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Multiindex method using offshore oceanbottom pressure data for realtime tsunami forecast
Earth, Planets and Space volume 68, Article number: 128 (2016)
Abstract
We developed a realtime tsunami forecast method using only pressure data collected from the bottom of the ocean via a dense offshore observation network. The key feature of the method is rapid matching between offshore tsunami observations and precalculated offshore tsunami spatial distributions. We first calculate the tsunami waveforms at offshore stations and the maximum coastal tsunami heights from any possible tsunami source model and register them in the proposed Tsunami Scenario Bank (TSB). When a tsunami occurs, we use multiple indices to quickly select dozens of appropriate tsunami scenarios that can explain the offshore observations. At the same time, the maximum coastal tsunami heights coupled with the selected tsunami scenarios are forecast. We apply three indices, which are the correlation coefficient and two kinds of variance reductions normalized by the L2norm of either the observation or calculation, to match the observed spatial distributions with the precalculated spatial distributions in the TSB. We examine the ability of our method to select appropriate tsunami scenarios by conducting synthetic tests using a scenario based on “pseudoobservations.” For these tests, we construct a tentative TSB, which contains tsunami waveforms at locations in the Seafloor Observation Network for Earthquakes and Tsunamis along the Japan Trench and maximum coastal tsunami heights, using about 2000 tsunami source models along the Japan Trench. Based on the test results, we confirm that the method can select appropriate tsunami scenarios within a certain precision by using the two kinds of variance reductions, which are sensitive to the tsunami size, and the correlation coefficient, which is sensitive to the tsunami source location. In this paper, we present the results and discuss the characteristics and behavior of the multiindex method. The addition of tsunami inundation components to the TSB is expected to enable the application of this method to realtime tsunami inundation forecasts in the near future.
Introduction
A wide variety of methods for nearfield tsunami forecasts have been proposed. These methods depend on the purpose and type of observational data (e.g., Tsushima and Ohta 2014). Here we define a “realtime tsunami forecast” to derive the information required for evacuation before the first arrival of a tsunami at the coast. In Japan, a realtime tsunami forecast using the hypocenter location and the earthquake magnitude determined from landbased seismological observation has been operated by the Japan Meteorological Agency (JMA) since 1999 (Tatehata 1997; Kamigaichi 2009). This is used as an initial forecast because it can be issued very quickly. However, it contains considerable uncertainty, because landbased seismic observation alone cannot constrain the hypocenter location and the magnitude of subduction zone earthquakes. Accordingly, a more accurate realtime tsunami forecast method using fault geometry information and the average amount of slip determined by the Global Navigation Satellite System (GNSS) was proposed by Blewitt et al. (2009). Moreover, the centroid moment tensor for a more accurate tsunami forecast could be estimated by Wphase waveform inversions (Benavente and Cummins 2013; Gusman and Tanioka 2014). Because the fault model is obtained from GNSS data and/or Wphase records within a few minutes after an earthquake occurs, it is possible to replace the initial forecast information with more accurate information (Tsushima and Ohta 2014). In addition, a tsunami forecast method to estimate the best tsunami source model by inversion analysis of tsunami waveform data from oceanbottom pressure gauges was proposed by Tsushima et al. (2009). In their method, the arrival times and amplitudes of tsunamis at the coasts are forecast by linearly combining precalculated Green’s functions. However, obtaining direct measurements of tsunamis requires more time to detect tsunami signals than obtaining seismic wave or realtime GNSS data (Tsushima and Ohta 2014, Figure 4). Attempting a breakthrough, Baba et al. (2014) investigated the correlation between offshore and coastal tsunami heights by using oceanbottom pressure data from the Dense Oceanfloor Network system for Earthquakes and Tsunamis (DONET) observation array (Kaneda et al. 2009). They successfully forecast the coastal tsunami height within 10 min after the occurrence of an earthquake by concentrating on predicting the tsunami scale. In addition, Yamamoto et al. (2016) proposed a rapid method to estimate the tsunami source location using a dense offshore observation network. They claimed that this location could be estimated within a few minutes after the occurrence of an earthquake by using the tsunami centroid location (TCL). Although direct measurements of tsunamis are used in their method, the required estimation time is comparable to that achieved using realtime GNSS data. It is possible to replace the earthquake location and magnitude with the tsunami source location estimated by Yamamoto et al. (2016) and the tsunami scale estimated by Baba et al. (2014) for the initial tsunami warning. Moreover, Maeda et