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Normalfaulting stress state associated with low differential stress in an overriding plate in northeast Japan prior to the 2011 Mw 9.0 Tohoku earthquake
Earth, Planets and Space volume 70, Article number: 51 (2018)
Abstract
Spatial and temporal variations in inland crustal stress prior to the 2011 Mw 9.0 Tohoku earthquake are investigated using focal mechanism solutions for shallow seismicity in Iwaki City, Japan. The multiple inverse method of stress tensor inversion detected two normalfaulting stress states that dominate in different regions. The stress field around Iwaki City changed from a NNW–SSEtrending triaxial extensional stress (stress regime A) to a NW–SEtrending axial tension (stress regime B) between 2005 and 2008. These stress changes may be the result of accumulated extensional stress associated with co and postseismic deformation due to the M7 class earthquakes. In this study we suggest that the stress state around Iwaki City prior to the 2011 Tohoku earthquake may have been extensional with a low differential stress. High pore pressure is required to cause earthquakes under such small differential stresses.
Introduction
After the Mw 9.0 earthquake that occurred on March 11, 2011, offshore Tohoku, Japan (hereafter, the 2011 Tohoku earthquake; e.g., Ozawa et al. 2011; Simons et al. 2011), many crustal earthquakes were induced in inland regions of northeastern Japan (e.g., Hirose et al. 2011; Yoshida et al. 2012). A remarkable phenomenon of the induced seismicity was a sudden increase in shallow normal faulting along the Pacific coast of northeastern Japan, most notably in the Fukushima and Ibaraki prefectures (Fig. 1). A Mw 6.6 earthquake occurred on April 11, 2011, in Iwaki City, Fukushima Prefecture (hereafter, the 2011 Iwaki earthquake; Fig. 1), just 1 month after the 2011 Tohoku earthquake. The focal mechanism of this earthquake is believed to correspond to normal faulting with a NE–SWoriented T axis (Fig. 1, adapted from Japan Meteorological Agency (JMA) catalog data; see e.g., Lin et al. 2013; Otsubo et al. 2013; Toda and Tsutsumi 2013), despite the fact that crustal normal faulting in response to a trenchtype earthquake is very rare (e.g., Farías et al. 2011).
Earthquake focal mechanisms are thought to be the most effective means of identifying crustal stress (e.g., Michael 1984), because they constrain the stress field at depths where earthquakes occur. Imanishi et al. (2012) reported a normalfaulting stress regime around Iwaki City prior to the 2011 Tohoku earthquake by applying the stress tensor inversion method of Michael (1984) to smallmagnitude earthquakes. They concluded that the 2011 Tohoku earthquake, in combination with a preexisting normalfaulting stress regime, triggered a normalfaulting earthquake sequence. However, the estimated stress tensor did not account for all focal mechanisms, suggesting the existence of stress heterogeneity.
The aim of this study is to explore spatial and temporal variations in crustal stress around Iwaki City prior to the 2011 Tohoku earthquake. We apply the multiple inverse method (Otsubo et al. 2008) to the earthquake focal mechanisms of Imanishi et al. (2012) and show that two normalfaulting stress states prevailed in different regions. We examine the tectonic background of the spatial and temporal variations in stress and discuss the stress level in the background of the region of the study area.
Methods
Imanishi et al. (2012) computed the focal mechanisms of 26 small shallow earthquakes (M_{j} ≤ 3.2, depth < 20 km) around Iwaki City that occurred between 2003 and 2010. We applied the stress tensor inversion to 12 earthquakes (Imanishi et al. 2012; Additional file 1: Table S1) with normalfaulting and strikeslip faulting mechanisms located within the source region of the normalfaulting earthquake sequence. Following Imanishi et al. (2011), we evaluated focal mechanism uncertainties for each event from the average of their Kagan angles (Kagan 1991), where uncertainties are measured between the best fitting solution and each solution whose residual is less than 1.1 × the minimum residual. Most events show normal faulting with T axes that trend WNW–ESE to NNW–SSE (Fig. 1). Imanishi et al. (2012) applied the method of Michael (1984) to these 12 focal mechanisms and obtained a normalfaulting stress regime with a minimum principal stress axis trending NW–SE and a stress ratio Φ = (σ_{2 }− σ_{3})/(σ_{1 }− σ_{3}) = 0.6–0.7, where σ_{1}, σ_{2}, and σ_{3} are the maximum, intermediate, and minimum principal stress axes, respectively. However, some focal mechanisms yielded different stress regimes, which may suggest that the assumption of a homogeneous stress state is inappropriate for these data.
