Constraints on the early-stage rupture process of the 2011 Tohoku-oki earthquake from 1-Hz GPS data
© The Society of Geomagnetism and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; The Geodetic Society of Japan; The Japanese Society for Planetary Sciences; TERRAPUB. 2012
Received: 27 December 2011
Accepted: 20 September 2012
Published: 28 January 2013
From the comparison of observed 1-Hz GPS data with simple forward computation that evaluates near and intermediate field terms, we put constraints on the early-stage rupture process of the 2011 Tohoku-oki earthquake. Mainly based on the time difference of the onset of large eastward displacements at stations along the northern coast of the source region, we estimate that the first significant moment release started around 35 km west of the hypocenter determined by JMA. The moment release occurred approximately from 20 s to 35 s after the initiation of the earthquake. Significant moment release around the hypocenter and in the near-trench region started from 25 s, and 35 s, at the earliest, respectively. Before about 20 s, the moment release of the 2011 Tohoku-oki earthquake must have been so small that any substantial displacements were not observed on land. The clear opposite motion that follows the large eastward displacement observed at many stations is due to the intermediate S-wave term.
Key wordsThe 2011 Tohoku-oki earthquake 1-Hz GPS rupture process near field term intermediate S-wave term
In order to understand the 2011 Tohoku-oki earthquake, it is crucially important to clarify the rupture process. Especially, the early-stage rupture process probably holds the principal key as to why the earthquake grew as large as magnitude 9. Many rupture models have been proposed for this earthquake mainly from seismic waveform inversion. These results have some common features, such as very large slip near the trench around 60 to 80 s (Ide et al., 2011; Lee et al., 2011; Shao et al., 2011; Suzuki et al., 2011; Yagi and Fukahata, 2011; Yoshida, K. et al., 2011; Yoshida, Y. et al., 2011; Yue and Lay, 2011) as well as the form of the moment-rate function, which has a shoulder around 35 s, a large peak at about 70 s, and which decreases to zero roughly at 150 s (Ammon et al., 2011; Hayes, 2011; Lay et al., 2011; Lee et al., 2011; Shao et al., 2011; Suzuki et al., 2011; Yagi and Fukahata, 2011; Yoshida, Y. et al., 2011; Yue and Lay, 2011), where time is measured from the initiation of the earthquake. However, the results of seismic waveform inversion show a significant difference in the rupture process during the initial 30 or 40 s. In some analyses, the rupture continues around the hypocenter (Shao et al., 2011; Yoshida, K. et al., 2011; Yoshida, Y. et al., 2011), whereas, in other analyses, large moment release occurs only in the down-dip (Ide et al., 2011; Koketsu et al., 2011), up-dip (Lee et al., 2011), or both regions (Yagi and Fukahata, 2011).
Other than seismic waveform inversion, a back projection analysis, using the Metropolitan Seismic Observation Network (MeSO-net) that passes through the Tokyo Metropolitan area, shows moment release both in the down-dip and up-dip regions (Honda et al., 2011). The MeSO-net data is considered to have a better resolution for the across-arc direction rather than the along-arc direction, because of the spatial relation between the network and the source area of the earthquake. The generation area of the first strong motion was commonly estimated in the down-dip region from the hypocenter based on the analysis of near-field strong motion data (Asano and Iwata, 2012; Suzuki et al., 2011; Yoshida, Y. et al., 2011). However, the strong motion data have defects in that they are limited in resolution in the across-arc direction, and their amplitude can be larger as a result of fast slip-rate change rather than large slip itself.
1-Hz GPS data observed by the Geospatial Information Authority (GSI) can give important constraints on this problem. Because GPS data record displacements, even if the sampling rate is high, the GPS data are more directly related with the moment release during the rupture process. In this paper, by comparing simple forward computation with observed 1-Hz GPS data, we aim to clarify the early stage rupture process of the 2011 Tohoku-oki earthquake.
2. 1-Hz GPS Data
Time series of surface displacements are recorded by the GPS Earth Observation Network (GEONET), operated by the Geospatial Information Authority (GSI) of Japan. GPS phase data with a sampling interval of one second are processed with a precise point positioning strategy implemented in the GIPSY-OASIS II software (Zumberge et al., 1997). The final (precise) orbits and clocks produced by the Jet Propulsion Laboratory (JPL) are used, and phase ambiguities are resolved.
The largest displacement in the GEONET was recorded at Oshika. In each station, we can note a very large eastward displacement with a clear time difference from south to north. Interestingly, the large eastward displacement is followed by significant opposite motion. The north-south and vertical displacements are relatively small during the initial 80 s, but the southward displacement at the peak (about 100 s) exceeds 2 m at Kesen-numa and Kamaishi, which is larger than that at Oshika. The southward displacements are also followed by the opposite (northward) displacements. The vertical displacement is largest at Oshika and decreases from south to north.
