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Rapid and quantitative uncertainty estimation of coseismic slip distribution for large interplate earthquakes using realtime GNSS data and its application to tsunami inundation prediction
Earth, Planets and Space volume 74, Article number: 24 (2022)
Abstract
This study proposes a new method for the uncertainty estimation of coseismic slip distribution on the plate interface deduced from realtime global navigation satellite system (GNSS) data and explores its application for tsunami inundation prediction. Jointly developed by the Geospatial Information Authority of Japan and Tohoku University, REGARD (REaltime GEONET Analysis system for Rapid Deformation monitoring) estimates coseismic fault models (a single rectangular fault model and slip distribution model) in real time to support tsunami prediction. The estimated results are adopted as part of the Disaster Information System, which is used by the Cabinet Office of the Government of Japan to assess tsunami inundation and damage. However, the REGARD system currently struggles to estimate the quantitative uncertainty of the estimated result, although the obtained result should contain both observation and modeling errors caused by the model settings. Understanding such quantitative uncertainties based on the input data is essential for utilizing this resource for disaster response. We developed an algorithm that estimates the coseismic slip distribution and its uncertainties using Markov chain Monte Carlo methods. We focused on the Nankai Trough of southwest Japan, where megathrust earthquakes have repeatedly occurred, and used simulation data to assume a Hoeitype earthquake. We divided the 2951 rectangular subfaults on the plate interface and designed a multistage sampling flow with stepwise perturbation groups. As a result, we successfully estimated the slip distribution and its uncertainty at the 95% confidence interval of the posterior probability density function. Furthermore, we developed a new visualization procedure that shows the risk of tsunami inundation and the probability on a map. Under the algorithm, we regarded the Markov chain Monte Carlo samples as individual fault models and clustered them using the kmeans approach to obtain different tsunami source scenarios. We then calculated the parallel tsunami inundations and integrated the results on the map. This map, which expresses the uncertainties of tsunami inundation caused by uncertainties in the coseismic fault estimation, offers quantitative and real time insights into possible worstcase scenarios.
Graphical Abstract
Introduction
A rapid understanding of the magnitude and fault areas of large earthquakes is crucial for disaster response. Numerous studies have shown the advantages of the highrate (typically 1 Hz) global navigation satellite system (GNSS) as a broadband sensor that can directly measure displacement without saturation (e.g., Larson et al. 2003; Ohta et al. 2006; Larson 2009). The use of onshore highrate GNSS data enable the rapid estimation of offshore finite fault models that are expected to be used for tsunami prediction (e.g., Blewitt et al. 20062009; Ohta et al. 2012; Melgar et al. 2012; Tsushima et al., 2014; Tsushima and Ohta 2014; Ohta 2016). The Geospatial Information Authority of Japan (GSI) operates a nationwide continuous GNSS network called GEONET. After the massive tsunami caused by the 2011 TohokuOki earthquake, the GSI and Tohoku University jointly developed the REGARD system (REaltime GEONET Analysis system for Rapid Deformation monitoring, Kawamoto et al. 2016, 2017), which consists of realtime GNSS positioning, automatic detection of coseismic displacement, and quasirealtime finite fault model inversion routines.
The finite fault models estimated by REGARD are helpful for obtaining the initial sea surface distribution for tsunami forecasting. The consortium led by Tohoku University has developed a realtime damage estimation system for tsunami inundation using the REGARD fault model as an initial tsunami source model (Musa et al. 2018; Ohta et al. 2018). This system is expected to be used for the initial response of the government when a disaster occurs.
For the 2016 Kumamoto earthquake (M_{w} 7.0), REGARD successfully estimated a single rectangular fault model automatically in real time (Kawamoto et al. 2016). However, estimation using only onshore GNSS data does not necessarily provide accurate estimates of offshore fault areas. From this point of view, in the single rectangular fault model, Ohno et al. (2021) developed a new method to quantitatively evaluate the uncertainties of the estimated results using the Bayesian inversion approach. This study showed a tradeoff between the fault area and slip amount, especially for offshore earthquakes, which affects the initial wave field of the tsunami. In the slip distribution model of REGARD, quantitative evaluation of the uncertainty is also essential because of the effects of station arrangement, modeling errors, and constraints on slip smoothing. For example, in the case of the 2011 TohokuOki earthquake, it was suggested that there was a large slip around the trench axis based on seafloor geodetic data (e.g., Iinuma et al. 2012), although such slip was not significantly suggested using only onshore GNSS data (e.g., Melgar and Bock 2015).
The quantification of the uncertainty of fault models enables us to consider the accuracy of tsunami predictions calculated based on them. With the underestimation of tsunami wave height in the 2011 TohokuOki earthquake as a lesson, the danger of announcing tsunami predictions as a single value has been proposed. The Japan Meteorological Agency (JMA) introduced the announcement of tsunami warnings with more qualitative expressions (JMA 2012). In addition, several studies have shown a method for adding uncertainty information to tsunami prediction (e.g., Sraj et al. 2014; Fukutani et al. 2015; Takagawa and Tomita 2015; Dettmer et al. 2016; Goda and Song 2016; Gibbons et al. 2020; Goda et al. 2020; Mulia et al. 2020; Giles et al. 2021). Dettmer et al. (2016) evaluated the uncertainty of the initial sea surface displacement in the 2011 TohokuOki earthquake deduced from tsunami waveforms using a transdimensional algorithm based on wavelet decomposition of the displacement field. Goda et al. (2020) presented an extensive tsunami hazard assessment for Nankai–Tonankai trough events using 1000 kinematic earthquake rupture models for Monte Carlo tsunami simulations. Giles et al. (2021) proposed a workflow that integrates the entire chain of components from the tsunami source to quantify hazard uncertainties by approximating the functionally complex and computationally expensive highresolution tsunami simulations with a simple and cheap statistical emulator. On the other hand, in the damage estimation system due to tsunami inundation, it is currently difficult to evaluate the impact of the uncertainty of fault models on tsunami prediction.
