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Afterslip distribution following the 2003 Tokachioki earthquake: An estimation based on the Green’s functions for an inhomogeneous elastic space with subsurface structure
Earth, Planets and Space volume 62, pages 923–932 (2010)
Abstract
We derive the 1yr afterslip distribution following the 2003 Tokachioki (Hokkaido, northeastern Japan) earthquake (Mw8.0) by inverting geodetic data, i.e., horizontal and vertical displacements, at 142 land stations of the Global Positioning System (GPS) in Hokkaido and northernmost Tohoku districts, together with vertical displacements at two offshore stations of pressure gauge (PG) off the Pacific coast of Hokkaido. We use the Green’s functions (GFs), calculated with a finite element method, for an inhomogeneous elastic (IE) model incorporating subsurface structure. Obtained results show a striking feature of the distribution pattern of significant afterslip, namely, a Ushaped afterslip zone encircling the coseismic rupture zone of the 2003 event. Amounts of the 1yr afterslip reach up to 0.9 m, and total seismic moments released from all afterslip zones are of the order of 1021 N m, corresponding to an earthquake of MW 8.0. For comparison, we also estimate the 1yr afterslips based on GFs for the homogeneous elastic (HE) model to find that the total seismic moment with GFs for the IE model is larger than that with GFs for the HE model by ∼33% (when the most probable values are compared) if we assume a rigidity of 40 GPa. This result implies that inhomogeneities due to subsurface structure have an important role in geodetic inversions.
1. Introduction
Since an epochmaking discovery of afterslip (or postseismic slip) following the 1994 Sanrikuharukaoki (Tohoku district, northeastern Japan) earthquake (M_{W}7.8) by Heki et al. (1997), the same phenomena have been reported in several studies (e.g., Hirose et al., 1999; Nishimura et al., 2000; Bürgmann et al., 2001; Yagi et al., 2001). Such afterslips have quite a significant role in discussing the deficit of slip amounts after the occurrence of interplate earthquakes, i.e., imbalance between plate convergence rate and amount of coseismic slip, or furthermore in discussing the recurrence interval or size of the next interplate earthquake. Hence, it is very important to estimate afterslips following such interplate earthquakes as precisely as possible.
The afterslip distribution following the 2003 Tokachioki (Hokkaido, northeastern Japan) earthquake (M_{w}8.0), which was the largest interplate earthquake in Japan in the last decade, has been estimated by several authors by inverting geodetic data, i.e., displacements on the ground surface. For example, Miyazaki et al. (2004), Miura et al. (2004), and Ozawa et al. (2004) deduced it from displacement data at many sites in the Hokkaido and northern Tohoku districts of a dense Global Positioning System (GPS) network GEONET (GPS Earth Observation Network; e.g., Miyazaki et al., 1997) operated by the Geospatial Information Authority (GSI) of Japan. Baba et al. (2006) also obtained afterslip distribution by inverting displacement data at many GEONET sites on land with additional vertical displacements at two offshore oceanbottom pressure gauge (PG) stations operated by the Japan Agency for MarineEarth Science and Technology (JAMSTEC) (e.g., Hirata et al., 2002). In these geodetic inversions, all authors used the Green’s functions (GFs, i.e., theoretical ground surface displacements due to unit dislocations on subsurface faults) calculated for a homogeneous elastic halfspace or for horizontally layered elastic media.
However, using the GFs calculated under such rather simplified elastic conditions seems to be misleading in the estimation of afterslip distribution, since the subsurface structure of any region, especially that in and around Japan, is more or less inhomogeneous, and such inhomogeneity should affect, to a certain extent, the surface displacements. In fact, performing some numerical 3D finite element calculations with a grid model for the Hokkaido and Tohoku districts, Sato et al. (2007) clarified that a very large discrepancy in the surface displacements existed between the cases of homogeneous and inhomogeneous elastic subsurface models. The discrepancies they found were more than 20% and even as large as ∼40% in some cases. On the other hand, the surface displacement data usually employed in geodetic inversions are those obtained with GPS having quite high precision, varing a few mm (for horizontal displacements) to several mm (for vertical displacements) (e.g., Nishimura et al., 2004). Hence, such quite large discrepancies strongly suggest that, for more precise and reliable geodetic inversions of afterslip distribution, the surface displacement calculated for an inhomogeneous elastic medium with realistic subsurface structure, unlike the usual cases so far, should be used as the GFs.
