The 2011 Tohoku Earthquake
- Open Access
InSAR-derived crustal deformation and fault models of normal faulting earthquake (Mj 7.0) in the Fukushima-Hamadori area
Earth, Planets and Space volume 64, Article number: 15 (2012)
Applying interferometric SAR (InSAR) analysis using ALOS/PALSAR data to inland crustal earthquakes in the Fukushima-Hamadori area, we succeeded in mapping a ground displacement associated with the Mj 7.0 earthquake that occurred on 11 April, 2011. The most concentrated crustal deformation is located ~20 km west of the city of Iwaki, showing displacements away from the satellite with ~2.2 m at the maximum. Clear displacement discontinuities are recognized with an offset of ~1.6 m at the maximum, which are just on the Shionohira, Idosawa and Yunotake faults. From field surveys, we found that earthquake surface faults appeared with a vertical offset of ~1.9 m, consistent with the InSAR observation, and their locations correspond to the discontinuities in the interferogram. We inverted the InSAR data to construct slip distribution models, and our models show (1) nearly pure normal fault motions (2) on west-dipping planes (3) with moderate-dip-angles (50–65°). The inferred west-dipping normal fault motion on the Yunotake fault is correlated with the present-day topographic features, consistent with the idea that the historically-repeated normal faultings have developed the topography. On the other hand, for the Shionohira and Idosawa faults antithetical relationships are presented, maybe suggesting that large normal faultings have been infrequent historically.
A megathrust earthquake with a moment magnitude (Mw) of 9.0 occurred on 11 March, 2011 (JST), rupturing the plate boundary on the east off northeastern Japan (Ozawa et al., 2011). Following the Mw 9.0 event, many inland crustal earthquakes occurred in addition to aftershocks on the plate boundary (Hirose et al., 2011). The Fukushima-Hamadori area and the surroundings are one of the regions where the seismicity drastically changed from a quiescent stage to an active stage. In this region, the crustal deformation rate is not so high and the region had been seismically inactive. No earthquakes exceeding a JMA (Japan Meteorological Agency) magnitude (Mj) 4.0 have occurred in the crust during the ten years prior to the Mw 9.0 event. However, more than 20 earthquakes exceeding Mj 5.0 have already occurred since the Mw 9.0 event, as of December, 2011 (Fig. 1). The timing of the seismicity activation suggests a possible causal relationship with the Mw 9.0 event. It is further striking that most of the earthquakes are of a normal fault type, which is not a typical type for the region of reverse/strike-slip motions reflecting the plate loading in an east-west direction. The crust along the coastal northeastern zone of Japan is considered to be subjected to a strong extensional stress change due to the reverse fault slip of the Mw 9.0 event and the subsequent afterslip, which presumably culminates in the promotion of a normal-fault slip.
On 11 April, 2011, a large inland earthquake, with Mj 7.0, struck the Fukushima-Hamadori area. This is the largest event among the inland crustal earthquakes since the Mw 9.0 event, as of the time of writing. The seismic data analyses show that the source mechanism is also a normal fault type, but this event seems to be rather complicated in that the rupture style cannot be accounted for by a slip on a single fault plane. This is because several earthquake surface faults appeared with (sub)meter order, suggesting that seismic ruptures proceeded on multiple fault planes. Despite the several such outstanding features of this event, however, it remains uncertain where and how the faults were involved in the seismic event. Obtaining detailed crustal deformation data and constructing fault models are crucial to understanding the unclear points.
Satellite synthetic aperture radar (SAR) data can provide detailed and spatially-comprehensive ground information, and an interferometric SAR (InSAR) enables us to measure ground deformation with high precision (e.g., Massonnet and Feigl, 1998; Bügmann et al., 2000). One of the advantages of InSAR observation is that local crustal deformation can be detected. Although GNSS sites (GEONET) are densely deployed with an average placement interval of ~20–30 km nationwide, it remains difficult to obtain high quality displacement data for small- to moderate-sized earthquakes, impeding detailed analysis of the source properties, such as fault modeling. Alternatively, the ground resolution of SAR data (ALOS/PALSAR) is ~10 m, and the InSAR observation works well to detect small- to moderate-sized ground deformation anomalies over a large area.
