: 4 August 2014

Abstract

The West Philippine Basin (WPB) occupies the western part of the Philippine Sea (PHS) plate. The WPB is generally considered to have opened from approximately 50 to 30 Ma at the CBF rift; however, the detailed spreading history of the WPB is not yet clear. In particular, the origin and age of the southern subbasin, the Palau Basin, are unknown. To better understand the initiation and early evolution of the Izu-Bonin (Ogasawara)-Mariana arc, knowing the configuration of the PHS plate at that time is necessary. In this study, we examine the spreading history of the WPB using newly acquired three-component magnetic anomaly and swath bathymetry data, as well as existing datasets. In the WPB south of the CBF rift, the observed magnetic anomalies correspond to Chron C16r to C21n (approximately 36 to 46 Ma). Prevailing models of the WPB reconstruction show a decrease in the spreading rate from 4.4 to 1.8 cm/year since C18n.2n (approximately 39.5 Ma). Our research, however, indicates that the change in the spreading rate is not required to correlate the observed magnetic anomalies to the geomagnetic polarity reversal timescale. The age of the spreading cessation in our interpretation, approximately 36 Ma, is several million years older than in previous estimates, and the spreading ceased progressively from southeast to northwest along the CBF rift. In the Palau Basin, seafloor fabrics and magnetic lineations trend N-S, which indicates E-W seafloor-spreading. Based on 40Ar/39Ar age, we suggest that the magnetic lineations correspond to polarity reversals from C18n.1n to C15r (approximately 38.5 to 35 Ma). The spreading of the Palau Basin may have been coeval with that of the WPB near the CBF rift, although their spreading directions are different.

Keywords

Magnetic anomaly Topography West Philippine Basin Palau Basin Seafloor spreading

Correspondence/Findings

Introduction

The West Philippine Basin (WPB) (Figure 1) occupies the western part of the Philippine Sea (PHS) plate. The WPB is generally considered to have formed by seafloor spreading during approximately 50 to 30 Ma, prior to the opening of the Shikoku and Parece Vela Basins; however, partly because of its structural complexity and the scarcity of modern geophysical data in the southern part of the WPB, the exact details of its formation are not yet clear despite a long history of studies (e.g., Hess1948; Uyeda and Ben-Avraham1972; Karig1975; Hilde and Lee1984; Deschamps and Lallemand2002; Taylor and Goodliffe2004). In particular, the southern subbasin, called the Palau Basin by Taylor and Goodliffe (2004), has been rarely studied, and its origin and age remained unknown. Recently, the initiation and evolution of the Izu-Bonin (Ogasawara)-Mariana arc have attracted considerable interest as a typical example of an oceanic island arc (e.g., Ishizuka et al.2006a,[b]). For a better understanding of the evolution of this arc, knowing the configuration of the PHS plate at that time is necessary. Thus, studies on the development history of the WPB are important.
Figure 1

Shaded relief map of the Philippine Sea plate and its vicinity. The gridded topography ETOPO1 derived from satellite altimetry (Sandwell and Smith1997) was used. Magnetic anomaly lineations are modified after Hilde and Lee (1984) (black) and Taylor and Goodliffe (2004) (brown and blue). ODE, Oki-Daito Escarpment.

The WPB is bounded on the east side by the Kyushu-Palau Ridge and the north side by the Oki-Daito Ridge (Figure 1). The WPB is subducting northwestward underneath the Ryukyu-Taiwan-Philippine arcs and controls volcanic activity there (e.g., Sato et al.2014). The NW-SE trending CBF rift (previously called the Central Basin Fault) in the central part of the WPB is considered to be a fossil spreading axis (e.g., Uyeda and Ben-Avraham1972; Louden1976; Fujioka et al.1999; Deschamps et al.2002). The depth of the basin ranges from 5,500 to 6,000 m, which is deeper than the depth expected from the standard age-depth curve, but in accord with the curve derived for back-arc basins (Park et al.1990). Several attempts have been made to identify magnetic anomalies based on total-force anomalies in the 1970s and 1980s. Louden (1976) and Mrozowski et al. (1982) identified anomalies 21 to 17 (approximately 47 to 37 Ma, according to the timescale of Gradstein et al. (2004)). Shih (1980) identified anomaly 7A (approximately 25 Ma) for the youngest age near the CBF rift, anomaly 21 (approximately 47 Ma) for the oldest age in the northern part of the WPB, and anomaly 25 (approximately 57 Ma) for the oldest age in the southern part of the WPB. These authors assumed a constant NE-SW spreading. Hilde and Lee (1984), on the other hand, proposed that the WPB was formed by two phases of spreading: one between anomalies 26 and 19 (approximately 59 to 40 Ma) in a NE-SW direction at a half-rate of 4.4 cm/year and another between anomalies 18 and 13 (approximately 40 to 33 Ma) in a N-S direction at a rate of 1.8 cm/year. PHS plate reconstructions (e.g., Hall et al.1995; Hall2002; Deschamps and Lallemand2002) are based on the interpretation of Hilde and Lee (1984), with the exception of the revision made in the region north of the Oki-Daito Escarpment by Deschamps and Lallemand (2002).