In this paper, we perform some inversions by using the GFs calculated for inhomogeneous elastic media, incorporating a realistic subsurface structure to estimate the afterslip distribution following the 2003 Tokachioki earthquake. We also perform an inversion with the GFs calculated for homogeneous elastic media to compare the obtained afterslip distribution with those obtained from GFs for inhomogeneous elastic media.
2. Method of Geodetic Inversions
The 2003 Tokachioki earthquake was an interplate earthquake that occurred on the plate interface between the subducted oceanic plate, namely, the Pacific plate, and the landside North American (or Okhotsk) plate. Hence, we naturally assume that the afterslip following the earthquake also took place on the plate interface between these two plates. The configuration of the boundary between the two plates in and around the epicentral region of the 2003 event has been proposed by several authors, mainly based on seismological studies (e.g., Hasegawa et al., 1983; Suzuki et al., 1983; Miyamachi et al., 1994; Katsumata et al., 2003). Among them, we adopt the one newly determined by Katsumata et al. (2003), which based on the hypocentral distribution of local earthquakes.
In order to estimate the distribution of afterslip, the plate interface in and around the coseismic slip zone of the 2003 event beneath the Pacific coast of Hokkaido is divided into many celllike rectangular subfaults (total number of subfaults is I×J, where I and J are the numbers of subfaults within each row and column of the subfault array). Fixing the azimuth of the afterslip vector (i.e., the direction of horizontal component of afterslip vector), we estimate the slip amount on each subfault (note that only the azimuth of afterslip vector is fixed and the direction of afterslip vector on each subfault plane is adjusted according to its geometry, namely, the strike and dip angle of the subfault plane). The azimuth of afterslip vector on each subfault is based on that of the coseismic slip vector of the 2003 event determined by Yamanaka and Kikuchi (2003). This azimuth of afterslip vector is assumed to be adequate for all subfaults not only inside the coseismic rupture zone but also outside.
In the inversion, we impose the same constraint as that adopted by Baba et al. (2006), i.e., a smoothness constraint, on the slip distribution on each subfault as follows:
where is the slip amount on the (i, j)th subfault. Equation (1) can be rewritten in a matrix form as follows:
where S is a matrix representing the smoothness constraint, whose elements can be calculated based on Eq. (1), and x is a vector of slip amounts on subfaults. The smoothness constraint represented by Eq. (2) can then be combined with a usual observational equation to form a modified one as follows:
where d is a vector of observed surface displacements, and α represents a smoothness parameter weighting the smoothness matrix S. G in Eq. (3) is a matrix whose element G_{ m,n } is the socalled GF describing the expected surface displacement at the mth observation point caused by a unit dislocation on the nth subfault for the (i, j)th subfault). The method of calculation of the GFs will be described in the next section. First, assuming a certain value for the smoothness parameter α, we solve Eq. (3) with an ordinary least squares method. Next, we calculate the socalled Akaike’s Bayesian Information Criterion (ABIC) (Akaike, 1980) based on Yabuki and Matsu’ura (1992) using the obtained model parameters and the assumed α. These processes are repeated to find the most appropriate smoothness parameter α which gives the minimum ABIC. Finally, using the smoothness parameter α obtained we solve Eq. (3) with a nonnegative least squares (NNLS) algorithm (e.g., Lawson and Hanson, 1974), together with a constraint for the slip at the lateral edges of the afterslip zone to be zero, to ensure stability of solution. Model error is also estimated with a boot strapping method (e.g., Tichelaar and Ruff, 1989).
3. Calculation of GFs
As mentioned earlier, GFs, i.e., the expected surface displacement at each observation point caused by a unit dislocation on each subfault, have been usually calculated with an assumption of a homogeneous or simply layered elastic halfspace (e.g., Miura et al., 2004; Miyazaki et al., 2004; Ozawa et al., 2004; Baba et al., 2006). However, such a simplified assumption seems inappropriate, especially for the region in and around Japan where the subsurface structure is very complicated. Hence, in order to incorporate the inhomogeneity due to such complication of subsurface structure, we adopt a 3D finite element technique in the calculation of GFs. For the calculation, we use the GeoFEM, a parallelized finite element code, developed at the Research Organization for Information Science and Technology (RIST) (e.g., Iizuka et al., 2002; Hyodo and Hirahara, 2004).