To obtain a further understanding of where and how ruptures proceeded in the Mj 7.0 event, for which a complicated source process is expected from the field survey, the SAR data analyses surely contribute to provide detailed and vital information regarding surface changes quantitatively. The primary aim of this paper is to understand the source properties of the Mj 7.0 event by constructing an elaborated fault model using InSAR-derived crustal deformation data. We first describe the SAR data analysis procedure in Section 2. In Section 3, we describe the characteristics of the crustal deformation associated with the inland crustal earthquakes; in particular, regarding displacement discontinuities corresponding to surface ruptures. On the basis of the InSAR data, we construct fault models using a rectangular fault plane with a uniform slip in Section 4. In Section 5, we construct a slip distribution model for the Mj 7.0 event by an inversion approach. Finally, in Section 6, we discuss the reliability of our derived slip distribution model, the relationship between the inferred fault motions and the present-day topographic features, and the effect of mainshock fault rupture on other fault ruptures.
2. SAR Data Analysis
We collected ALOS/PALSAR images to reveal the crustal deformation due to the earthquake that occurred in Fukushima-Hamadori area. In Japan, many faults, including the seismic source we now study, are located in mountainous areas with a vegetated environment, and thus the PALSAR’s L-band sensor should be a powerful tool for geodetic observation to extract ground information, even in mountains. JAXA (Japan Aerospace Exploration Agency) carried out urgent observations for the great earthquake (Mw 9.0) on 20 March (path 404), 7 April (path 56), and 18 April (path 403) with a fine beam mode, and on 14 March (path 60) and 31 March (path 61) with a ScanSAR mode, respectively, which covers our study area. Among them we used three paths of fine beam mode for the interferometric analysis, because the interferometric coherence of the obtained images using ScanSAR was too low to detect ground displacements, which may have resulted from large perpendicular baselines (~2 km and ~5 km). ALOS had completed its mission on 12 May, 2011, due to a power generation anomaly that occurred on 22 April, 2011. Thus, no image had been acquired since the date. The ALOS/PALSAR data was processed using GSISAR software (Fujiwara and Tobita, 1999; Fujiwara et al., 1999; Tobita et al., 1999; Tobita, 2003).
Obvious long-wavelength phase changes caused by the Mw 9.0 event were included in the original interferograms (Imakiire and Kobayashi, 2011). To pick up the crustal deformation due to the inland earthquakes, we assumed that the far-field displacement was zero and that the residual phases were expressed by a quadratic surface, and we subtracted the evaluated bilinear function from the original interferogram. We use the residual phase changes as the crustal deformation data associated with the inland earthquakes.
3. Crustal Deformation Map
3.1 Characteristics of ground surface displacement
Figure 2 shows the interferogram obtained from the ascending orbit data of path 403 acquired before, and after, the Mj 7.0 event (3 March, 2011–18 April, 2011). The crustal deformation is distributed over an ~40–50-km range, showing displacements away from the satellite. The most concentrated crustal deformation is located ~20 km west of the city of Iwaki. A maximum displacement of ~2.2 m is observed at point A (Fig. 2). In the further west of the intensive deformation area showing slant range lengthening, in contrast, small but clear slant range shortening signal is observed with ~10 cm. The importance of the shortening for the fault modeling is discussed later. Active faults, referred to as Shionohira, Idosawa and Yunotake faults, exist in the deformation area (Research Group for Active Faults of Japan, 1991; Ishiyama et al., 2011). This presumably suggests that these faults contributed to the seismic ruptures of the Mj 7.0 event in some way. The relationship with the active faults will be described in the next section.
We stress that we succeeded in obtaining the phase change map with high coherence for the whole source region. Some large inland earthquakes had lost the interferometric coherence significantly in the vicinity of the hypocentral area because of serious changes in the scattering conditions on the ground and too high displacement gradients—e.g., the 2008 Iwate-Miyagi Nairiku earthquake (Takada et al., 2009)—which impeded estimates of detailed crustal deformation and source properties. In contrast, owing to the high coherence, the InSAR map of the Mj 7.0 event enables us to investigate the ground surface change over the entire source area in detail.