The Palau Basin is separated from the main WPB by a fault zone, the Mindanao Fracture Zone (MFZ) (Figure 1). Taylor and Goodliffe (2004) showed that the MFZ is composed of multiple curvilinear strands. The water depth of the Palau Basin floor (approximately 5,500 m) is shallower than in the rest of the WPB north of the MFZ (approximately 5,500 to 6,000 m), and the pelagic sediment cover is thicker (Mrozowski et al.1982). Hilde and Lee (1984) assigned anomalies 26 and 25 (approximately 59 to 56 Ma) inside the Palau Basin without considering the presence of the MFZ, which may represent a structural boundary. To date, no radiometric dating of seafloor rocks from the Palau Basin has been reported.

In this study, we compile and analyze bathymetry and magnetic anomaly data collected in the southern part of the WPB over the last decade by the Japan Agency for Marine-Earth Science and Technology (JAMSTEC). Moreover, we include recent data acquired during the R/V Yokosuka YK10-14 cruise in 2010. We reexamine magnetic lineations in the WPB, including the Palau Basin, taking the advantage of using a shipboard three-component magnetometer (STCM) (Isezaki1986). We then present a revised spreading history of the WPB, including the formation of the Palau Basin.

Data and methods

Bathymetric and magnetic data were collected mainly in the Palau Basin during the R/V Yokosuka YK10-14 cruise. We also used datasets available at the JAMSTEC data portal (http://www.godac.jamstec.go.jp/dataportal/), which mainly consists of data obtained by R/V Mirai between 2000 and 2010 (see Additional file1 for the list of used datasets). SeaBeam 2112 multi-narrow-beam echo sounders were used for bathymetry on all cruises. For magnetic anomaly measurements, STCMs with ring-laser gyros were used during the YK10-14 cruise and for the datasets of the R/V Mirai cruises. A towed proton magnetometer was also employed during the YK10-14 cruise.

We basically followed the method of Isezaki (1986) for the measurement and data reduction using STCM. The magnetic anomaly data were subjected to long wavelength variations that are supposed to be caused by diurnal variations of the geomagnetic field as well as changes in the ship's magnetization with time - which we assumed to be constant. To rectify these variations, individual components of the observed magnetic data were filtered with a band-pass filter after removing a linear trend; variations with wavelengths from about 4.5 to 180 km were passed. Strikes of magnetic boundaries were determined for each survey line based on variation patterns of both vertical and horizontal components and the intensity of spatial differential vectors (ISDV) (Seama et al.1993). Boundary strikes with uncertainties larger than 20° or boundaries with deviation from the vertical larger than 20° were considered unreliable and rejected because they may not be related to two-dimensional structures.

Results

Swath bathymetry and magnetic anomaly profiles of the north component along survey lines in the WPB between the CBF rift and MFZ are shown in Figure 2, where they are superimposed on a topographic map derived from the satellite altimetry (Sandwell and Smith1997). The strikes of magnetic boundaries at each peak in ISDV were calculated and are shown on the magnetic anomaly profiles. The trend of abyssal hills is close to E-W near the CBF rift. Toward the south, approaching the MFZ, the trend progressively changes to NW-SE (Figures 2 and3c, Additional file2). The strikes of magnetic boundaries support the change of the spreading direction. Magnetic anomaly patterns are well correlated among survey lines (Figures 2 and3b) and indicate WNW-ESE trending magnetic lineations. At around 10.5° N, 130° E, the NW-SE magnetic boundary strike (orange bar in Figure 2) is inconsistent with the others; it is instead associated with the change in the orientation of the seafloor fabric (Figure 2, Additional file2). This may be a consequence of rift propagation, which is known to have frequently occurred in the northern part of the WPB (Deschamps et al.2008). In the southernmost part of the basin between 8° and 10° N, topography displays complex fabrics, and magnetic anomalies do not show coherent variations among survey lines (Figures 2 and3b,c).
Figure 2

North-component magnetic anomaly profiles in the WPB between the CBF rift and Mindanao Fracture Zone. Magnetic boundary strikes calculated from three-component anomalies are displayed with colored bars. Superimposed are shaded topographic relief based on the ETOPO1 grid and swath bathymetry along survey lines. See Additional file2 for a shaded relief map without magnetic profiles.