3.1 Subsurface structure and finite element grid
The model space and assumed subsurface structure for the finite element calculation are the same as those in Sato el al. (2007), so that we describe them briefly. The rectangle in Fig. 1 shows the model region, including the Hokkaido and Tohoku districts, northeastern Japan. The model space has a dimension of 1400 km (in the ESE direction)×1200 km (in the NNE direction)×200 km (depth). Since the curvature of the Earth’s surface is not taken into account, the model surface is treated as a flat plane. The assigned subsurface structure is shown in Fig. 2(a) which consists of four subregions, i.e., upper crust (UC), lower crust (LC), upper mantle (UM), and Pacific plate (PL). This subsurface structural model is based on the isodepth contours of the Conrad and Moho planes given by Zhao et al. (1992, 1994) and of the upper plane of the Pacific plate drawn by Katsumata et al. (2003, beneath Hokkaido area) and Hagiwara (1986, beneath Tohoku area).
We build a 3D finite element grid as shown in Fig. 2(b) by dividing the model space into many hexahedron elements with the CHIKAKU modeling system, consisting of CHIKAKUDB and CHIKAKUCAD developed at the RIKEN (e.g., Kanai et al., 1999, 2000, 2001) and CHIKAKUMESH developed at the Japan Atomic Energy Agency (JAEA) (e.g., Miyamura et al., 2004; Oishi et al., 2004). In order to obtain the GFs as precisely as possible, the grid used in the present study is much finer than that used in the previous study (Sato el al, 2007); the numbers of nodes and elements in the grid are 1,155,375 and 1,121,952, respectively, which are almost eightfold larger than those of the grid used in the previous study. A typical element near the surface in the central portion of the model has a size of ∼8 km (in horizontal direction)×1km(in depth direction). Examples of the vertical crosssectional views (in the ESE direction) of subsurface structure and finite element grid are shown in Fig. 3(a) and (b), respectively, which correspond to those along the lines ABin Fig. 2(a) and (b).
3.2 Material properties
The elastic material parameters, i.e., the Young’s modulus and Poisson’s ratio, assigned to UC, LC, UM, and PL are summarized in Table 1. In Table 1, the P and Swave velocities and densities for UC, LC, and UM used to derive the Young’s modulus and Poisson’s ratio are also listed. These P and Swave velocities are based on the seismological tomography by Nakajima et al. (2001), and densities are taken from Dambara and Tomoda (1969). The Young’s modulus and Poisson’s ratio of PL are adopted from Liu (1980) and Suito and Hirahara (1999), respectively.
In order to compare the afterslip distribution following the 2003 event obtained for an inhomogeneous subsurface structure with that for the homogeneous case, we also calculated the GFs for homogeneous elastic media, with the Young’s modulus and Poisson’s ratio presented in parentheses in Table 1 (i.e., 100 GPa and 0.25, respectively, as typical values). Hereafter, we denote these two material models as the inhomogeneous elastic (IE) model and homogeneous elastic (HE) model, respectively.
4. Data
Thedataweuse hereto derivethe 1yrafterslipfollowing the 2003 Tokachioki earthquake are the same as those employed in Baba et al. (2006). The data consist of two types; one is site displacement data obtained at continuous GPS stations and the other is offshore vertical movement data acquired with PG. These GPS and PG data are plotted in Fig. 4(a) and (b). The GPS data are horizontal and vertical displacements at 142 stations in the Hokkaido and northernmost Tohoku districts, which are the relative ones at the stations with respect to a reference station denoted by “R” in Fig. 4(a) and (b) (see Baba et al., 2006). In contrast, the PG data are absolute vertical displacements at two stations located far off the Pacific coast of Hokkaido operated by JAMSTEC. These absolute PG displacements are estimated after subtracting such components as the instrumental drift, ocean tides and thermal noises from the raw data, and they are considered to have observation errors of the order of 1 cm (see Hirata et al. (2002) and Baba et al. (2006) for detailed description on data reduction). All of these horizontal and vertical displacements at GPS and PG stations are those accumulated from 1 day to 1 year after the mainshock of the 2003 event, so that the afterslip distribution obtained here by the inversion of these data corresponds to that accumulated within this period (i.e., almost 1yr afterslip distribution). From the figures, it is found that the directions of horizontal GPS displacements are almost uniform and toward the southeast (i.e., toward the epicenter of the 2003 event). These horizontal displacements take the maximum value of ∼22 cm at a station near Cape Erimo, Pacific coast of Hokkaido, and decay gradually toward the inland area. In the southwestern portion of the Hokkaido and northernmost Tohoku area, there is no considerable horizontal displacement. Significant vertical displacements (uplift of ∼20 cm) can be recognized only at the two offshore PG stations.