al. (2015) proposed a tsunami forecast method based on a data assimilation technique using a dense offshore observation network rather than using seismic source parameters or the initial height of the sea surface. In their method, the tsunami wavefield including offshore tsunami height and velocity will be available as initial conditions for other tsunami forecasting methods such as tFISH (Tsushima et al. 2009), NearTIF (Gusman et al. 2014) to calculate the inundation or runup for realtime forecasting. For a realtime tsunami inundation forecast, some researchers have proposed new methods that use ondemand forward simulations with inverted tsunami source models (Tatsumi and Tomita 2013; Koshimura et al. 2014; Oishi et al. 2015). However, these methods are computationally expensive; hence, the coastal region to be included in the forecast is limited. A realtime tsunami inundation forecast on highresolution topography was achieved by Gusman et al. (2014), who proposed a new method that requires precalculated tsunami waveforms and tsunami inundation at nearshore points in advance of the occurrence of an earthquake. Their method involves the selection of the bestmatched tsunami scenario by comparing precalculated tsunami waveforms and synthetic tsunami waveforms calculated using forecast tsunami source information, such as fault models estimated by the Realtime Automatic detection method for Permanent Displacement (RAPiD) proposed by Ohta et al. (2012), WPhase data (Kanamori 1993; Gusman and Tanioka 2014), or initial seasurface displacement distributions (Tsushima et al. 2009). The precalculated tsunami inundation for the bestmatched tsunami scenario is then forecast.
We propose a new approach for realtime tsunami inundation forecasts that uses only tsunami data obtained by offshore oceanbottom pressure gauges without using any seismological observation data. Consequently, it is possible to predict tsunamis by avoiding the influence of estimation errors in the hypocenter location or the earthquake magnitude determined by seismological observations. For tsunami earthquakes, which are defined as events in which the size of the tsunami is significantly larger than that expected from seismic waves (Kanamori 1972), it is possible to appropriately evaluate the size of the tsunami irrespective of the earthquake magnitude estimated by seismological observations. In addition, to provide highresolution tsunami inundation forecasts for a wide coastal zone, we use a precalculated database rather than ondemand forward simulation. If we could consider all possible tsunami scenarios, the tsunami forecast would be highly precise. However, the number of tsunami scenarios that can be prepared is limited because of a finite amount of time and limited computing resources. In other words, a tsunami scenario selected from precalculated tsunami scenarios cannot always make correct predictions for an entire coastal region. Therefore, we select dozens of tsunami scenarios that can explain offshore observation data within acceptable thresholds in order to express the uncertainties of a tsunami forecast. Another basic concept of our approach is that the realtime tsunami forecast is derived directly from observed tsunami data without any information about the tsunami source, which is generally obtained by inversion and can contain large uncertainties.
In this paper, we propose the use of multiple indices to select appropriate tsunami scenarios. The first stage of our method involves the preparation of a Tsunami Scenario Bank (TSB), which contains tsunami waveforms at offshore stations and coastal tsunami information calculated using a number of possible tsunami source models. When a tsunami occurs, we use three indices to quickly select dozens of appropriate tsunami scenarios that can explain the offshore observations. At the same time, the coastal tsunami information coupled with the selected tsunami scenarios is forecast. The three indices are a correlation coefficient and two kinds of variance reductions and are used to compare the observed waveforms and the precalculated waveforms in the TSB. We conducted an evaluation to determine whether our method can select appropriate tsunami scenarios by considering realtime oceanbottom hydrostatic pressure data that are expected to be obtained by the Seafloor Observation Network for Earthquakes and Tsunamis (Snet) (Uehira et al. 2012; Kanazawa 2013), which is a dense and largescale offshore observation network under construction along the Japan Trench by the National Research Institute for Earth Science and Disaster Resilience (NIED). We constructed a tentative TSB by calculating offshore tsunami waveforms at the Snet instrument locations, and the maximum coastal tsunami heights along the Pacific coast of Kanto, Tohoku, and Hokkaido using about 2000 tsunami source models, which were previously prepared for a probabilistic tsunami hazard assessment in the Japan Trench region (Hirata et al. 2014). Furthermore, we discuss the characteristics and behavior of the multiindex approach in the matching procedure.
Matching method
Here we describe a method for comparing the observed waveform \(O({\varvec{r}}_i, t)\) and the precalculated waveform \(C({\varvec{r}}_i, t)\) registered in the TSB, for the ith observation station at a position \({\varvec{r}}_i\) after time t has elapsed following an earthquake.