3. Displacement Due to Dislocation Source
The onset of displacement is marked by the arrival of a P-wave. Displacement usually shows a peak at the arrival of an S-wave and significantly moves in the opposite direction after that. This opposite motion is caused by the intermediate S-wave term. In some cases, the opposite motion overwhelms the previous displacement (e.g., the vertical component in Fig. 3). When ΔT is 5 s, in comparison with ΔT = 10 s, displacement during the initial 5 s is exactly the same and the final displacement (static displacement) is exactly half.
The setting of the computation of Fig. 3 is very simple: we assumed a homogeneous infinite medium. Hence, we cannot discuss absolute values of moment from a comparison of this computation to observed data. However, the arrival timing of P- and S-waves in Fig. 3 should be almost correct to an accuracy of probably less than 10%, from the comparison of travel times with a few representative structure models, such as PREM, CRUST 2.0 (Bassin et al., 2000), and others (e.g., Yagi et al., 2012). The sense of displacement (the position of nodal planes), and the relative amplitude of displacements, are also considered to be basically correct from the analogy of static displacements between an infinite elastic medium and a stratified elastic half-space (Fukahata and Matsu’ura, 2005). Although we cannot discuss short-period displacements because of the neglect of the far-field terms, the travel times of the far-field terms are the same as those of the intermediate terms.
4. Estimation of Early Rupture Process
The computed feature of a large eastward displacement followed by a significant opposite motion (Fig. 4) corresponds well to the observed displacement (Fig. 2). As mentioned above, seismic waveform inversion results commonly show a very large slip near the trench around 60 to 80 s. Therefore, the large slip near the trench is considered to be the principal cause of this distinct observed GPS displacement. If we take into account the rigidity contrast along the plate interface (Lay et al., 2011) and the difference of sensitivity of displacement to a dislocation source (Fig. 4), the slip around the hypocenter may also greatly contribute to this distinct GPS displacement. In either case, subsidence and northward motions observed at each station around 2 minutes is consistent with the synthetic computation. As mentioned above, however, displacement at each station is generally caused by dislocation sources at various locations and timings. So, it is not easy to separate the various contributions to displacement except during the early stage.
From Fig. 4, we can see a large eastward displacement at Oshika for every source location. On the other hand, eastward displacements are very small at Kamaishi and Miyako for the down-dip source, and the eastward displacement is again very small at Miyako for the hypocenter source. The observed GPS data (Fig. 2) show that significant displacement at Oshika starts at about 32 s. On the other hand, the eastward displacement at Kamaishi is very small before 50 s and becomes larger after 60 s. At Miyako, substantial eastward displacement starts around 68 s. If the significant displacement at Oshika is caused by dislocation around the hypocenter, or in the up-dip region, substantial eastward displacement at Kamaishi must be recorded with several seconds delay. Therefore, the first significant moment release must start in the down-dip region.
The eastward displacement at Kamaishi gradually grows from 50 s to 60 s (Fig. 2). The eastward displacement of this period may be caused by the dislocation source around the hypocenter, but it is also possible that the same source responsible for the significant displacement at Oshika from 32 s causes this movement. As shown in Fig. 5, static eastward displacement at Kamaishi amounts to about 15% of that at Oshika. However, the displacement after 60 s at Kamaishi is much larger, and so the source location must be different. If the source locates around the up-dip point, as shown in Fig. 4(c), the eastward displacement at Ka-maishi must be followed by that at Miyako with a few seconds delay. Therefore, the onset of substantial eastward displacement at Kamaishi is not due to the source near the trench, but maybe around the hypocenter. In short, taking the travel time shown in Fig. 4(b) into account, the moment release around the hypocenter started from about 25 s if it caused the eastward displacement from 50 s at Kamaishi, and started from about 35 s if it caused the eastward displacement from 60 s. However, it is not easy to completely exclude the possibility that this significant eastward motion at Kamaishi was caused by a down-dip source to the north of the northern open circle in Fig. 1. Then, northward motion must transiently arrive at Oshika, but such motion can be cancelled out by the southward displacement due to other sources to the south.
Because substantial displacement starts around 68 s at Miyako, significant moment release in the up-dip region is considered to start around 35 s (Fig. 4(c)). Again, this estimate is the earliest timing. In fact, significant moment release must occur in the region to the north of the hypocenter and the assumed near-trench source (open square in Fig. 1) as well, because a clear westward motion after peaking in the eastward displacement (about 120 s) is observed even in Miyako (Figs. 2 and 4(c)).