With this background, the purpose of this study was to add uncertainty information to tsunami inundation estimation by quantifying the uncertainty of the coseismic slip distribution model estimated from onshore realtime GNSS data. We propose a "stepwise partitioning algorithm,” for estimating coseismic slip distribution using Markov chain Monte Carlo methods (MCMC). Furthermore, we propose a "realtime tsunami inundation risk map,” which visualizes the probability of risk of tsunami inundation based on the uncertainty of the estimated fault model. We verified the performance of this approach by applying it to simulated data in the Nankai Trough area.
Methods
Stepwise partitioning algorithm
Conventionally, the slip distribution model is estimated with a hyperparameter governing the intensity of slip smoothing constraints determined with an index, such as ABIC (Akaike's Bayesian Information Criterion, Akaike 1980; e.g., Fukahata 2009). The error matrix obtained in this case is essential for interpreting the uncertainty of slip amount at each subfault. These methods are highly relevant in terms of obtaining a single most likely solution and its error. In other words, with these approaches, it is difficult to obtain multiple models that can explain the observed data, and the discussion of the errors remains a challenge. It is important to present several possible models with errors, while satisfying the observed data, to treat the obtained results as disaster information. Recently, many studies have adopted the Bayesian approach to geodetic studies because of its advantages in quantifying uncertainty (Ito et al. 2012; Dettmer et al. 2014; Minson et al. 2014a2014b; Jiang and Simons 2016; Ohno and Ohta 2018; Ohno et al. 2021). Owing to its sampling process, MCMC can generate a large number of model samples and quantify the uncertainty as probability density function (PDF), which is the ensemble of those samples. In this study, we regarded the diversity of samples as individual slip distribution models that can explain the observation data to evaluate the uncertainties of tsunami inundation caused by uncertainties in the estimation of coseismic slip distribution. Furthermore, to get the diversity of samples efficiently in realtime, essentially similar to smoothing constraint, but we tried a different approach to regularization.
We adopted simulated data based on the assumed Mw 8.75 1707 Hoei earthquake (Furumura et al. 2011; Todoriki et al. 2013; Inoue et al. 2016; Kawamoto et al. 2017). The assumed slip reached from Suruga Bay to the westernmost part of Shikoku (Fig. 1). Let \({\varvec{\theta}}\) be a model parameter vector that contains slip amounts on subfaults along the plate boundary in the Nankai Trough, and \({\varvec{d}}\) be a permanent displacement data vector with three components (horizontal and vertical components) based on realtime GNSS observations. We used the same method as Ohno et al. (2021) for MCMC sampling. Bayesian estimation of the unknown model parameters conditional on the observations is based on Bayes’ theorem:
where \({\varvec{p}}\left({\varvec{d}}\right)\) is a PDF of the observations, \({\varvec{p}}\left({\varvec{\theta}}\right)\) is a prior PDF of the model parameters, \({\varvec{p}}\left({\varvec{d}}{\varvec{\theta}}\right)\) is a likelihood function, and \({\varvec{p}}\left({\varvec{\theta}}{\varvec{d}}\right)\) is a posterior PDF of the model parameters. Note that \({\varvec{p}}\left({\varvec{d}}\right)\) is constant, because observations are fixed values and, hence, the posterior PDF is proportional to the product of the prior PDF and likelihood function. The likelihood function measures the degree of fit between the observed data \({\varvec{d}},\) and calculated data \(\widehat{{\varvec{d}}}\left({\varvec{\theta}}\right)\). The residuals are given by \({\varvec{r}}\left({\varvec{\theta}}\right)=\widehat{{\varvec{d}}}\left({\varvec{\theta}}\right){\varvec{d}}\). When the number of observation stations is \(N\), the dimension of \({\varvec{d}} \mathrm{is} 3N\). Assuming that the estimation error follows a normal distribution function, the likelihood function is defined as follows:
where \({\sigma }_{ij} (i=E (\mathrm{East}), N (\mathrm{North}), U (\mathrm{UpDown}))\) (which is identical at every GNSS station) is an eventdependent hyper parameter that includes modeling and observation errors. This study assumed the hyper parameters for each horizontal and vertical components as follows:
where \({e}_{ij}\) is the steady noise of realtime GNSS observations. We used \({0.1d}_{ij}\) as the proxy for the modeling and observation errors and assumed \({\sigma }_{ij}\) on each component at each station is whichever of those two error sources is larger. By assuming that \({\sigma }_{ij}\) depends on the displacement while keeping the realtime GNSS steady noise as a lower bound, we can prevent the model from overfitting the data. We used the Metropolis–Hasting method as the MCMC sampler (hereafter, M–H method; Metropolis et al. 1953; Hastings 1970). We adopted parallel tempering with eight parallel chains to improve the search efficiency (Geyer 1991; Jasra et al. 2007). For simplicity of the realtime analysis, we fixed rake angles to 90°; as such, \({\varvec{\theta}}\) contains only slip amounts, the element number of which is the same as that of the subfaults. In addition, we assumed the slip amounts to be nonnegative, which is equivalent to assuming that the prior PDF formed a uniform distribution \(\mathrm{U}\left(0, \infty \right)\) for \({\varvec{\theta}}\). Incorporating nonnegative slip constraint into the inversion as a search range setting is one of the advantages of the MCMC sampling process over conventional methods. There were 2951 subfaults on the plate boundary. We adopted the analytical solution of Okada (1992) as the Green’s function for rectangular subfaults, where the fault width are approximately 8 km.