Three indices
As mentioned above, we use three indices, the correlation coefficient and two kinds of variance reductions, to compare \(O({\varvec{r}}_i, t)\) to \(C({\varvec{r}}_i, t)\). The correlation coefficient \(\hbox {R}(t)\), which is a function of time t, is defined as follows:
where n is the number of observation stations. Equation (1) indicates that \(\hbox {R}(t)\) is the cosine of the angle formed by two ndimensional vectors, \(O({\varvec{r}}_i, t)\) and \(C({\varvec{r}}_i, t)\), and \(\hbox {R}(t)\) has a maximum value of 1 when \(O({\varvec{r}}_i, t)\) is similar to \(C({\varvec{r}}_i, t)\). When \(O({\varvec{r}}_i, t)\) and \(C({\varvec{r}}_i, t)\) are completely opposite, \(\hbox {R}(t)\) becomes \(1\), i.e., \(\hbox {R}(t)\) ranges from \(1\) to 1. \(\hbox {R}(t)\) is expected to be sensitive to the tsunami source location, because \(\hbox {R}(t)\) strongly depends on the spatial distribution of \(O({\varvec{r}}_i, t)\) and \(C({\varvec{r}}_i, t)\). However, \(\hbox {R}(t)\) is close to 1 when their spatial distributions are similar, even though the amplitudes of \(O({\varvec{r}}_i, t)\) and \(C({\varvec{r}}_i, t)\) are very different.
Next, we define the variance reduction to discriminate between acceptable and unacceptable matching accuracy. In general, the variance reduction is defined as follows:
In this study, we define two variance reductions, \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\), as functions of time t normalized by the L2norm of either the observed waveform \(O({\varvec{r}}_i, t)\) or the calculated waveform \(C({\varvec{r}}_i, t)\), as follows:
where we use the sum of the squared residual as the difference in Eq. (2). As defined by Eqs. (3) and (4), both variance reductions become 1 when \(O({\varvec{r}}_i, t)\) equals \(C({\varvec{r}}_i, t)\), i.e., variance reductions of 1 indicate the best matches. These values become smaller as the difference between \(O({\varvec{r}}_i, t)\) and \(C({\varvec{r}}_i, t)\) increases. Therefore, \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) range from \(\infty\) to 1.
Next, we rewrite Eqs. (3) and (4) as
where \(\alpha (t)\) is defined as follows:
which is the square root of the ratio of the L2norm of \(C({\varvec{r}}_i, t)\) to the L2norm of \(O({\varvec{r}}_i, t)\) and is larger than 0 \((\alpha (t) > 0)\). Figure 1 shows \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) as functions of \(\alpha (t)\) for fixed values of \(\hbox {R}(t)\) in Eqs. (5) and (6). When \(\alpha (t)\) is significantly larger than 1, i.e., the sum of the squares of \(C({\varvec{r}}_i, t)\) is larger than the sum of the squares of \(O({\varvec{r}}_i, t)\), \(\hbox {VRO}(t)\) has a large negative value that is proportional to the square of \(\alpha (t)\), as given in Eq. (5). A large \(\alpha (t)\) indicates that \(C({\varvec{r}}_i, t)\) is overestimated with respect to \(O({\varvec{r}}_i, t)\). On the other hand, an \(\alpha (t)\) value that is significantly smaller than 1 indicates that \(C({\varvec{r}}_i, t)\) is underestimated with respect to \(O({\varvec{r}}_i, t)\). In this case, \(\hbox {VRC}(t)\) has a large negative value that is proportional to the inverse of the square of \(\alpha (t)\), as shown in Eq. (6). From the above considerations, we clearly find that \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) are sensitive to overestimation and underestimation of \(C({\varvec{r}}_i, t)\) with respect to \(O({\varvec{r}}_i, t)\).
Figure 2 shows the relations among the variance reductions, \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\), the correlation coefficient \(\hbox {R}(t)\), and the ratio \(\alpha (t)\). All possible pairs of \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) are plotted between the purple curves, which indicate \(\hbox {R}(t) = 1\), and the light blue curve, which indicates \(\hbox {R}(t) = 1\). The red and orange lines show pairs of \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) with \(\alpha (t)\) values of 0.5, 1.0, and 2.0.
Waveform conversion
We avoid the mismatch caused by wave phase differences by using the maximum value of the absolute values of the observed waveforms \(O_{\mathrm{converted}}({\varvec{r}}_i, t)\), defined as follows:
The converted values become constant after a sufficient time lapse following an earthquake. We also apply the same conversion to the calculated waveform \(C({\varvec{r}}_i, t)\) as follows:
When we compare the converted waveforms \(O_{\mathrm{converted}}({\varvec{r}}_i, t)\) and \(C_{\mathrm{converted}}({\varvec{r}}_i, t)\), the correlation coefficient \(\hbox {R}(t)\) never becomes negative, i.e., \({\mathrm{R}}(t)\) ranges from 0 to 1.