5. Discussion and Conclusions
As mentioned above, the results of seismic waveform inversion commonly show a shoulder in the moment-rate function at around 35 s. The observed eastward displacements at Oshika, Kesen-numa, and the stations in Fig. 7, also have clear shoulders approximately from 55 s to 70 s (Figs. 2 and 7(a)). As shown in Figs. 5 and 7(b), these observed data can be well explained by a cessation of significant moment release roughly at 35 s. That is to say, in the 2011 Tohoku-oki earthquake, significant moment release first occurred in the down-dip region approximately from 20 s to 35 s, which is well consistent with the inversion result of Yagi and Fukahata (2011). The shoulder of the moment-rate function is considered to be caused in this way. On the other hand, significant moment release near the trench started after 35 s, which is clearly later than their result. A large moment release, first in the down-dip region, followed by a large slip near the trench, well corresponds to the inversion result of Ide et al. (2011), but the timing of the transition is later and the location of large down-dip slip is apparently too close to the coast in their result.
Analyses of high-rate GPS data are relatively new (e.g., Ji et al., 2004; Miyazaki et al., 2004; Ammon et al., 2011; Yue and Lay, 2011; Ohta et al., 2012; Wright et al., 2012). However, as shown by this study, high-rate GPS data contain rich information about the rupture process of earthquakes. For example, the southward displacement at Watari after 100 s is considered to correspond to the rupture propagation southward in the later stage of the 2011 Tohoku-oki earthquake (e.g., Suzuki et al., 2011; Koketsu et al., 2011; Yagi and Fukahata, 2011; Yue and Lay, 2011). Fast downward displacement around 90 to 95 s at Oshika is accompanied by fast southward and eastward displacements. This motion may be caused by a dislocation source to the south of the down-dip square and to the west of the southern open circle in Fig. 1. To fully extract the rich information from high-rate GPS data is an interesting challenge.
The figures were created with the GMT software by Paul Wessel and Walter H. F. Smith (Wessel and Smith, 1998). We thank anonymous reviewers for useful comments. This study was supported by Grant-in-Aid for Scientific Research No. 21540428 and 24540450 of the Japan Ministry of Education, Culture, Sports, Science and Technology to YF and YY.
- Aki, K. and P. G. Richards, Quantitative Seismology, Volume I, 557 pp, W. H. Freeman and Company, New York, 1980.Google Scholar
- Ammon, C. J., T. Lay, H. Kanamori, and M. Cleveland, A rupture model of the 2011 off the Pacific coast of Tohoku Earthquake, Earth Planets Space, 63, 693–696, 2011.View ArticleGoogle Scholar
- Asano, K. and T. Iwata, Source model for strong ground motion generation in the frequency range 0.1–10 Hz during the 2011 Tohoku earthquake, Earth Planets Space, 64, this issue, 1111–1123, 2012.View ArticleGoogle Scholar
- Bassin, C., G. Laske, and G. Masters, The current limits of resolution for surface wave tomography in North America, Eos Trans. AGU, 81, 897, 2000.Google Scholar
- Fukahata, Y. and M. Matsu’ura, General expressions for internal deformation fields due to a dislocation source in a multilayered elastic half-space, Geophys. J. Int., 161, 507–521, 2005.View ArticleGoogle Scholar
- Hayes, G. P., Rapid source characterization of the 2011 Mw 9.0 off the Pacific coast of Tohoku Earthquake, Earth Planets Space, 63, 529–534, 2011.View ArticleGoogle Scholar
- Honda, R., Y. Yukutake, H. Ito, M. Harada, T. Aketagawa, A. Yoshida, S. Sakai, S. Nakagawa, N. Hirata, K. Obara, and H. Kimura, A complex rupture image of the 2011 off the Pacific coast of Tohoku Earthquake revealed by the MeSO-net, Earth Planets Space, 63, 583–588, 2011.View ArticleGoogle Scholar
- Ide, S., A. Baltay, and G. C. Beroza, Shallow dynamic overshoot and energetic deep rupture in the 2011 Mw 9.0 Tohoku-oki earthquake, Science, 332, 1426–1429, 2011.View ArticleGoogle Scholar