It should be noted that vertical displacement data obtained with GPS and PG have relatively larger observation errors than horizontal ones. However, if the data are weighted in inversions based on their errors, the retrieved afterslip distributions strongly depend only on the horizontal data, and the residuals of vertical data are larger than those of horizontal ones (this is because of two reasons: (1) amount of vertical data is almost half of that of the horizontal data, (2) the vertical displacements are generally smaller than horizontal ones). This means that the vertical data have to be adequately treated in inversions. Hence, in the present study, all data are assigned an equal weight so that the afterslip distribution can be appropriately determined.
Also note that the displacement at each station shown in Fig. 4(a) and (b) may be a mixture caused by two effects on the plate interface, namely, the effect of afterslip to be estimated and that of drag (or the socalled back slip) on other portions of the plate interface due to stationary plate subduction. However, since the latter is considered to be much smaller than the former in the time span within 1 year after the 2003 event, we simply assume here that all displacements used for the inversions are those caused by only the former, i.e., afterslip. Although such simplification may introduce some bias into the estimated afterslip distributions, they can be still considered to preserve the essential feature of them.
5. Results
5.1 Checkerboard resolution test
In order to assess the resolving power of the inversion scheme described in the previous section, before inverting the actual dataset we perform a checkerboard resolution test using synthetic data calculated from an artificial slip distribution (i.e., a “checkerboard” pattern). The assumed “checkerboard” pattern consists of slips of 0.9 m and 0 m on alternating subfaults, as shown in Fig. 5(a). First, theoretical crustal displacements at all stations shown in Fig. 4(a) and (b) due to such slip distribution are calculated. Then, these theoretical values of displacements are disturbed by adding Gaussian random noise to create a synthetic dataset. Considering previous studies by, for example, Nishimura et al. (2004), the standard deviations of added Gaussian random noise are set to 1 mm and 3 mm, respectively, for horizontal and vertical displacement data.
Such synthesized data with Gaussian random noise are treated as observed ones and inverted to reproduce the “checkerboard” pattern of assumed slip distribution. The retrieved slip distribution is shown in Fig. 5(b), which should be compared with the assumed slip distribution shown in Fig. 5(a). The assumed slip pattern is found to be fairly well reproduced beneath the land area and the area within about 80–100 km off the coastline, although it has not been adequately reproduced, in general, in the offshore area far off the coastline. From this resolution test, it can be said that the distribution of the data to be used for inversion in the present study has a fairly good resolving power for most of the area where the afterslip might occur, except for the offshore area far off the coastline, so that the afterslip distributions obtained from these data are considered to be mostly reliable.
5.2 Oneyear afterslip distribution of the 2003 Tokachioki earthquake
Inverted 1yr afterslip distributions following the 2003 Tokachioki earthquake together with their error distributions (1σ standard deviations) are described below.
5.2.1 Afterslip obtained with GFs for IE model
First, the results with GFs for the IE model are presented. Figure 6(a) and (b) show the obtained 1yr afterslip and its error distributions. In this case, the most appropriate smoothness parameter α in Eq. (3) is found to be 0.022 based on the minimum ABIC of 435.4.
From the figure, it is found that significant afterslips are retrieved in three zones; the first one is a zone almost linearly running from west to southeast of Cape Erimo, the second is a zone also linearly running out to the offshore of Tokachi area, almost parallel to the first one, and the third is a linear zone located off the Tokachi running almost parallel to the coast. These three zones of significant afterslip thus form an almost Ushaped pattern, with the southwest corner of the “U” clearly extending toward the far offshore (i.e., toward the southeast). Amounts of the afterslips are mostly more than 0.45 m and even reach up to 0.9 m. The region surrounded by these significant afterslip zones has no afterslip; this is a striking feature of the obtained afterslip distribution. On the other hand, errors of afterslips are mostly less than 0.3 m, gradually increasing with increasing distance from the land area to take the maximum (∼0.75 m) error far off Cape Erimo. Such a pattern of error distribution, which is consistent with the result of the checkerboard resolution test shown in Fig. 5(b), is very natural, since almost all data used for inversion are those on land, and only a few offshore data are available. Note that, although the errors in both areas beneath the Tokachi Plain (north of Cape Erimo) and off the plain are shown with the same color in the figure corresponding to a range between 0.15 m and 0.3 m, there is some difference between them if examined in detail; the errors in the area beneath the Tokachi Plain are smaller than those in the area off the plain (the formers are less than 0.2 m while the latters are mostly between 0.2 m and 0.3 m).