Construction of a tentative TSB
In this study, we set up 1890 tsunami source models, which can affect the Pacific coast of Kanto, Tohoku, and Hokkaido, in the region of the Japan Trench. The models, which were previously prepared for probabilistic tsunami hazard assessment (Hirata et al. 2014), are used to construct a tentative TSB. We then calculate synthetic offshore tsunami waveforms \(\eta ({\varvec{r}}_i, t)\) for 150 stations of Snet by solving nonlinear longwave equations using a staggered leapfrog finitedifference scheme. We use nesting grid systems with a minimum size of 50 m for the land side that corresponds to the target coastline shown as the blue line in Fig. 3, and larger mesh sizes of 150, 450, and 1350 m for the sea side. A runup boundary condition is applied to the coastal regions, and an open boundary condition is applied to the rims of the 1350m mesh systems. In these calculations, we assume that the seasurface displacement is the same as the vertical seafloor displacement of coseismic crustal deformation caused by an earthquake, and the seasurface displacement is immediately completed at time \(t=0\). The calculated tsunami waveforms \(\eta ({\varvec{r}}_i, t)\) are converted to oceanbottom hydrostatic pressure changes \(C({\varvec{r}}_i, t)\) as follows:
where \(\rho\) is the average density of seawater, g is the gravitational acceleration, and \(\eta _0({\varvec{r}}_i)\) is the initial seasurface displacement, which is the same as the permanent seafloor deformation calculated by Okada’s formula (Okada 1985). We also assume that the hydrostatic oceanbottom pressure, which is proportional to the total water depth, does not change during an earthquake, i.e., \(C({\varvec{r}}_i, t=0) = 0\), because the oceanbottom pressure gauges are displaced by seafloor deformation equal to the seasurface displacement. Finally, we register the calculated waveform \(C({\varvec{r}}_i, t)\) with its fault model and the maximum coastal tsunami heights along the Pacific coast of Kanto, Tohoku, and Hokkaido shown as the blue line in Fig. 3 in the tentative TSB.
Case studies and evaluations
We investigated whether it is possible to select appropriate tsunami scenarios from the tentative TSB by using the three indices defined in Eqs. (1), (3), and (4) with the maximum absolute values defined in Eqs. (8) and (9). Moreover, we also assumed that specified synthetic observed waveforms are “pseudoobservation” waveforms because the Snet has not yet recorded actual tsunami observation data. We then examine the selected tsunami scenarios by comparing the maximum coastal tsunami height distributions of the pseudoobservation scenarios and the selected tsunami scenarios. In this section, we describe the results of these examinations.
Examination using a tsunami scenario in the TSB (Model I)
As the first pseudoobservation scenario, named Model I, we choose a Mw 8.0 earthquake that occurred off the Boso Peninsula in the Kanto region, where the plate interface was not ruptured by the 2011 Tohoku earthquake. This fault model is shown as a purple polygon in Fig. 3. Our multiindex method selects 16 tsunami scenarios under the criteria of VRO (\(t=5\) min) \(\ge\) 0.0, VRC (\(t=5\) min) \(\ge\) 0.0, and R (\(t=5\) min) \(\ge\) 0.7 as illustrated in Fig. 3. Figure 4a compares the pseudoobservation waveform \(O({\varvec{r}}_i, t=5\,\hbox {min})\) and the bestmatched tsunami scenario, named scenario A, waveform \(C({\varvec{r}}_i, t=5\,\hbox {min})\), which is represented by the green polygon in Fig. 3 and the green square in Fig. 4c. Figure 4b compares the converted pseudoobservation waveforms with that of scenario A. Figure 4c, d plots the selected tsunami scenarios on the VRO–VRC diagram. The scenario shown at (VRO \((t=5\,\hbox {min})\), VRC (\(t=5\,\hbox {min})) = (1,1)\) in Fig. 4c represents Model I. From Fig. 4d, which shows a wider range of the VRO–VRC diagram, we can see that many unselected tsunami scenarios are plotted along the R (\(t=5\) min) = 0.0 curve, i.e., many tsunami scenarios registered in the tentative TSB do not satisfy the threshold \({\mathrm{R}}\;(t=5\,\mathrm{min}) \ge 0.7\). Figure 5 is a color contour map for R (\(t=5\) min) plotted at the centroid location of the slip distribution of fault models registered in the TSB. The figure suggests that the calculated scenarios with \(\hbox {R}(t)\) close to zero are far from the location of the fault model of the pseudoobservation scenario, i.e., \(\hbox {R}(t)\) is sensitive to the tsunami source location.