In contrast to conventional stress tensor inversion methods (e.g., Gephart and Forsyth 1984; Michael 1984), the multiple inverse method (MIM; Otsubo et al. 2008) is able to separate and isolate stresses from complex focal mechanism data based on a resampling technique without prior information. Significant stresses were categorized into clusters of stress tensors using the resampling technique of Otsubo et al. (2008), which employs kmeans clustering, similar to Otsubo et al. (2006), to recognize clusters of stress tensors. For the ith cluster, the 95% confidence interval (CI ^{(i)}_{95} ) is calculated using CI ^{(i)}_{95} = σ^{(i)} _{mean} ± 1.96 × SE^{(i)}, where σ^{(i)} _{mean} is the mean of the contributing stresses (i.e., the cluster center) and SE^{(i)} is the standard error about the mean. SE^{(i)} itself is defined by the equation SE^{(i)} = S^{(i)}/(N^{(i)})^{1/2}, where S^{(i)} is the standard deviation of the ith cluster and N^{(i)} is the number of stress observations contributing to S^{(i)}. The standard deviation is calculated from the distance between the cluster center and each stress tensor assigned to the same cluster. We employed the angular stress distance described by Yamaji and Sato (2006) to calculate distances in this study.
When we applied MIM to the 12 focal mechanisms derived by Imanishi et al. (2012), we employed the combination number k_{f} = 5 and the enhance factor e = 8, following Otsubo et al. (2008, 2013). A value of 4 or 5 is usually assigned to k_{f} because the stress tensor inversion is an evendetermined problem for four observations and is overdetermined for five (Yamaji 2000; Otsubo et al. 2008). The enhance factor e is a parameter used to attenuate the effects of noisy data in the solution space (Yamaji 2000). The default value of e is 8; MIM nominally accepts values in the range 0 ≤ e ≤ 99.
Results
We applied MIM to the data set of Imanishi et al. (2012) and detected two normalfaulting stress regimes, labeled A and B in Fig. 2. For stress regime A, σ_{1} and σ_{3} are orientated at 331°/75° and 140°/15°, respectively, and the stress ratio Φ = 0.54 ± 0.18 (Fig. 2b, c). Thus, regime A corresponds to a NNW–SSEtrending triaxial extensional stress. The second solution, regime B, shows σ_{1} and σ_{3} orientations of 147°/87° and 299°/3°, respectively, with a stress ratio Φ = 0.84 ± 0.10 (Fig. 2b, c), which corresponds to NW–SEtrending axial tension (σ_{1} = σ_{v} ≈ σ_{2} >> σ_{3}). The angular stress distance between A and B, defined as the dissimilarity between two stresses (Yamaji and Sato 2006), is ~ 39°, suggesting that the stresses are significantly different from each other (Nemcok and Lisle 1995). The σ_{3} orientations of the stresses do not overlap at the 95% confidence level for the means and standard deviations of the kmeans clusters (Fig. 2). The solution of Imanishi et al. (2012), using the method of Michael (1984) and shown by crosses in Fig. 2b, diverges from regime B by ~ 27° and from A by ~ 31°, suggesting a slightly better match to B.