In addition to the Mj 7.0 event, additional crustal deformation is detected by the InSAR analyses using different SAR data pairs. Figure 3 shows interferograms obtained from the data acquired before the Mj 7.0 event. In the interferogram of Fig. 3(a), which is obtained from the SAR data pair of 2 February, 2011, and 20 March, 2011, we can recognize an ear-shaped displacement distribution, caused by the Mj 6.1 event that occurred on 19 March, 2011. The most concentrated crustal deformation is located ~10 km west of the city of Kitaibaraki, with a maximum slant range lengthening of ~40 cm. Figure 3(b) shows an interferogram obtained from the SAR data pair of 20 November, 2010, and 7 April, 2011. Crustal deformation due to the Mj 6.0 event (23 March, 2011), in addition to that of the Mj 6.1 event, can be clearly seen in the interferogram, located ~10 km west of the city of Iwaki. Comparing the two source regions to the active fault traces indicated by red lines, both seismic events seem to be irrelevant to known active faults. The corresponding phase changes are included also in the interferogram of Fig. 2, although the signal of the Mj 6.0 event appears together with the phase changes due to the Mj 7.0 event.
3.2 Displacement discontinuities corresponding to ground surface ruptures
It is notable that we can identify clear major and minor displacement discontinuities in the InSAR map (Fig. 2). In particular, three main displacement boundaries can be recognized with lengths of tens and several kilometers in the source region of the Mj 7.0 event, indicated by arrows. The discontinuity lines run just on the Shionohira, Idosawa and Yunotake fault traces. Figure 4(a) shows a profile of the line-of-sight (LOS) displacement along the cross-section line of X–X′ (Fig. 2). Displacement jumps can be seen at some points, which probably correspond to surface ruptures. The offsets strongly suggest that it is not a single fault rupture, but rather multiple ruptures which are involved in the seismic event. According to Hikima (2012), multiple shocks are recognized in the seismograms. The largest displacement offset is observed along the Shionohira fault. The maximum discrepancy across the discontinuity is approximately 1.6 m. On the other hand, the maximum offset for the Yunotake fault is observed as ~60–70 cm.
Figure 5 shows photographs taken at some points corresponding to the displacement discontinuities in the interferogram. The positions of photographs (A to F) are shown by white circles in Fig. 2. Field surveys reveal that earthquake surface faults appeared to be associated with the Mj 7.0 event, and we confirmed that the discontinuities in the interferogram do correspond to the surface ruptures. The photographs A and B, viewed from west and north, respectively, show that the hanging wall block drops down relative to the footwall one, which is of normal fault with west-dipping. From our field survey, the ground offset is measured to be approximately 1.9 m (photo A), equivalent to a LOS displacement of ~1.5 m. The maximum LOS displacement of the offset measured from the InSAR data agrees with the field observation.
The photographs C and D show the ground offsets taken at the Yunotake fault (Fig. 2), viewed from south and southeast, respectively. They also evidently show that the hanging wall block in the southwest drops down relative to the footwall one in the northeast, showing normal fault motions.
We also detected some surface cracks along the Idosawa fault in our field survey (Photo E). They suggest that some surface change did occur along the Idosawa fault as identified in the interferogram, but we were not able to infer the fault motion sense and/or amount of offset from the observed cracks.
In addition to the above-mentioned major discontinuities, we can identify several minor displacement boundaries with lengths of a few kilometers, which may not be seismic faults but so-called secondary faults. One of the minor discontinuities can be clearly seen in the cross-section of Fig. 4(a), indicated by a small arrow. A small, but clear, gap is detected. The gap is less than 10 cm. We can find out some cracks at, and around, the offset position (photo F), but they are not so clear that we can estimate the sense of ground movement.