Figure 6 shows the evaluations for maximum coastal tsunami height distribution for Model I. Figure 6a indicates the maximum coastal tsunami height distributions of Model I (red line) and 16 selected tsunami scenarios (gray lines) along the coastline of Kanto, Tohoku, and Hokkaido represented by the blue line in Fig. 3. A variety of maximum coastal tsunami height distributions shown as gray lines in Fig. 6a, which indicate overestimation and underestimation by Model I, could express the uncertainties of a tsunami forecast. We evaluated the extent to which the selected tsunami scenarios were able to approximate the pseudoobservation scenario by using the three indices defined by Eqs. (1), (3), and (4) to compare the maximum coastal tsunami height distributions of the pseudoobservation scenario with those of the selected tsunami scenarios. In this study, we refer to the coastal indices as coastal R, coastal VRO, and coastal VRC, which are defined by the pseudoobservation distributions and the calculated distributions of maximum coastal tsunami heights that do not depend on time t. Figure 6b plots 16 selected tsunami scenarios on the coastal VRO–VRC diagram for comparing the maximum coastal tsunami height distributions for the corresponding tsunami scenarios. In this figure, the colored squares indicate the selected tsunami scenarios whose colors are the same as those of Fig. 4c, and the gray crosses indicate the unselected tsunami scenarios.
The use of \(t=5\) min is reasonable and appropriate for nearfield forecasting, e.g., in the Kanto region, because a realtime forecast is needed for evacuation purposes before the first arrival of a tsunami at the coast. However, it is still reasonable and appropriate to use \(t=10\) min for the Tohoku and Hokkaido regions. We next investigate the selected tsunami scenarios 10 min after the occurrence of an earthquake using the same criteria that were used in the previous examination: VRO (\(t=10\) min) \(\ge\) 0.0, VRC (\(t=10\) min) \(\ge\) 0.0, and R (\(t=10\) min) \(\ge\) 0.7. We confirm that 7 of the 16 tsunami scenarios selected at \(t=5\) min comply with the criteria at \(t=10\) min and the bestmatched tsunami scenario, which is represented by the green polygon and square in Figs. 3 and 4c, is selected as the bestmatched scenario at \(t=10\) min. We also confirm that the uncertainty in the set of selected tsunami scenarios is reduced because seven selected tsunami scenarios are matched in the coastal VRO \(\ge\) 0.89, VRC \(\ge\) 0.85, and R (\(t=10\) min) \(\ge\) 0.95 (see Fig. 4c). However, the other scenario, which is not selected at \(t=5\) min, satisfies the criteria at \(t=10\) min with (VRO (\(t=10\) min), VRC (\(t=10\) min), R (\(t=10\, \hbox {min})) = (0.78, 0.30, 0.97)\). The three indices indicate that this scenario is selected as an underestimated scenario (small VRC), but that the spatial distribution is very similar (large R). Therefore, suitable criteria should be considered for further work.
Correlation between offshore indices and coastal indices
Figures 7 and 8 represent the correlation between the offshore indices at time \(t = 5\) min and the coastal indices for Model I. In these figures, the colors of the squares indicating the selected tsunami scenarios are the same as those of Fig. 4c, and the gray crosses indicate the unselected tsunami scenarios. Figure 7a shows the correlation between the offshore VRO (\(t=5\) min) and the coastal VRO. As shown in this figure, most of the coastal VRO values for the selected tsunami scenarios are closer to 1 than the offshore VRO values for the corresponding tsunami scenarios (coastal VRO \(\gtrsim\) offshore VRO (\(t=5\) min)). As shown in Fig. 7b, the coastal VRC values for all tsunami scenarios are closer to 1 than the offshore VRC values [coastal VRC \(\gtrsim\) offshore VRC (\(t=5\) min)]. Figure 8, which presents a diagram showing the correlation between the offshore R (\(t=5\) min) and coastal R, indicates that all of the coastal R values for the selected tsunami scenarios are closer to 1 than the offshore R (\(t=5\) min) values [coastal R \(\gtrsim\) offshore R (\(t=5\) min)]. On the other hand, many of the coastal R values for the unselected tsunami scenarios (gray crosses) are smaller than the offshore R (\(t=5\) min) values for the corresponding tsunami scenarios. These tsunami scenarios are not selected, because their variance reductions do not satisfy the thresholds in spite of the good correlation coefficient. Table 1 lists the offshore indices and coastal indices for scenario A, which are represented by the green polygon in Fig. 3 and the green squares in Figs. 4, 6, 7, and 8. Model Ir, the results of which are included in the comparison in Table 1, is described in the next section. We also calculate the geometric mean K and geometric standard deviation \(\kappa\) defined by Aida (1978) to compare the maximum coastal tsunami height distributions of the pseudoobservation scenario (Model I) with that of scenario A. Therefore, it is possible to select appropriate tsunami scenarios that have maximum tsunami height distributions constrained within the criteria used for the offshore waveform comparison.