Figure 3

Correlation of the observed and synthetic magnetic anomaly profiles in the West Philippine Basin. The vertical-component anomalies are presented. (a) Synthetic magnetic anomaly profile assuming a half spreading rate of 1.8 cm/year, (b) observed anomaly profiles, (c) shaded topographic relief along 130° E from swath bathymetry data, and (d) synthetic profile assuming a half spreading rate of 4.4 cm/year. Skewness of 160°, magnetization intensity of 2.5 A/m, and magnetized layer top depth of 6 km and thickness of 1 km were assumed. The geomagnetic polarity timescale of Gradstein et al. (2004) is used. See Figure 2 for the locations of the magnetic profiles. Color scale of the shaded topographic relief is the same as Figure 2.

A topographic relief map of the Palau Basin is displayed in Figure 4. Although the Palau Basin is covered with relatively thick sediments, abyssal hills trending N-S to NNW-SSE are well expressed in the central part. When approaching the Philippine Trench to the west, the trend of abyssal hills gradually changes to NNE-SSW. Figure 5 shows the three-component and total-force magnetic anomalies along three E-W survey lines (lines 17, 19, and 21). The variations in the east and vertical components are larger than those in the north component, suggesting the presence of nearly N-S striking magnetic lineations. The amplitudes of total-force anomalies are small (Figure 5d), which is consistent with the occurrence of N-S striking magnetic lineations in low latitudes. Although the original configuration of the Palau Basin is not known, PHS plate motion models suggest a large clockwise rotation since the Eocene and that the Palau Basin was in low latitudes south of the equator at approximately 40 Ma (Hall et al.1995; Deschamps and Lallemand2002). Good agreement of anomaly patterns among the survey lines and nearly N-S magnetic boundary strikes also support the occurrence of E-W seafloor spreading.
Figure 4

Shaded relief map of the Palau Basin and Mindanao Fracture Zone (MFZ). The ETOPO1 grid and swath bathymetry data along ship tracks were used. The vicinity of the MFZ is enlarged, and a red cross indicates the locality of dated basalt (Ishizuka et al. in prep.). Red lines show survey lines of three-component magnetic anomaly shown in Figure 5.

Figure 5

Magnetic anomaly profiles in the Palau Basin. (a) The north, (b) east, and (c) vertical component anomalies and (d) total-force anomalies. Magnetic boundary strikes calculated from the three-component anomalies are shown on (c) (red bar). Shaded relief topography from the ETOPO1 grid and swath bathymetry data along survey lines are superimposed. Color scale is the same as Figure 4.

Magnetic anomaly interpretation

Spreading model of the West Philippine Basin south of the CBF rift

Comparisons between the observed magnetic anomalies and predictions from two-dimensional block models are shown in Figure 3 for the vertical component (see Additional file3 for the north component). The block models with skewness of approximately 150° to 180° fit the observation, which agrees with the findings of previous studies (Louden1976; Shih1980; Mrozowski et al.1982; Hilde and Lee1984). We tested two spreading scenarios: one assumes a constant spreading rate of 4.4 cm/year, while the other supposes two-phase spreading as proposed by Hilde and Lee (1984), which is a decrease in the spreading rate from 4.4 to 1.8 cm/year at the beginning of C18n.2n (39.46 Ma).

Characteristic anomaly patterns between the boundaries of C21n/C20r and C19n/C18r (45.35 to 40.44 Ma) are well correlated among all survey lines and agree with the predicted anomalies for the both components. This is consistent with the previous identification of anomalies 21 to 19 (Louden1976; Shih1980; Mrozowski et al.1982; Hilde and Lee1984). In older areas between approximately 10° N and the MFZ, however, correlating the observed and predicted anomalies is difficult, where seafloor fabrics are complex (Figures 3 and4, Additional file2). According to the constant spreading model, magnetic polarity reversals between the boundaries of C19n/C18r and C17n.1n/C16r (40.44 to 36.51 Ma) show good agreement with the observed anomalies between approximately 14.5° and 16° N. According to the two-phase spreading model, the observed anomalies may correspond to magnetic polarity reversals between the boundaries of C18r/C18n.2n and C13n/C12r (39.46 to 33.27 Ma); however, the correlation is ambiguous. Complex seafloor fabrics were observed between approximately 15.5° and 14.5° N along 130° E (Figures 2 and3c). Magnetic anomaly patterns observed over this area are somewhat irregular compared to the areas located to the south and north. According to the constant spreading model, the half spreading rate in the studied area is approximately 8 cm/year at C20r (45.35 to 42.77 Ma) and approximately 6 cm/year after the C20n/C20r boundary (42.77 Ma).