Displacement discontinuities can be recognized associated with not only the Mj 7.0 event but also the Mj 6.1 and the Mj 6.0 events (arrows in Figs. 2 and 3). LOS displacement profiles show the clear gaps of ~10 cm for the Mj 6.0 event (Fig. 4(a)) and ~30 cm for the Mj 6.1 event (Fig. 4(b)). These suggest that significant fault ruptures occurred at a rather shallow depth, although there are no reports of the appearance of earthquake surface faults or surface cracks.
In, and around, the source regions, several GNSS sites are deployed, indicated by white squares (Figs. 2 and 3). Considering the size of the ground deformation, however, GNSS observations can hardly detect the locally-distributed ground anomalies such as the displacement boundaries. The detection of the displacement boundaries and an awareness of their spatial extent demonstrate the advantage of the InSAR analysis in that small- to moderate-sized ground deformation anomalies can be observed over a large area with a high spatial resolution.
4. Rectangular Fault Models with Uniform Slip for the Mj 7.0 and Mj 6.0 Events
On the basis of the obtained interferogram data, we first try to construct a fault model under the assumption of a rectangular fault with a uniform slip in an elastic half-space (Okada, 1985). A rectangular fault model has the advantage that it can represent a macroscopic feature of the source property with its simple notation. In the interferogram of the Mj 7.0 event, the phase changes associated with the Mj 6.1 and the Mj 6.0 events are included. The effect of the Mj 6.0 event, especially, is not negligible for the modelling of the Mj 7.0 event. Thus, we first construct the Mj 6.0 event model. The LOS displacements predicted by the two models are subtracted from the original interferogram, and then the residual is used for the modelling of the Mj 7.0 event. For the Mj 6.1 event, we used a fault model that had already been constructed by Kobayashi et al. (2011).
4.1 Mj 6.0 event on 23 March, 2011
The interferogram has ground surface changes over a range of several tens of kilometers, producing too many values to be easily assimilated in a modeling scheme. In order to reduce the number of data for the modelling analysis, we resampled the interferogram data beforehand, using a quadtree decomposition method. Essentially, we followed an algorithm presented by Jónsson et al. (2002). For a given quadrant, if, after removing the mean, the residue is greater than a prescribed threshold (1 cm in our case), the quadrant is further divided into four new quadrants. This process is iterated until either each block meets the specified criterion, or until the quadrant reaches a minimum block size (8 × 8 pixels in our case). Upon application of the above-mentioned procedure, the sizes of interferogram data sets were reduced from ~5.3 million to 1948. For the modeling, we applied a simulated annealing method for searching the optimal fault parameters (e.g., Cervelli et al., 2001). We randomly gave parameters within a search range of 140.75°–140.85° in longitude, 37.00°–37.10° in latitude, 0.1–10 km in depth, 1–10 km in length, 1–5 km in width, 180°–220° (0°–40°) in strike, 10°–90° in dip, − 130°–−50° in rake, and 0.1–2 m in slip amount, respectively. To estimate the individual confidence of inferred parameters, we employed a bootstrap method (Efron, 1979). We attempted a two-segment model in addition to the one-segment model. As a result, the AIC (Akaike’s information criterion) (Akaike, 1974) values support the one-segment model (AIC = −2776) rather than the two-segment model (AIC = −2619). Figure 6 shows the LOS displacement calculated using our preferred model and the residuals between the observations and the calculations. Our model is able to reproduce well the observations. The estimated fault parameters are listed in Table 1. Our fault model shows (1) a west-dipping fault plane with a dip angle of 67°, (2) a NS-oriented strike, and (3) a nearly pure normal fault motion. The seismic moment is estimated to be 7.88 × 1017 N m (Mw 5.9) with a rigidity of 30 GPa.