Influence of dynamic rupture process (Model Ir)
Instant rupture propagation is assumed in the previous examination. However, the propagation of a real earthquake tsunami would be delayed due to the dynamic rupture process of the coseismic fault slip (e.g., Hartzell and Heaton 1983; Mulia and Asano 2016). We examine the influence of the dynamic rupture process by modifying Model I to obtain Model Ir by using the convolution between offshore waveforms and a linear ramp function with a rise time of 3 min. For Model Ir, we examine how the multiindex approach works under the same thresholds: VRO (\(t=5\) min) \(\ge\) 0.0, VRC (\(t=5\) min) \(\ge\) 0.0, and R (\(t=5\) min) \(\ge\) 0.7. As a result, some tsunami scenarios selected in Model I are selected again. Figure 9a shows the offshore VRO–VRC diagram derived from comparisons of the offshore waveforms at \(t=5\) min. The colored squares indicate the selected tsunami scenarios with colors that are the same as those in the previous results for Model I, e.g., Fig. 4c. The offshore indices for 10 selected tsunami scenarios in this examination are worse than those for Model I in Fig. 4c. The original tsunami scenario (Model I) is selected with VRO (\(t=5\) min) = 0.80, VRC (\(t=5\) min) = 0.89, and R (\(t=5\) min) = 0.97. Furthermore, scenario A is selected as a wellmatched tsunami scenario again with VRO (\(t=5\) min) = 0.52, VRC (\(t=5\) min) = 0.78, and R (\(t=5\) min) = 0.92 (Table 1). Figure 9b shows the selected tsunami scenario for Model Ir on the coastal VRO–VRC diagram; however, the coastal VRO and coastal VRC values are the same as those for Model I because the maximum coastal tsunami height may not change essentially. As shown in this figure, most of the selected tsunami scenarios are restricted within the region bound by coastal VRO \(\ge\) 0.58 and coastal VRC \(\ge\) 0.67. In this examination, therefore, our proposed method is not significantly affected with the rise time of 3 min at \(t=5\) min. Moreover, we examine modified Model I with rise times in the range of 1–5 min. The second column of Table 2 shows the results of three indices comparing Model I and modified Model I for a rise time ranging from 0 min (no rise time) to 5 min in steps of 1 min. The result for Model Ir is shown at a rise time of 3 min (fourth line in Table 2). For a rise time of 5 min, however, the original tsunami scenario (Model I) is not selected within the given thresholds due to (VRO (\(t=5\) min), VRC (\(t=5\) min), R (\(t=5\) min)) = (\(0.06,0.72,0.96\)).
Application of the dynamic rupture process of the coseismic fault slip to the pseudoobservation scenario would delay the tsunami propagation. Therefore, the timeshifted tsunami scenario is expected to match the modified Model I more accurately than the tsunami scenarios without time shift. We evaluate this assumption by defining three timeshifted indices by modifying Eqs. (1), (3), and (4) as follows:
where \(C({\varvec{r}}_i,t\tau )\) is the timeshifted calculated tsunami waveform, and \(\tau\) is the amount by which the time shifted. In this examination, we investigate \(\tau = 1, 0, 1, 2, 3\), and 4 min (\(\tau\) should be shorter than \(t=5\) min). Then we calculate VRO\((t,t\tau )\), VRC\((t,t\tau )\), and R\((t,t\tau )\) using timeshifted calculated tsunami scenario \(C({\varvec{r}}_i,t\tau )\) for each modified Model I, which has a rise time of 0, 1, 2, 3, 4, and 5 min. Based on these examinations, the results of the three indices obtained by comparing Model I and modified Model I are presented in Table 2. As seen in Table 2, a time shift of \(\tau =2\) min is the bestmatched case for a rise time of 3 min. For a rise time of 5 min, a time shift of \(\tau =3\) min could be selected within the given threshold because (VRO (\(t=5\) min), VRC (\(t=5\) min), R (\(t=5\) min)) = (0.93, 0.92,0.96). The results in Table 2 suggest that \(\tau\) of the bestmatched case is approximately half of the amount of rise time applied to the pseudoobservation waveform.