In the M–H method, we propose new transition candidates by applying random perturbations \(\Delta{\varvec{\theta}}\) with uniform distribution between \({\Delta{\varvec{\theta}}}_{\mathrm{max}}\) and + \({\Delta{\varvec{\theta}}}_{\mathrm{max}}\). However, applying MCMC to such a problem with many unknown parameters takes a long time to converge. Therefore, in addition to parallel tempering, we improved the search efficiency using a multistage approach with stepwise partitioning of perturbation groups. Figure 2 shows an overview of the "stepwise partitioning algorithm". The Markov chain was divided into four stages (number of steps in each chain): stage 1 (\(3\times {10}^{6}\) steps); stage 2 (\(3\times {10}^{6}\) steps); stage 3 (\(3\times {10}^{6}\) steps); and stage 4 (\(3\times {10}^{6}\) steps). In each stage, we set spatial perturbation groups in advance, because grouping \(\Delta{\varvec{\theta}}\) around subfaults promoted convergence. Thus, we applied the same perturbation \(\Delta{\varvec{\theta}}\) to the samecolored subfaults, as shown in Fig. 2; we refer to these predetermined areas with the same \(\Delta{\varvec{\theta}}\) as "perturbation groups". The number of perturbation groups are 80, 185, 388, and 1451 for stage 1, 2, 3, and 4, respectively. Increasing the number of perturbation groups as the stage progresses allows us to estimate the roughtodetailed features. The utilization of such a grouping is equivalent to reducing the number of unknown parameters. It should be noted that we did not change the shapes of the 2951 rectangular subfaults; that is, only the perturbation groups were changed. Thus, the analytical displacements in each step were calculated for 2951 background subfaults using a constant each subfault’s Green's function.
As shown in Fig. 2, in the transition between stages, we used the median of the posterior PDFs of the previous stage as the initial value for the next stage and used the 95% confidence interval (CI) as the amount of perturbation \({\Delta{\varvec{\theta}}}_{\mathrm{max}}\) for the next stage. By inheriting the uncertainty as the transition amount, we searched for a broader slip amount with more uncertainty in a limited number of samples. Therefore, in the initial 10% of samples for each stage, we adjusted \({\Delta{\varvec{\theta}}}_{\mathrm{max}}\) by equal multiplication so that the acceptance rate would be 20–40% (e.g., Roberts and Rosenthal 2001), and the samples under adjustment were discarded during PDF generation as burnin. In addition to the model parameters, we also calculated Variance Reduction (VR) for evaluation of the estimated model:
In the later stage, the partitioning may be excessive for the sensitivity of the data and earthquake magnitude. We calculated the AIC (Akaike's Information Criterion, Akaike 1973) using the following equation to determine the optimum stage:
where \(L\) indicates the maximum likelihood, and \(M\) indicates the number of unknown parameters, which is the number of perturbation groups in each stage.
The approach presented above is similar to the transdimensional approach (e.g., Dettmer et al. 2014), but our algorithm was designed to force change in one direction to simplify the problem for realtime purposes. Moreover, our procedure is predefined by a set of perturbation groups with different spatial resolutions. Then, an optimum stage is selected based on AIC corresponding to a regularization process similar to smoothing constraints with discrete search (i.e., 4 stages) of regularization parameters. We designed this approach to automatically generate various models with the appropriate spatial resolution for the magnitude of the target earthquake without smoothing constraints between adjacent subfaults. The subsequent tsunami calculation process ("Realtime tsunami inundation risk map" section) utilizes samples from one selected stage rather than multiple stages. In each stage with the constant spatial resolution, we can benefit from sampling without smoothing constraints as a diversity of multiple samples.
The computation time of this approach is within 30 min for each stage (\(3\times {10}^{6}\) steps in each chain) using an SXAurora TSUBASA Type20B processor with eight parallel chains in the case of 642 GNSS stations. In this study, we decided the number of samples with the highest priority to obtain a sufficient number to evaluate the differences between the stages. For realtime utilization, the convergence judge (e.g., Gelman 1996) should be introduced and must move to the next stage automatically. According to the estimated results of this paper, the number of chains in each stage seems to converge at about 10% of the number of advance settings. Based on this, if we could design convergence judges and AIC staging decisions properly, it is possible to complete the calculation up to stage 2 in approximately 6 min, which is a computation time that may be used in real time in the future.
Realtime tsunami inundation risk map
In general, because the tsunami inundation calculation is a nonlinear problem, it is difficult to evaluate the uncertainty of the tsunami inundation based on a single coseismic fault slip model and variation index, such as standard deviation of slip amounts. Therefore, to evaluate this uncertainty, we need to prepare multiple coseismic fault slip models that explain the data well. However, it is not realistic to calculate tsunami inundation for all MCMC samples, even if calculation speed were to improve in the future. Therefore, our algorithm aims to efficiently classify MCMC samples and integrate multiple tsunami inundation scenarios to probabilistically present tsunami inundation risk. Here, assuming that multiple calculations of \({10}^{2}\) orders will be possible within a time of several minutes in the future, we added "realtime" to the flow name in this study.
Figure 3 shows a flow chart of the realtime tsunami inundation risk map process.