The Wallace–Bott hypothesis (Wallace 1951; Bott 1959) states that an earthquake’s slip vector is parallel to the resolved shear stress on the fault. Based on this hypothesis, we assume that a stress is compatible with a fault slip direction if the misfit angle between the slip direction predicted by the stress and the observed slip direction on the same fault plane is sufficiently small. In this study, we adopt the approach of Otsubo et al. (2008, 2013) for the analysis of stress and associated focal mechanisms in the Iwaki City region. The spatial and temporal changes in stress can be identified by relating observed slip directions from focal mechanisms to a single stress solution (Otsubo et al. 2008, 2013). The threshold of the misfit angle was determined here based on the uncertainties of the strike, dip, and rake (Gephart and Forsyth 1984; Michael 1991). When the misfit angles are smaller than the uncertainties of the stress and focal mechanism solutions, the observed slip directions agree with theoretical values to within the estimated uncertainties.
Figure 3 shows the computed misfit angle for each focal mechanism with respect to A and B, with only the smaller angle for each pair of nodal planes shown. If we assume that a stress with a misfit angle of less than 30° is compatible with a datum (e.g., Gephart and Forsyth 1984; Michael 1991), either or both stresses are able to explain the source of 10 of the 12 events (Fig. 3). The stress for the two earthquakes with larger misfit angles (nos. 4 and 11) is unclear because the stress tensor inversion is underdetermined for a value of two earthquakes (Yamaji 2000; Otsubo et al. 2008). These earthquakes are located deeper than 15 km, which is below both the focal depth of the 2011 Iwaki earthquake (~ 6 km) and the floor of the inland seismicity that was experienced after the 2011 Tohoku earthquake (~ 10 km) (Fig. 1; see also Imanishi et al. 2012); thus, we do not discuss them further.
Discussion
Using the focal mechanisms of Imanishi et al. (2012), MIM reveals two normalfaulting stress states around Iwaki City before the 2011 Tohoku earthquake (Fig. 2). In this study, we discuss the temporal and spatial stress changes around Iwaki City to explain the stress heterogeneity.
Temporal and spatial stress changes around Iwaki City
We attribute the variations in the stress field to temporal variations. Stress regime A can be seen to account for all the focal mechanisms derived from earthquakes that occurred before 2005. This implies that only stress regime A should be used as an appropriate solution before 2005 (Fig. 3). In contrast, stress regime B can be seen to account for all the focal mechanisms, except for no. 11, derived from earthquakes occurring after 2008 (Fig. 3). In the intervening period between 2005 and 2008, derived focal mechanisms can be related to both stress regimes A and B. Hence, one possible explanation of the stress heterogeneity is that the stress field around Iwaki City temporally changed from a NNW–SSEtrending triaxial extensional stress (regime A) to a NW–SEtrending axial tension (regime B), with the transition between the two occurring from 2005 to 2008. Hence, we define stress period I from 2003 to 2005 and stress period II from 2008 to 2010 (Fig. 3).
Next, we consider the dynamics for the stress changes around Iwaki City. The σ_{3} orientation of stress regime B is subparallel to the orientations of the co and postseismic displacements of large earthquakes (Mw ~ 7) that occurred during the period 2005–2010 (Fig. 2b; Suito et al. 2011). The postseismic deformation determined from continuous GNSS monitoring reveals that the seismic moments released by transient slip following the M7 class earthquakes are much larger than the seismic moment estimates for the earthquakes themselves (Suito et al. 2011). Stress regime B may therefore be the result of accumulated extensional stress associated with co and postseismic deformation due to the M7 class earthquakes, which occur more frequently than M9 class earthquakes.
We focus on the location of the epicenter of the earthquakes to explain the stress heterogeneity around Iwaki City. Stress regime A accommodates all focal mechanisms derived from earthquakes in the western part of the study area around 140.8°E, except for no. 11. This implies that stress regime A is the most appropriate solution for this region (Fig. 4). On the other hand, stress regime B encompasses all focal mechanisms in the region around 141.0°E (Fig. 4). In the area between the two regions, the computed focal mechanisms could be related to either regime (Fig. 4). Hence, we infer that a series of M7 class earthquakes altered the stress regime only in the east of the study area.