Moreover, this approach supports the constraint of the time at which the tsunami originates. In previous examinations, we assumed that the time of origin of the tsunami is known for the purpose of comparing \(O({\varvec{r}}_i,t)\) and \(C({\varvec{r}}_i,t)\). However, the time of origin is unknown during a realtime tsunami forecast. As shown in the first line of Table 2, comparisons based on the time shift \(\tau\) are consistent with searches for the time of origin. The bestmatched case (\(\tau =0\) min) provides a wellmatched scenario for the time at which the tsunami originated. This examination enables us to confirm that the time at which the tsunami originated could be estimated by the timeshifted comparisons using multiple indices.
Examination of 2011 Tohoku earthquake tsunami (Model II)
In the pseudoobservation scenario chosen from the tentative TSB, the pseudoobservation waveform may be well matched with some tsunami scenarios stored in the tentative TSB, because similar fault models are found in the tentative TSB (Table 1). When the variance reduction is larger than 0.7, these scenarios are generally recognized to be matched (e.g., Tanioka et al. 1995; Baba and Cummins 2005). On the other hand, the slip distribution for a real earthquake source is usually more complex than the characterized fault models registered in the tentative TSB. Therefore, to test our method for a more realistic tsunami source model, we calculate tsunami waveforms by using the slip distribution of the 2011 Tohoku earthquake, suggested by the Cabinet Office (2012) as a pseudoobservation scenario (Model II). Although this source model was estimated by considering the effect of the rupture process on the fault plane, we assume that the coseismic crustal deformation is immediately completed at time \(t=0\) in order to focus on the influence of the complexity of the fault model. We use the same thresholds: VRO (\(t=5\) min) \(\ge\) 0.0, VRC (\(t=5\) min) \(\ge\) 0.0, and R (\(t=5\) min) \(\ge\) 0.7, as in the previous examinations.
Figure 10a compares the pseudoobservation waveform \(O({\varvec{r}}_i, t=5\) min) with the waveform \(C({\varvec{r}}_i,t=5\) min) of the bestmatched tsunami scenario, which is represented by the purple square shown at (VRO (\(t=5\) min), VRC \((t=5\,\hbox {min})\), R (\(t=5\) min)) = (0.66, 0.67, 0.83) in Fig. 10c. Figure 10b compares the converted pseudoobservation waveforms with the waveform of the bestmatched tsunami scenario. Figure 10c, d represents offshore VRO–VRC diagrams for 50 selected tsunami scenarios and others 5 min after the earthquake. The number of selected tsunami scenarios is larger than that in the previous examination, because the tentative TSB is constructed with a bias toward tsunami scenarios for large earthquakes, such as the tsunami caused by the 2011 Tohoku earthquake. As shown in Fig. 10d, the values of VRC (\(t=5\) min) for many unselected tsunami scenarios are strongly negative. This indicates that the 2011 Tohoku earthquake tsunami is close to the maximum class of tsunami scenarios registered in the tentative TSB, i.e., many tsunami scenarios registered in the tentative TSB are rejected due to underestimations. Figure 11 is a color contour map for R (\(t=5\) min) plotted at the centroid location of the slip distribution of fault models registered in the TSB. The figure shows that the distribution of R (\(t=5\) min) values is approximately consistent with the fault slip distributions proposed by Cabinet Office (2012) and obtained by the other inversion results (e.g., Fujii et al. 2011; Satake et al. 2013; Hossen et al. 2015).
Figure 12 shows the evaluations for the maximum coastal tsunami height distribution of Model II. Figure 12a indicates the maximum coastal tsunami height distribution of Model II and 50 selected tsunami scenarios. Figure 12b plots the selected tsunami scenarios on the coastal VRO–VRC diagram. In this figure, the colored squares, of which the colors indicate the same scenarios as those in Fig. 10c, indicate the selected tsunami scenarios. We confirm that our method can select tsunami scenarios appropriately for the pseudoobservation scenario calculated from the complex fault model, because the selected tsunami scenarios satisfy coastal \({\mathrm{VRO}} \ge 0.69\), coastal \({\mathrm{VRC}} \ge 0.57\), and coastal \({\mathrm{R}} \ge 0.87\) (Fig. 12b). However, there are no tsunami scenarios, whose offshore variance reductions, VRO and VRC, are larger than 0.7 (Fig. 10c). By comparing Figs. 10c and 12b, we conclude that the coastal VRO and VRC values for all the selected tsunami scenarios are reduced by a larger amount than the offshore VRO (\(t=5\) min) and VRC (\(t=5\) min) values.