i.
Obtain sufficient MCMC samples to evaluate the uncertainty of the slip distribution model ("Stepwise partitioning algorithm" section). Samples from which VR was extracted are equivalent to a representative value based on the posterior PDF.

ii.
Classify these samples into small clusters (K) using the kmeans approach using \({\varvec{\theta}}\) as the feature value.

iii.
Generate K representative slip distributions (using the median value of each subfault), and use them as inputs to calculate individual K tsunami inundations.

iv.
Count the number of inundations on the map.
The resulting map shows the possible tsunami arrival rate in each computation grid based on the uncertainty of fault slip estimated from realtime GNSS data.
The main feature of our algorithm is the clustering of MCMC samples, whereas generally utilize posterior PDFs. As discussed, the nonlinearity of tsunami inundation calculation is a problem, so we need to obtain sufficient fault models to evaluate the tsunami risk. In contrast, samples using the M–H method are not necessarily independent, because the M–H method proposes samples by perturbing the previous one. We adopted the kmeans method (Steinhaus, 1956) to classify the samples into a predetermined number, with the number of clusters K determined by considering the computational cost of tsunami inundation, the availability of denominators for probability display, and the maintenance of the diversity of MCMC samples. The feature value used for clustering is the slip vector \({\varvec{\theta}}\), because the clustering phase does not depend on the specific target region of the tsunami calculation. Samples with the same VR were used to ensure fairness in terms of reproducibility of the observed data.
Here, the target of the tsunami inundation calculation was a 1563 km^{2} area between Tosa City and Aki City in Kochi Prefecture (red box in Additional file 1: Figure S1). Additional file 1: Table S1 lists the conditions of the tsunami inundation calculation. The grid size in the target area was 30 × 30 m, and the number of grids was 1,736,388 (2,082 grids along the east–west direction and 834 grids along the north–south direction). Tsunami propagation and inundation were calculated using the TUNAMI code (Tohoku University's numerical analysis model for investigating tsunami), which numerically solves the nonlinear shallow water equation using the staggered leapflog finite difference method (Imamura 1995). The tsunami simulation was carried out from the time of the earthquake to 6 h later. The fracture propagation of the earthquake was not considered, and the slip was assumed to be instantaneous. We calculated seafloor displacement using the analytical result of Okada (1992), and the uplift of the seawater due to the horizontal movement of the seafloor was considered (Tanioka and Satake 1996). Coastal structures, such as breakwaters, were input as line data every 30 m and were not breached by earthquakes or tsunamis; buildings were not considered. We used the maximum inundation depth up to 6 h after each calculation grid as the inundated depth.
Results
Uncertainty of slip distribution
We applied the stepwise partitioning algorithm ("Stepwise partitioning algorithm" section) to the simulated data—that is, displacement data at 642 GEONET stations calculated using the analytical result of Okada (1992) with Gaussian noise (standard deviation of 2 cm horizontally and 5 cm vertically).
Figure 4 shows the estimation results for four stages: median of the posterior PDFs and the 95% CI which was calculated from the difference between samples located at 2.5% and those at 97.5%. For all stages, the estimated fault model based on the median value well reproduced the observed data. However, the 95% CI was large, especially near the trough axis, and increased from near the land toward the offshore. This suggests that slip was well estimated in regions with large slip, while that offshore had low estimated resolution.
As the number of perturbation groups increased with the progress of the stage, the obtained slip distribution consisted of slips with shorter wavelengths (Fig. 4). In particular, in stage 4, a large amount of local slip occurred on certain small perturbation groups. Figure 5 shows the Markov chains and PDFs of Mw and VR for all samples except the burnin. The VR increased with an increase in the model's freedom, which shows that the fourstage sampling successfully estimated models with high VR values without smoothing constraints. However, the amount of increase was small from stage 3 to stage 4. These results suggest that the spatial scale of the slip depended on that of the perturbation groups, because they were estimated without the smoothing constraint. The bottom chains in Fig. 5a show the calculated AIC values for each sample using Eq. (5). The mean values (± standard deviation) of AIC in each stage were 5502 ± 35, 5384 ± 47, 5455 ± 66, and 7572 ± 78, respectively. The AIC values of stage 2 and stage 3 were lower than those of stage 4, which objectively suggests the possibility of overdivision. Based on this, we mainly use the samples of stage 2 for further analysis in "Uncertainty of tsunami inundation" section. Comparing the input (Fig. 1), the median slip is located more landward at all stages (Fig. 4). The Mw and VR values calculated based on the median models (inset in Fig. 4; vertical red lines in Fig. 5b) were differed slightly from those calculated based on each sample (PDFs in Fig. 5b). These indicate that the model obtained for each sample does not completely agree with the slip distribution by representative values because of the diversity of the slip in the neartrench area.