5.2.2 Afterslip obtained with GFs for HE model
Next, the results with GFs for the HE model will be given. The obtained 1yr afterslip and its error distributions are shown in Fig. 7(a) and (b). In this case, ABIC takes its minimum value of 399.9, giving the most appropriate smoothness parameter α of 0.017. In order to verify the afterslip distribution shown in Fig. 7(a), we compare it with the one obtained with the GFs analytically calculated for a homogeneous elastic halfspace having the same value of elastic properties as the HE model listed in Table 1. Analytical calculations of GFs were performed using a computer program for triangular dislocations coded by W. Stuart at the United States Geological Survey (personal communication) based on Comninou and Dundurs (1975). The afterslip distribution shown in Fig. 7(a) was found to be consistent with that obtained with thus analytically calculated GFs (root mean square (RMS) discrepancy between them is 0.034 m).
The retrieved afterslip distribution pattern is mostly similar to that obtained with GFs for the IE model shown in Fig. 6(a), and amounts of the afterslips are again mostly more than 0.45 m, even reaching up to 0.9 m. However, one remarkable difference between these two cases, i.e., those with GFs for the HE and IE models, should be recognized; the extreme extension of the Ushaped significant afterslip zone in the southwest corner seen in the IE model case disappears in the HE model case. In addition, each region forming the Ushaped afterslip zone seems to be slightly thinner in the case of the HE model than that in the case of the IE model. Error distribution pattern is also similar to that in the IE model case shown in Fig. 6(b); errors of afterslips are again mostly less than 0.3 m with a maximum error of ∼0.45 m at a region far off Cape Erimo.
6. Discussion
Here we discuss the 1yr afterslip distribution following the 2003 Tokachioki earthquake obtained in the present study. First, we compare our results with those in other studies. As mentioned earlier, several authors have estimated the afterslip distribution following the 2003 Tokachioki earthquake by using GFs calculated for a uniform and homogeneous elastic halfspace or for a horizontally layered elastic media (e.g., Miura et al., 2004; Miyazaki et al., 2004; Ozawa et al., 2004; Baba et al., 2006). Choosing the result obtained by Baba et al. (2006) among these, we compare the afterslip distribution obtained here for the HE model with their result. The reasons for choosing Baba et al. (2006) to be compared with our results are as follows. First, our observational data used to derive the afterslip distribution are the same as those used by Baba et al. (2006), and second, both studies estimate only the amount of afterslips by fixing the direction of afterslips. Comparing the afterslip distribution shown in Fig. 7(a) with their estimation from the same dataset including the PGs data (i.e., figure 6(b) in Baba et al., 2006), we become aware that these two results are generally very similar to each other. Thus, it can be said that both our inversion and their inversion give almost the same afterslip distribution. However, a detailed comparison reveals some discrepancy. In our results, the region of larger afterslip can be seen more in the southern area, while in their results this region seems to be located rather in northern portion of afterslip area. This discrepancy between our estimation and their estimation may be based on the assumed geometries of subfaults in these two estimations being slightly different from each other, especially in the southwestern portion of the subfault array, though both of them are based on the plate interface model by Katsumata et al. (2003). In these two estimations, the strike and dip angle of subfaults do not strictly coincide. Baba et al. (2006) fixed the strike to 240 degrees for all subfaults, and only dip angles were adjusted to the shape of the plate interface. On the other hand, in our model, both the strike and dip angle of each subfault were adjusted to the geometry of the plate interface.
Next, as pointed out in the previous section, the most striking feature of afterslip distribution patterns shown in Figs. 6 and 7, respectively, with the GFs for the IE and HE models, is that there is an area of no afterslip almost encircled by Ushaped significant afterslip zones. The area where no afterslip is retrieved approximately coincides with the main coseismic slip zone of the 2003 event clarified from seismic inversion (e.g., Yagi, 2004). Such a pattern of afterslip distribution following this earthquake was also retrieved by Baba et al. (2006) as mentioned above. This feature of afterslip distribution pattern suggests that the coseismic rupture zone of the large earthquake and its afterslip zone are complementary with each other and has a significant role in investigation of physics of large earthquakes.