4.2 Mj 7.0 event on 11 April, 2011
We attempt to construct the rectangular fault model of the Mj 7.0 event. We downsampled the interferogram data from ~6.2 million to 5298 in the same manner as in the previous section. We assumed a two-segment model that consists of the Shionohira and Yunotake faults. We tried a three-segment model adding the Idosawa fault to the two-segment model, but the AIC estimate favored the two-segment model. For the parameter search of the Shionohira fault, we randomly gave parameters within a search range of 140.63°–140.69° in longitude, 36.97°–37.03° in latitude, 5–20 km in length, 1–10 km in width, 30°–90° in dip, −135°–−45° in rake, and 1–6 m in slip, respectively, while for the Yunotake fault, 140.73°–140.78° in longitude, 37.01°–37.04° in latitude, 5–15 km in length, 1–10 km in width, 30°–90° in dip, −135°–−45° in rake, and 0–5 m in slip, respectively. The strikes are fixed at the 160° (340°) and 130° (310°) for the Shionohira and the Yunotake faults, so as to fit to the averaged orientations of the displacement discontinuities, respectively. For the calculation, we attempted both west- and east-dipping faults. The appearances of the earthquake surface faults strongly suggest that significant slips occurred near the ground surface, thus we fix the fault top position at a depth of 0 km below sea level (bsl). Estimated fault parameters and their errors are listed in Table 2. The total seismic moment is estimated to be 1.45 × 1019 N m, equivalent to Mw 6.7 with a rigidity of 30 GPa (Shionohira fault: 9.20 × 1018 N m (Mw 6.6), Yunotake fault: 5.35 × 1018 N m (Mw 6.4). Our fault model shows that the slips are nearly pure normal fault motions with dip angles of ~60° and ~80° for the Shionohira and the Yunotake faults, respectively. For both the faults, west-dipping faults are preferable to eastones.
Figure 7 shows the LOS displacement calculated from the fault models and the residuals between the observations and the calculations. Despite the simple fault models with uniform slips on planar faults, our fault models are able to reconcile the spatial pattern of displacement distribution well, suggesting that the derived fault models macroscopically pick up the nature of the source. However, there still remains non-negligible displacements, which probably originate in the spatial inhomogeneity of slip on the fault planes and a lack of the contribution of the Idosawa fault. A more elaborated fault model is constructed in the next section.
5. Slip Distribution Model for the Mj 7.0 Event
To model the ruptures associated with the Mj 7.0 event more precisely, we construct a slip distribution model by a least squares method. The fault geometry is assumed to be a plane fault, and we put each plane by fitting the surface breaks to the interferograms by trial and error. We set three rectangular faults corresponding to the Shionohira, Yunotake, and Idosawa faults. The fault top position is fixed to the depth of 0 km bsl. The individual fault is divided into square patches with a size of 1 × 1 km. We use the dislocation equations derived by Okada (1985) to calculate the surface displacement in the variable LOS directions. In the inversion, only the dip-slip and strike-slip components are estimated for each patch. Because of no constraint on the slip direction, there arose physically implausible slips in places, but they are minor in the overall slip distribution. The increase of model parameters gives rise to instability of the solution. To stabilize the solution, we here impose a spatial smoothness constraint on the slip distribution using a Laplacian operator. The relative weight of the constraints is determined by Akaike’s Baysian information criterion (Akaike, 1980). We assume the Shionohira and the Yunotake planar faults dipping westward, following the results in the previous section, while for the Idosawa fault we tried the possibility of both west- and east-dipping faults. The problem we solve is a nonlinear inversion on a parameter of the dip angle. We here determine the dip angle by a grid search, in which we first conduct the grid search with a coarse interval of 10° and then with a finer interval of 5° surrounding the dip angle determined in the previous step. We set the search range from 40° to 90°, referring to the results in the previous chapter that low-angle fault planes are not favourable.
We cannot neglect the contribution of the cross-terms of the covariance matrix for the InSAR data, because they have a strong spatial correlation in general, which largely results from the variations of atmospheric water vapour (Lohman and Simons, 2005; Fukahata and Wright, 2008). We incorporate the cross-terms of the covariance matrix in the inversion scheme, following the equation presented by Fukahata and Wright (2008), and now take the characteristic correlation distance of errors to be 10 km (Wright et al., 2003; Fukahata and Wright, 2008).