Figure 6 shows eight examples of posterior PDFs from stage 2. The point A, B and F are the area off Cape Ashizuri, where the estimated slip was large and arranged in the fault dip direction. The 95% CI at point A (close to land) was small, while the value at point B (farther offshore) was large. At point F, located further offshore, the search extends to approximately 10 m, while the maximum frequency value remains at zero. These tendencies were also observed for points C and G. In the case of point E, which corresponds to a region, where the assumed slip gradually decays, the PDF includes the assumed slip (red line in Fig. 6). This diversity of offshore slip suggests a tradeoff of slip in the fault dip direction. The diversity is more pronounced owing to the lack of realtime seafloor observation sites. Ideally, modeling should be done according to spatial resolution (we discuss in "Optimization of perturbation groups for each stage and background subfaults" section). As shown above, because the tradeoff between model parameters and the posterior PDF was not necessarily normally distributed, this study used the median as the representative value (cf. mean and mode). These results, focused on one stage, show that the MCMC can estimate significant slip distributions without smoothing constraints, and that the variability of the uncertainty based on data can be quantified as posterior PDFs.
Uncertainty of tsunami inundation
We applied the "realtime tsunami inundation risk map ("Realtime tsunami inundation risk map" section)" to the MCMC samples of stage 2, where had the lowest AIC (see "Uncertainty of slip distribution" section). First, among the \(3\times {10}^{6}\) MCMC samples of stage 2, we extracted 319,184 samples with VR of 99.52%, which is the representative value of the PDF (Fig. 3i). We then classified the extracted samples into 100 clusters using the kmeans method. In each cluster, we generated one scenario using the median values for each subfault belonging to the cluster (Fig. 3ii). Using these scenarios as inputs, we calculated 100 tsunami inundation calculations for the area of Kochi Prefecture (Fig. 3iii). Finally, we counted the number of inundated points on each grid on the map (Fig. 3iv). The threshold of the inundated point was 1 cm or more during the 6 h since the earthquake. We did not apply any weights to obtain the frequencies.
Figure 7a shows the generated realtime tsunami inundation risk map. The envelope of the maximum inundation area and the arrival probability (risk level) are shown. The area where the risk of tsunami inundation is extremely high in all 100 cases (pink coloring) is similar to the inundation area due to the assumed slip (Fig. 8c). The areas with the highest probability of tsunami inundation are the Uranouchi Bay, Monobe River, and Yasu River. In addition, the southern half of Kochi Airport also has a high risk of inundation. These results show that tsunami inundation is strongly related to land topography and rivers. Tsunamis would likely run northward along large rivers (e.g., Niyodo River, Monobe River), and extend their inundation area around rivers and waterways (e.g., Shimoda River). The limit of tsunami runup on land was defined in some cases by the fact that the kinetic energy was zero, and in other cases, because it could not overcome the difference in elevation of the terrain (rivers, channels, and embankments). For comparison, Fig. 7b shows an elevation map of the same area. High inundation risk is generally distributed in areas with elevations of 10 m or less. On the other hand, tsunami inundation does not spread to Urado Bay, despite the low elevation, owing to the structural conditions in the tsunami calculation. The elevation of area A in Fig. 7b varies gently (from 0 to 8 m), and Fig. 7a shows a clear gradation of 0–100%. Area B has an embankment of more than 1 m and this becomes the inundation boundary. Area C has an elevation of more than 10 m parallel to the coast; in about 50% of the scenarios inundation proceeded from the east side, and in a few scenarios, inundation overcame from the south to the north. Therefore, the results of inundation calculations vary depending on small differences in topographical data and arrival tsunami scenarios.
Figure 7a shows that there were few areas, where the probability of inundation was 50–90%. This indicates that the tendency of inundation is different between always inundated and rarely inundated areas. Figure 8 shows the cases with large inundation areas. The inundation area of the largest two cases was more than 40 \({\mathrm{km}}^{2}\), which is clearly larger than the assumed slip (16.784 \({\mathrm{km}}^{2}\)). In both cases, the initial wave fields had large uplift and subsidence in the offshore area of Kochi Prefecture. If these two cases were removed from the count, the appearance of the map changed (Additional file 1: Figure S2). In addition, samples with large vertical seafloor deformation for the entire slip area did not necessarily have large tsunami inundation areas (Additional file 1: Figure S3), because tsunami inundation was evaluated on a local scale.
It is also important to consider the method of editing the realtime tsunami inundation risk maps. Additional file 1: Figure S4 shows editing examples, where (a) the map is weighted by the label frequency distribution (Fig. 9b), and where (b) the threshold value of the inundation depth considered to be inundation was changed from 1 cm to 1 m. In Additional file 1: Figure S4(a), there was almost no change in the frequency tendency of the inundation area, because there was no strong correlation between the frequency and the inundation area. However, as shown in Additional file 1: Figure S4(b), there was a decrease in the inundation probabilities, because inundation of less than 1 m was not counted.