Magnetic lineations in the Palau Basin

Age estimation of the Palau Basin is not straightforward because no radiometric age data is available for basement rocks in the vicinity of the three E-W survey lines. In addition, the length of these lines is insufficient for unique magnetic anomaly identification. Further complexity comes from that we do not know whether the studied area constitutes the eastern or western limb of a spreading center. Ishizuka et al. (in preparation) obtained a radiometric age, 40.4 Ma, from basalt collected at a cliff in the MFZ, where the basement of the Palau Basin is considered to be exposed (Figure 4). We investigated the possibility of temporal correlation with the geomagnetic polarity time scale around 40 Ma because the longitude of the locality of the dated basalt and the western end of the survey lines are almost the same. An E-W spreading direction is inferred based on the N-S abyssal hill trend. We examined two cases: the eastern and western limbs of a spreading ridge. In the case of the eastern limb, the observed anomalies in the east and vertical components reasonably fit the predicted anomalies from C18n.1n (approximately 38.5 Ma) to the end of C15r (approximately 35 Ma) (Figure 6). This implies a half spreading rate of approximately 4.3 cm/year, which is slightly slower than that of the WPB. In this model, we adopted skewness of 90°, which was derived from the remanent declination (D r ) and inclination (I r ) of 60° and 0°, respectively. The D r of 60° incorporated a large clockwise rotation of the PHS plate since the Eocene (Hall et al.1995; Deschamps and Lallemand2002). The ambiguity in D r does not affect the magnetic anomaly interpretation because changes in D r between 30° and 90° cause skewness variations of only several degrees. PHS plate motion models suggest that the paleolatitude of the Palau Basin at approximately 40 Ma was between the equator and 10° S (Hall et al.1995; Deschamps and Lallemand2002). When an I r of -20° is adopted, the skewness becomes 110°, which does not significantly affect our interpretation. A skewness of 90° produces no anomaly in the north component, which is consistent with the observation. In the case of the western limb, no correlation was found.
Figure 6

Correlation of the observed and synthetic magnetic anomaly profiles in the Palau Basin. (a) The east-component anomalies and (b) the vertical-component anomalies. Half spreading rate of 4.4 cm/year, skewness of 90°, magnetization intensity of 2.5 A/m, and magnetized layer top depth of 6 km and thickness of 1 km were assumed.

Discussion

We have successfully correlated observed magnetic anomalies in the WPB with predictions from the geomagnetic polarity reversal timescale. The three-component magnetic measurements enabled us to identify magnetic lineations more efficiently than total-force measurements. The amplitude of total-force anomaly is reduced in low latitudes depending on the geometry of two-dimensional magnetized bodies, which is not the case in three-component anomalies. In addition, a consistency check among the individual components can provide a stronger constraint on magnetic anomaly interpretation than in the case of only total-force anomaly.

Our magnetic lineation identification between the boundaries of C21n/C20r and C19n/C18r (45.35 to 40.44 Ma) in the WPB south of the CBF rift is consistent with previous studies based on total-force anomalies (Louden1976; Shih1980; Mrozowski et al.1982; Hilde and Lee1984). The counter-clockwise topographic fabric change over time is consistent with previous observations along a single line (Andrews1980; Taylor and Goodliffe2004) and similar to those described to the north of the CBF rift (Deschamps and Lallemand2002). Taylor and Goodliffe (2004) suggested that C20r fans southeastward and is much wider compared with its counterpart to the north of the CBF rift due to a ridge jump during C20r. However, the fan shape of C20r observed around 11° N, 130° E seems to be a local feature as it does not appear on the adjacent survey lines near 131° E (Figure 2). An offset accommodating the difference in spreading directions is inferred to occur between the two regions; thus, invoking the occurrence of a ridge jump is not necessary. Topographic fabrics in the oldest part of the basin, between 10° N and the MFZ to the south, are highly disorganized (Figures 2,3c, and4), and estimating ages based on magnetic anomalies is impossible. This is probably the result of frequent reorganizations of seafloor spreading by means of propagating rifts and overlapping spreading centers during an incipient stage of back-arc basin formation. Tectonic stresses caused by the activity of the MFZ may also be responsible for the complexities.