Figure 8 shows the calculated LOS displacement predicted from our model and the residual between the observations and the calculations. Compared with the result of uniform slip models in the previous chapter, the slip distributed model significantly reduces the residuals and is able to account for the observations better. In particular, there is little residual in the proximity of the Yunotake fault.
The optimal dip angles for Shionohira, Yunotake, and Idosawa faults are determined to be 50°, 65°, and 50°, respectively. The total seismic moment is 1.55 × 1019 N m (Mw 6.7) assuming a rigidity of 30 GPa, and the released moments for each fault are estimated to be 9.22 × 1018 N m (Mw 6.6), 4.22 × 1018 N m (Mw 6.4), and 2.09 × 1018 N m (Mw 6.1) for the Shionohira, Yunotake, and Idosawa faults, respectively. According to the results of JMA CMT, NIED CMT, and Global CMT solutions, the seismic moments are 1.2 × 1019 N m (Mw 6.7), 9.58 × 1018 N m (Mw 6.6), and 1.2 × 1019 N m (Mw 6.7), respectively. Our result is good agreement with them.
Figure 9 shows the estimated slip distributions. The major slip on the Shionohira fault occurred near the ground surface. The slips are nearly pure normal fault motions over all the fault plane. For the Yunotake fault, the major slip is distributed at a depth less than 5 km along the dip from the fault top, while at a greater depth no significant slip is inferred. A normal fault motion is dominant over all the fault plane. Slips of ~2 m are estimated at the northwest of the fault, and the shallow slip significantly includes a sinistral component. The slip on the Idosawa fault also shows a nearly pure normal fault motion as well as the other two faults. The major slips are distributed at, and around, 5 km along the dip from the fault top. The estimated maximum slip is less than 1 m, which is much smaller than the slips on the other two faults.
6.1 Reliability of the fault model
To confirm the reliability regarding the estimated dip angle, which is a nonlinear fault parameter in our inversion scheme, the residual distribution for the case of a 10°-interval search is shown as a function of dip angle in Fig. 10. The residuals of the solution obtained at each step of the grid search are plotted. On each panel, the dip angle of the Shionohira fault is fixed at a certain angle (e.g., for the top left panel, the dip angle is fixed at 40°), and the residuals (vertical axis) are shown as a function of the dip angle of the Yunotake fault (horizontal axis). Individual lines on each panel are the residuals of when the dip angle of the Idowasa fault is fixed at a certain angle. The residuals are normalized so as to be 0 to 1, and the scale of the vertical axis is the same for comparison. First, we find that there is a tendency that small residuals are achieved when the dip angle of the Shionohira fault is neither high nor low, but is moderate. Similarly, moderate angles are preferable to high/low angles for the Yunotake fault, irrespective of the dip angles of the Shionohira fault. For the Idosawa fault, in all cases, west-dipping is preferable to east-dipping and moderate dip angles, identical to the Shionohira fault, are favorable. It means that the dip angles are well constrained in the residual space.
Next, let us confirm the reliability of the dip angle for the Shionohira fault from a different aspect. For both the rectangular fault model and the slip distribution model, the preferred dip angle is evaluated to be 50 ~ 60°. According to field surveys along the fault, however, the dip angle seems to be high as it is shown that the hanging wall block falls down nearly vertically (Fig. 5(A)). To test the reliability of the moderate angle, we employed a forward modeling. Here, we gave a uniform normal-fault-slip of 5 m, equivalent to Mw 6.6 on a rectangular fault plane (10 × 5 km), and we tried three cases: dip angles = 80, 60, and 40°. Figure 11 shows the calculated LOS displacement fields for each dip angle we assigned. Broken contour lines are drawn only for the LOS shortening area so as to distinguish between the lengthening and the shortening. In the case of a high-angle (Fig. 11(a)), the fringe pattern in the western side of the fault is relatively circular compared with the observation. Furthermore, the high-angle fault does not produce a slant range shortening distributing in the further west of the intensive deformation (Fig. 2). In the case of the low-angle (Fig. 11(c)), a slant range shortening is produced, but is too large. On the other hand, a moderate-angle model can reproduce well the characteristics that neither high- nor low-angle models can explain (Fig. 11(b)). It strongly suggests that a significant normal fault slip is inevitable to occur on not high-/low- but moderate-dip-angle fault plane. We could not rule out the possibility that a slip occurred with a high-dip-angle near the ground surface, such as a listric fault, but such a curved fault plane is not implied in the aftershock distribution from the JMA catalog.