Although both of the afterslip distributions obtained with the GFs for the IE and HE models show a Ushaped pattern, there is remarkable difference in the shapes at the southwest corner; an extreme extension of significant afterslip zone, toward the far offshore in the southeast direction, can be recognized in the case of GFs for the IE model, while such an extension disappears in the case of GFs for the HE model. Of course, since the estimation errors of afterslips are rather larger there, it may not be adequate to emphasize this difference too much. However, the fact that such an extension of the significant afterslip zone at the southwest corner can be seen clearly in one case (i.e., IE case) while it can not be seen at all in another case (i.e., HE case), although the errors are similarly larger there in both cases, may suggest that this difference in the afterslip distribution between the IE and HE models reflects more or less the reality. If so, it might be of importance in any discussion of the extent of area where the elastic energy is released as afterslips.
By the way, what is the reason for this difference in afterslip distribution at the southwest corner between the IE and HE models? This difference is considered to be derived from the discrepancy of GFs between these two models. To confirm this, we compare GFs for these two models against subfaults located in this portion. Figure 8(a) illustrates the difference of GFs (horizontal components) between the IE and HE models against one of such subfaults; i.e., subfault#050, for example, which is just located, as shown in the figure, almost at the center of the extremely extending portion of the Ushaped afterslip distribution. It is obvious that there are significant differences in GFs between the IE and HE models, especially for the stations in and around Cape Erimo where the difference in GFs reaches more than 30%. On the other hand, GFs for the IE and HE models are almost identical to each other against subfaults located in the portion where the afterslip is commonly retrieved for these two models. For example, Fig. 8(b) shows GFs for the IE and HE models against subfault#221 whose location is indicated in the figure. Although we show in Fig. 8 the comparison of GFs only for horizontal components, the same features as those described here can be noticed for the vertical components of GFs. Thus, the difference in the afterslip distribution between the IE and HE models can be attributed to the discrepancy in GFs between these two models. What then does cause such large discrepancy in GFs against the subfault#050 between the IE and HE models? As seen in the figure, this subfault is located near the JapanKurile trenchtrench junction far off Cape Erimo. The area near the junction must be strongly affected by inhomogeneity due to subsurface structure, and thus the GFs against subfaults near the junction, such as subfault#050, can differ greatly between the IE and HE models. On the other hand, subfault#221 is far away from the junction, so that the effect of inhomogeneity is not so large there resulting in almost identical GFs between the IE and HE models.
Finally, in order to compare the results of afterslip distribution with GFs for the IE and HE models from another point of view, we calculate the total seismic moments released from all subfaults. In these calculations, a rigidity of 40 GPa is used for all subfaults in the HE model case, while those of 33.5 GPa, 39.7 GPa, and 53.2 GPa are respectively used for the subfaults between UC and PL, between LC and PL, and between UM and PL in the IE model case. These values of rigidity are calculated from the Young’s moduli and Poisson’s ratios for UC, LC, UM, and PL in each model (in the case of the IE model, the rigidities for subfaults between, for example, UC and PL, are assumed to be the average value of those of UC and PL). Thus, the calculated total seismic moment for the IE model case is N m (corresponding to an earthquake of M_{W} 8.0), while that for the HE model case is (0.80 ± 0.49) × 10^{21} N m (corresponding to an earthquake of M_{ W } 7.9) (note that the reason for larger error of the total seismic moment for the IE model than for the HE model comes from the fact that, as seen in Figs. 6(b) and 7(b), errors of afterslips for the IE model are larger than those for the HE model in the southern portion of the afterslip area). Hence, it can be said that the total seismic moment for the IE model is larger than that for the HE model, although the discrepancy between them may be somewhat critical since errors are not small. The difference in the total seismic moment between the IE and HE models is ∼33% when the most probable values are compared. Most of this difference is attributable to the southeastward extreme extension of the Ushaped significant afterslip zone in the southwest corner, which can be seen only in the case of the IE model. The difference also comes from the fact that, as already mentioned, each region forming the Ushaped afterslip zone is slightly thinner in the case of the HE model than that in the case of the IE model. As described in Introduction, the extent of afterslip following an interplate earthquake can play quite a significant role in discussing how much of the cumulative stress built by the plate convergence is compensated for by the co and postseismic slips, and in discussing the recurrence interval or the size of the next earthquake. Therefore, the larger seismic moment released by afterslip for the IE model than for the HE model may lengthen the recurrence interval or reduce the magnitude of the next earthquake such as the 2003 event in the Hokkaido corner; this can, in turn, influence to a certain extent the assessment of seismic hazard in this region.