These realtime tsunami inundation risk maps provide quantitative probabilistic information. As the concept of the target area is not included in the scenario classification method (Fig. 3i, ii), the same map can be generated for any region using the same MCMC samples.
Discussion
Setting optimization in stepwise partition algorithm
Optimization of \({{\varvec{\sigma}}}_{{\varvec{i}}{\varvec{j}}}\) in the likelihood function
In this study, we assumed \({\sigma }_{ij}\) (see Eq. (3)). In contrast, Ohno et al. (2021) automatically adjusted \({\sigma }_{ij}\) according to the event using the maximum likelihood estimation scheme. Here, this adjustment was not applied to the slip distribution model, because the large number of parameters easily explained the observed data, resulting in a very small estimate of \({\sigma }_{ij}\). This dynamic adjustment is more effective for a single rectangular fault model; however, modeling errors exist in the slip distribution model owing to the uncertainty of Green's function. Therefore, in this study, we assumed \({\sigma }_{ij}\), which depends on the displacements and observation errors.
Optimization of a priori information
Ohno et al. (2021) used earthquake early warning values (EEW: latitude, longitude, depth, M) as a priori information. While our algorithm does not use such a priori information, it is important to appropriately utilize such information to achieve accurate and rapid estimation for realtime estimation. For example, the algorithm can use the EEW and independent estimated models, such as the single rectangular fault model and the slip distribution by REGARD, as a priori information.
Optimization of perturbation groups for each stage and background subfaults
As discussed in "Uncertainty of slip distribution" section, there was a tradeoff of slip in the dip direction. We applied a stepwise partitioning algorithm to various assumed slip distributions and found a similar tendency (Additional file 1: Figures S5–S10). The position and wavelength of the slip in the dip direction affected the tsunami calculation. Optimization of the perturbation group settings is especially important, because the empirical geophysical law (slip continuity) is not considered when a smoothing constraint is not used. For example, it is desirable to evaluate the spatial resolution depending on the location of the observation stations and to determine the division of the perturbation group accordingly. Kimura et al. (2019) developed an algorithm for automatically setting up the division of subfaults according to the arrangement of observation stations. It may be effective to use this algorithm for setting subfaults (smallest division) and arranging the perturbation group in each stage. The required size varies depending on the magnitude of the earthquake, and so we should determine the optimum stage objectively (i.e., using the AIC) and judge the convergence (e.g., using Gelman 1996) automatically for realtime utilization.
Optimum number of clusters
The optimum number of clusters K for kmeans ("Uncertainty of tsunami inundation" section) should be determined considering the cost of realtime computation, the availability of denominators for probability display, and the availability of a sufficient number of clusters that do not distort the diversity of all samples. Here, we consider the validity of K = 100 in comparison with K = 300.
Figure 9 shows the results of clustering using kmeans. According to the elbow method graph (Fig. 9a), a cluster number of K = 50–100 seems to be appropriate. On the other hand, according to the frequency distribution of the clusters (Fig. 9b), even if we increased the number of clusters from K = 100 to K = 300, it looks like the classification just was subdivided overall. Figure 9c shows the correlation between the number of models included in each cluster and the variability of the slip distribution, which is a scalar sum of the ranges of slip amounts on each subfault. According to Fig. 9c, both the number of models included (horizontal axis) and variability (vertical axis) are smaller for K = 300 than for K = 100. This may indicate that by increasing the number of clusters, clusters were formed among the slip distribution models that have the closest features to each other. Figure 9d shows the variability of the VRs for the K scenarios (the median model in each cluster). Although the used samples have the same VR (99.52%), those of the classified scenarios vary in the order of the second decimal place. Note that there are some scenarios, where VR is greater than the original VR (99.52%). This is probably because the outlierlike shortwavelength slip of each sample was smoothed by taking the median at each subfault, resulting in a model that better explains the data.
Figure 10 shows the correlation between the number of models included in each cluster and the inundation areas for K = 100 and K = 300. The frequency distribution of the tsunami inundation area (vertical axis) is asymmetric, with a peak near the tsunami inundation area due to the assumed slip (16.784 \({\mathrm{km}}^{2}\)) and long tail on the side of the large tsunami inundation. The maximum and minimum inundation areas for K = 100 and K = 300 are similar. On the other hand, 300 cases of K = 300 are distributed so that they filled in the gaps between the 100 cases of K = 100. The maximum inundation area for K = 300 is slightly larger than that for K = 100 (and the maps look slightly different; Additional file 1: Figure S11). These characteristics suggest that the larger the number of K, the more the tsunami scenario is subdivided, and the degree of smoothing of extreme slip decreases. However, for the present trial, K = 100 was sufficient to obtain the range of the inundation area.