6.2 Relationship between fault motions and topography
A 3D mapping of an interferogram, draped over the topographic relief, is shown in Fig. 12 to facilitate comparison between the InSAR map, the topography, and the configuration of our fault models. Let us first consider the Yunotake fault area. Vertical displacements predicted from our models are depicted in the middle layer. Our fault model shows that the Yunotake fault is of normal fault motion with a west-dipping plane, producing an upheaval at the northeastern side of the fault and subsidence at the southwestern side (Fig. 12). Comparing this to the topography, we can clearly see that the normal fault motion is correlated with present-day topography, in that the mountainous area is at the northeastern side of the fault. According to the Research Group for Active Faults of Japan (1991), the topographic high corresponding to the fault scarp has been recognized as the fault features (fault topography) for the Yunotake fault. The coseismic slip motion is quite consistent with the orientation of the long-term cumulative displacement, supporting the idea that the normal fault motions have repeated historically on the Yunotake fault, and have contributed to the development of the present-day topography. A right lateral component, besides the dip slip, has been also identified from the fault outcrop (According to the Research Group for Active Faults of Japan, 1991), but our fault model shows no right lateral slip but rather, partly, a left lateral one.
Also for both the Shionohira and the Idosawa faults, normal fault motions on west-dipping planes are inferred from our modeling. The fault model predicts that the largest ground subsidence occurred in the west of the Shionohira fault (Fig. 12). By analogy with a similar mechanism interpreted for the Yunotake fault, we may speculate that if normal faulting had been experienced on the faults repeatedly actively, a topographic high would have been developed in the east. The topography, however, is antithetical to the coseismic displacements with normal fault motions, although earthquake surface faults are just on the topographic lineaments (Figs. 4 and 12). Little correlation between the fault motions and the present-day topography may suggest that large normal fault slip events have been rare on the Shionohira and the Idosawa faults historically.
6.3 Are the ruptures on the other two faults promoted by that on the Shionohira fault?
Ruptures on multiple faults are probably involved in the Mj 7.0 event, but, from the InSAR data we are unable to obtain information regarding the time history of the ruptures. According to analyses of seismic waveform data, the rupture of the Mj 7.0 event started on the Shionohira fault, followed by that on the Yunotake fault with a delay of about 10 s (Hikima, 2012). Are the ruptures on the Yunotake fault promoted by those on the Shionohara fault? A Coulomb Failure Function change (ΔCFF) can be an indicator to judge whether the static stress change is conducive to slip on a fault plane. We first test whether or not the slip on the Yunotake fault can be facilitated by the static stress change caused by the slip on the Shionohira fault. Referring to the geometries and the rakes, we set each patch of our slip model for the Yunotake fault as a receiver fault. We assumed 0.4 as an effective coefficient of friction, including a pore pressure effect, according to Stein et al. (1994), and the rigidity of 30 GPa. Figure 13(a) shows the estimated ΔCFF distribution on the Yunotake fault. Gray-colored areas represent negative sign values. The result shows that the slip on the Shionohira fault contributes to promoting the slip in the deeper area, while suppressing it in the shallower area. It is not consistent with the estimated slip distribution on the Yunotake fault in that major slips concentrate at shallow depth. We attempted to evaluate the stability of our stress change pattern for an effective coefficient of friction from 0.2 to 0.8, and confirmed that in all cases the ΔCFF values are negative at shallow depths as well (−3.9 to −2.5 MPa at the maximum).