In the present study, we do not incorporate other possible factors, that might affect the estimation of the afterslips, such as the viscoelastic relaxation in the upper mantle and poroelastic response in the crust as well as the Earth’s curvature; all of these may affect the surface deformation pattern to some extent. In future studies, these factors should be also incorporated as much as possible in order to make more reliable estimation of the afterslips.
7. Conclusions
In this study, we invert geodetic data of horizontal and vertical surface displacements to estimate the 1yr afterslip following the 2003 Tokachioki earthquake. In inversions, we use the GFs calculated for the inhomogeneous elastic (IE) model incorporating the subsurface structure beneath Hokkaido and Tohoku districts. For comparison, we also perform inversions with the GFs calculated for the homogeneous elastic (HE) model. The displacement data are those obtained at 142 continuous GPS stations in Hokkaido and northernmost Tohoku district and two offshore PG stations far off the Pacific coast of Hokkaido.
The results of the inversions can be summarized as follows:

(1)
Based on the GFs calculated for the IE model, the significant afterslip zone shows a Ushaped pattern with an extreme extension of the southwest corner toward the far offshore in the southeast direction. Such a Ushaped distribution pattern is the most striking feature of the significant afterslip zone. The amount of afterslip within 1yr after the 2003 event reaches up to 0.9 m, and the area with no afterslip encircled by significant afterslip zone corresponds to the area of coseismic rupture.

(2)
If the HE model is used, the significant afterslip zone is almost similar to that based on the IE model. However, a remarkable difference can be seen; the extreme extension of the Ushaped significant afterslip zone at the southwest corner recognized in the case of using GFs for the IE model disappears in this case. Besides, each region forming the Ushaped afterslip zone seems to be slightly thinner than that in the case of using GFs for the IE model.

(3)
The total seismic moment released by the afterslip estimated with the GFs for the IE model (i.e., (1.06 ± 0.60) × 10^{21} N m corresponding to an earthquake of M_{W} 8.0) is larger than that with the GFs for the HE model (i.e., (0.80 ± 0.49) × 10^{21} N m corresponding to an earthquake of M_{W} 7.9) by ∼33% (when the most probable values are compared). Such a discrepancy in the estimated seismic moment released by afterslip can influence the evaluation of the recurrence interval or the size of the next earthquake of 2003 event type in the Hokkaido corner.
Based on these results, we may conclude that the afterslip following the 2003 Tokachioki earthquake inverted with the GFs for the IE model incorporating the subsurface structure is different to a considerable extent from that with the GFs for the HE model. This suggests that, in geodetic inversions, the GFs calculated for the IE model considering the subsurface structure should be used like in the present study instead of those for the HE model.
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Acknowledgements
The GFs used in this study were calculated with GeoFEM, a parallelized finite element code developed at the Research Organization for Information Science and Technology (RIST), on the Earth Simulator (ES) at the Earth Simulator Center of Japan Agency for MarineEarth Science and Technology (JAMSTEC). The 3D finite element grid used for the calculations of GFs was originally created by Mr. Naoya Minagawa when he was student at the Graduate School of Education, Tokyo Gakugei University, with the CHIKAKU system consisting of the CHIKAKUDB, CHIKAKUCAD and CHIKAKUMESH developed at the RIKEN and the Japan Atomic Energy Agency (JAEA). We also thank Prof. Kazuro Hirahara at Kyoto University for his kind help and advice in the calculations of GFs with GeoFEM on ES. Comments from Dr. Miura of Tohoku University and an anonymous reviewer were quite useful to improve the manuscript. Most of the figures in this paper were generated with the Generic Mapping Tools (Wessel and Smith, 1998).
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Sato, K., Baba, T., Hori, T. et al. Afterslip distribution following the 2003 Tokachioki earthquake: An estimation based on the Green’s functions for an inhomogeneous elastic space with subsurface structure. Earth Planet Sp 62, 923–932 (2010). https://doi.org/10.5047/eps.2010.11.007
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DOI: https://doi.org/10.5047/eps.2010.11.007
Key words
 2003 Tokachioki earthquake
 afterslip
 geodetic inversion
 Green’s function
 inhomogeneous elastic space
 finite element method