Estimation of differential stress around Iwaki City
Figure 5 shows the GNSS time series of the NW–SE component at sites near Iwaki City together with the occurrence times of five M7 interplate earthquakes. The time series show a deviation from a steady westward movement after the 2008 Mj 7.0 Ibarakiken Oki earthquake (label B). The timing of the transition toward eastward motion appears to correlate with the period during which stress regime B was dominant. The observation supports the hypothesis that the inferred change in stress field over time was due to extension associated with the co and postseismic deformation from the M7 class earthquakes.
We compared the stress changes caused by the co and postseismic deformation with the extensional stresses in stress periods I and II. The direction of extensional stresses induced by the co and postseismic deformation is almost parallel to the orientation of the σ_{3} axes, while it is perpendicular to the orientations of the σ_{1} and σ_{2} axes (Fig. 2b). Because σ_{1} is the overburden pressure, σ_{1} is almost constant during the co and postseismic deformation. Hence, the extensional stress induced by the co and postseismic deformation should only affect the magnitude of σ_{3} rather than those of σ_{1} and σ_{2}, and in order for the stress ratio to change from 0.54 (± 0.18) to 0.84 (± 0.10), σ_{3} must decrease. Here, the reduction in the magnitude of σ_{3} corresponds to a buildup of extensional stress.
The magnitude of the differential stress in the study area is estimated based on the temporal change in the stress field (Fig. 6). For convenience, in the following discussion, we define σ ^{A}_{1} (σ ^{B}_{1} ), σ ^{A}_{2} (σ ^{B}_{2} ), and σ ^{A}_{3} (σ ^{B}_{3} ) as the maximum, intermediate, and minimum compressive principal stresses for stress A (and B), respectively. The differential stress for stress A (B) can be expressed by Δσ^{A }= σ ^{A }_{1} − σ ^{A}_{3} (Δσ^{B} = σ ^{B }_{1} − σ ^{B}_{3} ). From the change in the stress ratio from 0.54 (± 0.18) to 0.84 (± 0.10), we obtain the following relationships: σ ^{B}_{3} − σ ^{A }_{3} ~ 0.09 − 9.03Δσ^{A} and Δσ^{B }~ 1.08 – 10.03Δσ^{A} (Fig. 6). The former relationship indicates that the extensional stress induced by the co and postseismic deformation is approximately 0.1 to 9 times as large as the differential stress for stress A. The latter relationship signifies that the extensional differential stress increases by a factor of almost 1.1 to 10 from stress A to stress B. Based on the amount of displacement from the co and postseismic deformation (~ 1–3 cm; Fig. 5), the resulting strain is estimated to be ~ 3 × 10^{−7} to 2 × 10^{−6} for the NW–SE component between the two sites near Iwaki City. Assuming that the crust is elastic with a Young’s modulus of 32 GPa, the induced stress, σ ^{B}_{3} − σ ^{A}_{3} , is estimated between 0.9 × 10^{−2} and 6.4 × 10^{−2} MPa. Inserting this estimated value into the relationships derived above, we obtain differential stresses for stress A, Δσ^{A}, and stress B, Δσ^{B}, of approximately 1.00 × 10^{−3} to 7.11 × 10^{−1} and 1.10 × 10^{−3} to 7.13 MPa, respectively. Hence, we propose that the differential stress is less than the order of 1 MPa around Iwaki City prior to the 2011 Tohoku earthquake.