Figure 13(b) shows the ΔCFF distribution on the Yunotake fault, but adding the effect of static stress changes caused by the Mw 9.0, the Mj 6.1, and the Mj 6.0 events. We used the fault model proposed by the Geospatial Information Authority of Japan (GSI) for the Mw 9.0 event (GSI, 2011). ΔCFF values with a positive sign are expected over all the fault plane, but negative ACFF values still remain in the major slip area, suggesting that the static stress change does not play a role in promoting the major slip. Although the temporal relationship between the onset of the Shionohira fault and the Idosawa fault is not well-understood, we attempt an estimate of ΔCFF for the Idosawa fault under the assumption that the rupture on the Shionohira fault was followed by that on the Idosawa fault. Also for the Idosawa fault, ΔCFF values with a negative sign are distributed on the major slip area, indicating the suppression of the slip (Figs. 13(c) and (d)).
On the other hand, it is possible that the occurrence of aftershocks reacts to the static stress changes. Figure 14 shows the seismicity in, and around, the source region of the Mj 7.0 event. Figures 14(a) and (b) are the seismicity maps during one month before, and after, the occurrence of the Mj 7.0 event, respectively. We obviously find that aftershocks actively occurred in, and around, the Shionohira fault after the Mj 7.0 event, while around the Yunotake fault no remarkable increase of earthquakes is noticeable. Although the source mechanisms of the aftershocks in, and around, the Yunotake fault are not known well, the inactive seismicity might reflect the stress shadow area produced by the mainshock slip on the Shionohira fault.
The analysis result on the static stress change does not support the idea that the static stress change due to the slip on the Shionohira fault is responsible for the initiation of the rupture on both the Yunotake fault and the Idosawa fault. Other mechanisms, such as dynamic triggering, may have played a role in inducing the ruptures on the other two faults. The problem concerning the triggering of ruptures is beyond the scope of this paper. This question is a matter for future studies.
7. Concluding Remarks
We have applied an interferometric SAR (InSAR) analysis using ALOS/PALSAR data to inland crustal earthquakes in the Fukushima-Hamadori area and we have detected the crustal deformation associated with the Mj 7.0 event. The following conclusions were derived from the analyses:
The most concentrated crustal deformation is located ~20 km west of the city of Iwaki, showing displacements away from the satellite with ~2.2 m at the maximum.
Clear displacement discontinuities are recognized in the interferograms, with an offset of ~ 1.6 m at the maximum, which are just on the Shionohira, the Yunotake, and the Idosawa faults.
From the field surveys, we found that earthquake surface faults appeared with a vertical offset of ~ 1.9 m at the maximum, equivalent to ΔLOS of ~ 1.5 m. Their locations match the discontinuities identified in the interferogram.
Our slip distribution model shows nearly pure normal fault motions on west-dipping planes with a moderate dip angle for all three faults (Shionohira, Yunotake, and Idosawa).
The west-dipping normal fault motion on the Yunotake fault is correlated with present-day topographic features, while those on both the Shionohira and Idosawa faults are inversely correlated with the topography.
A ΔCFF estimate suggests that the static stress change due to the mainshock fault rupture on the Shionohira fault does not initiate the slips on the other two faults, maybe suggesting that other mechanisms are involved in the triggering of rupture on these two faults.
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PALSAR data were provided from the Earthquake Working Group under a cooperative research contract with JAXA (Japan Aerospace Exploration Agency). The ownership of PALSAR data belongs to JAXA and METI (Ministry of Economy, Trade and Industry). We used hypocenter data processed by the Japan Meteorological Agency (JMA). We used GMT (The Generic Mapping Tools) provided by Wessel and Smith (1998) for constructing the figures. We thank two reviewers (Dr. P. S. Agram and an anonymous reviewer) and the editor (Prof. Miura) for their helpful comments to improve our manuscript.
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Kobayashi, T., Tobita, M., Koarai, M. et al. InSAR-derived crustal deformation and fault models of normal faulting earthquake (Mj 7.0) in the Fukushima-Hamadori area. Earth Planet Sp 64, 15 (2012). https://doi.org/10.5047/eps.2012.08.015
- Fukushima-Hamadori (Mj 7.0)
- earthquake surface faults
- normal fault
- Shionohira fault
- Idosawa fault
- Yunotake fault