For magnetic lineation identification, we considered both constant spreading and two-phase spreading. Our results indicate that magnetic anomalies can be well explained without introducing a spreading rate change (Figure 3). In particular, detailed structures within C17 fit remarkably well with the observation based on a constant spreading model; agreement with the model prediction is better than that using a reduced spreading rate of 1.8 cm/year. As per the data available to them, Hilde and Lee (1984) adopted the two-phase spreading model mainly because they believed that the roughness of the seafloor increases near the CBF rift. This was interpreted as a slower spreading rate. The area between approximately 14.5° and 15.5° N near 130° E is such an example; however, this may have been caused by the reorganization associated with slight changes in the spreading direction rather than a slower spreading rate (Deschamps et al.2002,2008). Okino and Fujioka (2003) described long-lasting discontinuities extending from the CBF rift to the northern and southern WPB along with pseudo-faults related to eastward ridge propagations. Furthermore, the CBF rift may have been reactivated after the cessation of spreading (Fujioka et al.1999). Thus, the seafloor roughness near the CBF rift does not necessarily reflect a change in the spreading rate.

According to our results, the cessation of spreading at the CBF rift is estimated to have occurred at approximately 36 Ma near 130° E, which is older than the 30/33 Ma estimation using the two-phase spreading model (Hilde and Lee1984; Deschamps and Lallemand2002). It appears that the spreading ceased progressively from southeast to northwest along the CBF rift; at 15° N, 133° E, the cessation occurred at approximately 37.5 Ma (line MR02-K04), and at approximately 35.5 Ma at 16.5° N, 130° E (line MR06-05) (Figure 3). The northwestward waning of the spreading is consistent with the hypothesis that the spreading at the CBF rift was triggered by the Oki-Daito mantle plume in the western part of the WPB (Ishizuka et al.2013). Hilde and Lee (1984) proposed almost uniform cessation ages along the CBF rift; however, even based on such a two-phase spreading model, the cessation was earlier in the eastern part (Figure 3). Volcanic and tectonic activities may have continued until approximately 15 Ma at the CBF rift, which is much later than the cessation of spreading (Fujioka et al.1999; Deschamps et al.2002). Similar post-spreading volcanism is known to have occurred at the extinct spreading axis (the Kinan Seamount Chain) after the cessation of spreading in the Shikoku Basin (Ishizuka et al.2009).

Our results indicate that the Palau Basin was formed by E-W seafloor spreading, between approximately 35 to 39 Ma with a half rate of approximately 4.3 cm/year, which is slightly slower than that of the WPB. The estimated age of the Palau Basin is close to that of the younger part of the WPB near the CBF rift. This implies that the age of the seafloor just north of the MFZ is considerably older than that of the Palau Basin, which is consistent with the observation that the water depth of the Palau Basin is shallower than in the main part of the WPB. We speculate that the spreading center of the main part of the WPB and that of the Palau Basin were originally parallel and in the N-S direction; the former center then rotated counterclockwise along the MFZ. Our estimated age difference of approximately 5 Ma and average spreading rate of 4.3 cm/year require left-stepping offsets of about 200 km in total between the magnetic survey lines at approximately 6° N and the MFZ at approximately 8° N. Due to the sediment cover, identifying any topographic feature that would indicate the occurrence of these offsets is difficult. Further measurements of three-component magnetic anomalies along longer survey lines associated with the dating of basalts are required to confirm our model.

Declarations

Acknowledgements

We thank all onboard scientists, officers, and crew of the YK10-14 cruise of R/V Yokosuka for the cooperation. We also thank Hiromi Fujimoto of Tohoku University for making us available for the ring laser gyro and Nobukazu Seama of Kobe University for the three-component magnetometer during the YK10-14 cruise. The manuscript was greatly improved by constructive comments of two anonymous reviewers. This research was supported by a Grant-in-Aid for Scientific Research ((C) No. 22540473) from the Japan Society for the Promotion of Science. The GMT software (Wessel and Smith1995) was used for processing the data and producing the figures.

Authors’ Affiliations

(1)
Graduate School of Life and Environmental Sciences, University of Tsukuba
(2)
Geological Survey of Japan, AIST
(3)
Atmosphere and Ocean Research Institute, University of Tokyo

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© Sasaki et al.; licensee Springer. 2014

This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.