Background of the low differential stress around Iwaki City
We consider the generation of the 2011 Iwaki earthquake in the context of the low differential stress in the study area. We showed the stress heterogeneity around Iwaki City prior to the 2011 Tohoku earthquake as the spatial or temporal stress changes. In this study, we could not identify a possible explanation of the stress heterogeneity. In both cases, we suggest that the stress state around Iwaki City prior to the 2011 Tohoku earthquake might have been extensional with a low differential stress. A low differential stress prior to the 2011 Iwaki earthquake was reported by Yoshida et al. (2015), who estimated differential stress magnitudes ~10^{0}–10^{1} MPa by comparing the stress orientations in the postIwaki earthquake period with static stress changes due to the Iwaki earthquake and three nearby M5 class earthquakes. Tomographic studies have imaged lowvelocity anomalies beneath the hypocenter of the 2011 Iwaki earthquake (Fig. 1; see also Kato et al. 2013), which may correspond to zones of high porefluid pressure. Zhao (2015) showed that a lowvelocity zone is visible in the lower crust and mantle wedge, and that it extends beneath the hypocenter of the 2011 Iwaki earthquake, down to the subducting Pacific slab. The discharge of a large amount of thermal water after the 2011 Iwaki earthquake (Sato et al. 2011; Kazahaya et al. 2013) indicates that earthquakes in this region promote the upwelling of deep groundwater. The earthquakes themselves may be triggered by a decrease in effective normal stress and fault strength due to the increased porefluid pressure (e.g., Sibson 1990; Micklethwaite and Cox 2006; Terakawa et al. 2013). By examining the fault failure of the 2011 Iwaki earthquake with respect to the change in the state of stress in the Iwaki area produced by the 2011 Tohoku earthquake, Miyakawa and Otsubo (2015) showed that excess fluid pressure is required to explain the 2011 Iwaki earthquake. Therefore, we infer that high porefluid pressure could enable the generation of earthquakes under conditions of low differential stress (Sibson 1992).
Conclusions
An investigation of spatial and temporal changes in extensional stress in the interseismic period before the 2011 Mw 9.0 Tohoku earthquake revealed that the preTohoku stress state around Iwaki City was significantly heterogeneous. Our findings support the inference that the stress state around Iwaki City prior to the 2011 Tohoku earthquake was extensional with a low differential stress. The differential stress of the normalfaulting stress regime increased after the 2011 Tohoku earthquake.
The multiple inverse method (MIM) of stress inversion resolves statistically significant stress heterogeneities in the study area. The MIM is capable of detecting stress heterogeneities that cannot be detected using more conventional stress tensor inversion methods. The application of the MIM to other study areas in the future may provide an important monitoring tool for evaluating stress change.
Abbreviations
 JMA:

Japan Meteorological Agency
 GNSS:

global navigation satellite system
 MIM:

multiple inverse method
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Authors’ contributions
MO led and designed the research and drafted the manuscript. MO carried out the stress tensor inversion analysis, drafted the figures, and contributed to assessing the results. AM and KI contributed to the discussion of the results. All authors read and approved the final manuscript.
Acknowledgements
We thank two anonymous reviewers for suggestions that led to improvements in the manuscript. We thank Dr. T. Nishimura for discussions on GNSS data, and Dr. J. Hardebeck for fruitful discussions. This study was supported by MEXT KAKENHI (number 26109003). Some of the figures were generated using Generic Mapping Tools (GMT; Wessel and Smith Wessel and Smith 1998).
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The authors declare that they have no competing interests.
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Additional file
Additional file 1.
Fault slip data set obtained from focal mechanisms of earthquakes determined by Imanishi et al. (2012) around Iwaki City prior to the 2011 Tohoku earthquake.
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Otsubo, M., Miyakawa, A. & Imanishi, K. Normalfaulting stress state associated with low differential stress in an overriding plate in northeast Japan prior to the 2011 Mw 9.0 Tohoku earthquake. Earth Planets Space 70, 51 (2018). https://doi.org/10.1186/s4062301808139
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DOI: https://doi.org/10.1186/s4062301808139
Keywords
 Crustal stress
 2011 Tohoku earthquake
 Deformation
 Stress tensor inversion
 Differential stress