- Ji, C., K. M. Larson, Y. Tan, K. W. Hudnut, and K. Choi, Slip history of the 2003 San Simeon earthquake constrained by combining 1-Hz GPS, strong motion, and teleseismic data, Geophys. Res. Lett., 31, L17608, doi:10.1029/2004GL020448, 2004.Google Scholar
- Koketsu, K., Y. Yokota, N. Nishimura, Y. Yagi, S. Miyazaki, K. Satake, Y. Fujii, H. Miyake, S. Sakai, Y. Yamanaka, and T. Okada, A unified source model for the 2011 Tohoku earthquake, Earth Planet. Sci. Lett., 310, 480–487, 2011.View ArticleGoogle Scholar
- Lay, T., C. J. Ammon, H. Kanamori, L. Xue, and M. J. Kim, Possible large near-trench slip during the 2011 Mw 9.0 off the Pacific coast of Tohoku Earthquake, Earth Planets Space, 63, 687–692, 2011.View ArticleGoogle Scholar
- Lee, S. J., B. S. Huang, M. Ando, H. C. Chiu, and J. H. Wang, Evidence of large scale repeating slip during the 2011 Tohoku-Oki earthquake, Geophys. Res. Lett., 38, L19306, doi:10.1029/2011GL049580, 2011.Google Scholar
- Matsu’ura, M., Deformation and fracture, in Earth and Planetary Science 6: Earth’s Continuum Mechanics, 175–237, Iwanami Shoten, 1996 (in Japanese).Google Scholar
- Miyazaki, S., K. M. Larson, K. Choi, K. Hikima, K. Koketsu, P. Bodin, J. Haase, G. Emore, and A. Yamagiwa, Modeling the rupture process of the 2003 September 25 Tokachi-Oki (Hokkaido) earthquake using 1 Hz GPS, Geophys. Res. Lett., 31, L21603, doi:10.1029/2004GL021457, 2004.Google Scholar
- Ohta, Y., T. Kobayashi, H. Tsushima, S. Miura, R. Hino, T. Takasu, H. Fujimoto, T. Iinuma, K. Tachibana, T. Demachi, T. Sato, M. Ohzono, and N. Umino, Quasi real-time fault model estimation for near-field tsunami forecasting based on RTK-GPS analysis: Application to the 2011 Tohoku-Oki earthquake (Mw 9.0), J. Geophys. Res., 117, B02311, doi:10.1029/2011JB008750, 2012.Google Scholar
- Shao, G., X. Li, C. Ji, and T. Maeda, Focal mechanism and slip history of the 2011 Mw 9.1 off the Pacific coast of Tohoku Earthquake, constrained with teleseismic body and surface waves, Earth Planets Space, 63,559–564, 2011.View ArticleGoogle Scholar
- Suzuki, W., S. Aoi, H. Sekiguchi, and T. Kunugi, Rupture process of the 2011 Tohoku-Oki mega-thrust earthquake (M9.0) inverted from strong-motion data, Geophys. Res. Lett., 38, L00G16, doi:10.1029/2011GL049136, 2011.Google Scholar
- Wessel, P. and W. H. F. Smith, New, improved version of generic mapping tools released, Eos Trans. AGU, 79, 579, 1998.View ArticleGoogle Scholar
- Wright, T. J., N. Houlié, M. Hildyard, and T. Iwabuchi, Real-time, reliable magnitudes for large earthquakes from 1 Hz GPS precise point positioning: the 2011 Tohoku-Oki (Japan) earthquake, Geophys. Res. Lett., 39, L12302, doi:10.1029/2012GL051894, 2012.View ArticleGoogle Scholar
- Yagi, Y. and Y. Fukahata, Rupture process of the 2011 Tohoku-oki earthquake and absolute elastic strain release, Geophys. Res. Lett., 38, L19307, doi:10.1029/ 2011GL048701, 2011.View ArticleGoogle Scholar
- Yagi, Y., A. Nakao, and A. Kasahara, Smooth and rapid slip near the Japan Trench during the 2011 Tohoku-oki earthquake revealed by a hybrid back-projection method, Earth Planet. Sci. Lett., 355–356, 94–101, 2012.View ArticleGoogle Scholar
- Yoshida, K., K. Miyakoshi, and K. Irikura, Source process of the 2011 off the Pacific coast of Tohoku Earthquake inferred from waveform inversion with long-period strong-motion records, Earth Planets Space, 63, 577–582, 2011.View ArticleGoogle Scholar
- Yoshida, Y., H. Ueno, D. Muto, and S. Aoki, Source process of the 2011 off the Pacific coast of Tohoku Earthquake with the combination of teleseismic and strong motion data, Earth Planets Space, 63, 565–569, 2011.View ArticleGoogle Scholar
- Yue, H. and T. Lay, Inversion of high-rate (1 sps) GPS data for rupture process of the 11 March 2011 Tohoku earthquake (Mw 9.1), Geophys. Res. Lett., 38, L00G09, doi:10.1029/2011GL048700, 2011.View ArticleGoogle Scholar
- Zumberge, J. F., M. B. Heflin, D. C. Jefferson, M. M. Watkins, and F. H. Webb, Precise point positioning for the efficient and robust analysis of GPS data from large networks, J. Geophys. Res., 102, 5005–5017, 1997.View ArticleGoogle Scholar