In the case of K = 100, there was a negative correlation between the inundation area and the number of models included in each cluster (Fig. 10). However, as shown in Fig. 9b where colored the clusters with an inundation area of 40 \({\mathrm{km}}^{2}\) or more, there was not necessarily a relationship between the frequency of each cluster and the flooded area in Kochi City. This may be because the number of models included in each cluster shows a tendency for the “entire” slip distribution, whereas inundation was evaluated by focusing on a target area, which seems to be a natural result. On the other hand, samples with extreme slip patterns tend to be classified into clusters with small frequencies, and the possibility that these samples cause maximum inundation in some other areas cannot be excluded.
Utilization of realtime tsunami inundation risk maps
The risk of tsunami inundation is expressed by multiplying hazard (e.g., tsunami inundation) by exposure (e.g., population and buildings) and fragility (e.g., buildings), then dividing it by resiliency (e.g., Wood 2011). The realtime tsunami inundation risk maps evaluate the probability of tsunami inundation for each area, which corresponds to the probabilistic representation of hazards in the above equation.
For example, if we reflect the difference in day/night population (i.e., exposure), we can evaluate the difference in disaster risk depending on the time of day, and if we reflect the difference in resiliency, we can quantify the disaster risk according to the time scale we want to evaluate. In addition, to maximize the benefit of evaluating disaster triggers as probabilities in this study, it is easier to evaluate the risk level if other factors can be treated as probabilities in the same dimension. For easytounderstand expression, qualitative evaluation may also be useful (e.g., three risk levels of large, medium, and small). Furthermore, if we take the envelope of the maximum inundation area, we can extract the worstcase scenario for the event (Fig. 7a).
As mentioned in "Introduction" section, the realtime tsunami inundation damage estimation system is expected to be utilized as a function of the disaster information system (DIS) of the Cabinet Office for the initial response of the government when a disaster occurs. Our developed framework for the quantitative evaluation of uncertainty in tsunami inundation prediction has the potential to improve this system. The risk level can be expressed as a probability instead of a single inundation prediction. This system has the potential to improve understanding of high disasterrisk regions and to support the decisionmaking process for the initial response in such areas.
Conclusions
In this study, we developed a new coseismic fault model estimation algorithm using Bayesian statistics to quantitatively evaluate the estimation uncertainty in the realtime estimation of slip distribution using realtime GNSS data. In addition, as an application of the quantified uncertainty, we investigated how the uncertainty of the fault model estimation may affect tsunami inundation prediction and proposed a new method to extract the uncertainty of tsunami inundation prediction.
One of the major problems in the estimation of slip distribution models with MCMC is that they take a long time to converge. To overcome this problem for realtime purposes, we developed a stepwise partitioning algorithm. We divided the entire Markov chain into four stages with different perturbing groups, and used the 95% CI in the previous stage as the amount of perturbation in the next stage. This enabled us to extract multiple models with different spatial patterns that explained the observed data well. We applied the algorithm to the numerical simulation data of the Nankai Trough region (assumed to be the Mw 8.75 1707 Hoei earthquake). The 95% CI of the obtained posterior PDFs increased with distance from the coast to the offshore, indicating the uncertainty in estimating plate boundary slip from onshore GNSS.
We developed a realtime tsunami inundation risk map process to fully utilize the advantages of the stepwise partitioning algorithm, wherein the uncertainty of slip distribution is quantified as a large number of samples. Specifically, we classified the slip distribution models into 100 clusters determined by the kmeans method after extracting samples that have the same VR. We calculated the individual tsunami inundation using 100 scenarios. Furthermore, we counted the number of inundations in each grid on the map and displayed them probabilistically. We showed the envelope of the maximum inundation area and the probability of reaching each computational grid in Kochi City, Kochi Prefecture. However, to truly utilize the obtained tsunami inundation risk, it may be necessary to examine the kind of information needed not only from the viewpoint of disaster triggers but also from the viewpoint of society as a recipient.
Availability of data and materials
The analyzed data for the current study are available from the corresponding author upon reasonable request.
Abbreviations
 ABIC:

Akaike's Bayesian Information Criterion
 AIC:

Akaike's Information Criterion
 CI:

Confidence Intervals
 DIS:

Disaster Information System
 EEW:

Earthquake Early Warning
 GEONET:

GNSS Earth Observation NETwork system
 GNSS:

Global Navigation Satellite System
 GSI:

Geospatial Information Authority of Japan
 JMA:

Japan Meteorological Agency
 MCMC:

Markov chain Monte Carlo methods
 PDF:

Probability Density Function
 REGARD:

REaltime GEONET Analysis system for Rapid Deformation monitoring
 TUNAMI:

Tohoku University's Numerical Analysis Model for Investigating tsunami
 VR:

Variance Reduction
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Acknowledgements
The paper benefited from careful reviews by Dr. Sarah Minson and an anonymous reviewer. This study was supported by the Japan Society for the Promotion of Science GrantinAid for Scientific Research (KAKENHI; grant no. 17H06108) and by the Toray Science Foundation (Toray Science and Technology Grant). This work was also supported by the JST FOREST Program (grant number: JPMJFR202P, Japan). This study was also supported by the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan, under its The Second Earthquake and Volcano Hazards Observation and Research Program (Earthquake and Volcano Hazard Reduction Research). This work was also supported by the Next Generation HighPerformance Computing Infrastructures and Applications R&D Program by MEXT. This work was also supported by the Research Project for Disaster Prevention on the great Earthquakes along the Nankai trough by MEXT.
Funding
This study was supported by the Japan Society for the Promotion of Science GrantinAid for Scientific Research (KAKENHI; grant no. 17H06108) and by the Toray Science Foundation (Toray Science and Technology Grant). This work was also supported by the JST FOREST Program (grant number: JPMJFR202P, Japan). This study was also supported by the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan, under its The Second Earthquake and Volcano Hazards Observation and Research Program (Earthquake and Volcano Hazard Reduction Research). This work was also supported by the Next Generation HighPerformance Computing Infrastructures and Applications R&D Program by MEXT. This work was also supported by the Research Project for Disaster Prevention on the great Earthquakes along the Nankai trough by MEXT.
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KO and YO designed the study, developed the programs, and analyzed the data. SK and TA performed the tsunami inundation calculations. AM and HK contributed to speeding up the programs developed. YO, SK, RH, and HK assisted in the interpretation of the results. All authors read and approved the final manuscript.
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K.O. was a graduate student at the Graduate School of Science, Tohoku University (now at the Geospatial Information Authority of Japan). Y.O. and R.H. are associate professor and professor, respectively, at the Graduate School of Science, Tohoku University. S.K. and T.A. are professor and research fellow, respectively, at the International Research Institute for Disaster Science, Tohoku University. A.M. and H.K. are visiting professor and professor, respectively, at the Graduate School of Information Sciences, Tohoku University.
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Table S1 and Figures S1–S11.
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Ohno, K., Ohta, Y., Hino, R. et al. Rapid and quantitative uncertainty estimation of coseismic slip distribution for large interplate earthquakes using realtime GNSS data and its application to tsunami inundation prediction. Earth Planets Space 74, 24 (2022). https://doi.org/10.1186/s40623022015866
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DOI: https://doi.org/10.1186/s40623022015866