Effectiveness of using multiple indices
We investigate the effectiveness of using three indices simultaneously by using only one index for Model II when selecting tsunami scenarios. In general, the variance reduction normalized by observation has been used for comparing observed and calculated data (e.g., Chi et al. 2001; Kubo et al. 2002; Ktenidou et al. 2011). Therefore, we examine the case of using only \(\hbox {VRO}(t)\) defined by Eq. (3) with a threshold of \({\mathrm{VRO}}\;(t=5\,\mathrm{min}) \ge 0.0\). For this examination, we selected the smallest tsunami scenarios (Mw 7.0) with a large negative value of VRC (\(t=5\) min) from the tentative TSB. If only \(\hbox {VRO}(t)\) is used as an index, underestimated tsunami scenarios could be selected and forecast. Even if we were to use the stricter threshold \({\mathrm{VRO}}\;(t=5\,\mathrm{min}) \ge 0.5\), the underestimated tsunami scenario (Mw 8.6) would still be selected; its VRO (\(t=5\) min) is 0.515, but its VRC (\(t=5\) min) is \(0.972\).
We avoid such an underestimation by presuming that it is effective to use both \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) simultaneously instead of using only \(\hbox {VRO}(t)\). A more effective approach to eliminating underestimated tsunami scenarios would be to set a stricter threshold for \(\hbox {VRC}(t)\), for example, \({\mathrm{VRO}}(t) \ge 0.0\) and \({\mathrm{VRC}}(t) \ge 0.5\). As we described above, the correlation coefficient \(\hbox {R}(t)\) facilitates the constraint of the tsunami source location. Therefore, we conclude that the combination of three indices rather than a single index allows us to achieve a more accurate tsunami forecast. However, by setting the threshold for \(\hbox {R}(t)\), we notice that the threshold \({\mathrm{R}}(t) \ge 0.7\) is not effective with \({\mathrm{VRO}}(t) \ge 0.5\) and \({\mathrm{VRC}}(t) \ge 0.5\), because \(\hbox {R}(t)\) always satisfies \({\mathrm{R}}(t) \ge 0.75\). When \({\mathrm{VRO}}(t) \ge 0.0\) and \({\mathrm{VRC}}(t) \ge 0.0\) are used as thresholds, \(\hbox {R}(t)\) always satisfies \({\mathrm{R}}(t) \ge 0.5\). Therefore, we suggest that the thresholds for the two variance reductions, \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\), are defined first to constrain the tsunami size. Then, the threshold for the correlation coefficient \(\hbox {R}(t)\) is defined to constrain the tsunami source location.
Conclusions
In this paper we propose a new method for achieving realtime tsunami forecasts. The method uses multiple indices to select appropriate tsunami scenarios by comparing waveforms that were observed offshore with those that are precalculated and registered in the TSB. We applied our method to a Mw 8.0 earthquake that occurred off the Boso Peninsula that was registered in the tentative TSB and the 2011 Tohoku earthquake as pseudoobservation scenarios. These examinations enabled us to confirm that appropriate tsunami scenarios could be selected by using the three indices, which consist of two kinds of variance reductions and a correlation coefficient, with offshore waveforms obtained by both pseudoobservation and by calculation, both of which are derived from oceanbottom pressure changes. Mathematical considerations and synthetic examinations revealed that two different kinds of variance reductions, \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\), which are normalized by the L2norm of either the observed or calculated waveforms, are sensitive to overestimation or underestimation of the tsunami size. We also found the correlation coefficient \(\hbox {R}(t)\) to be sensitive to the spatial distribution of the offshore tsunami, i.e., it is sensitive to the tsunami source location. Therefore, we concluded that the use of a combination of three indices rather than a single index is promising for providing more accurate tsunami forecasts. Furthermore, we investigated the correlations between offshore indices, derived from comparisons of offshore tsunami waveforms, and coastal indices, calculated from comparisons of maximum coastal tsunami height distributions. We found that it is possible to select appropriate tsunami scenarios that have maximum coastal tsunami height distributions constrained within the criteria used for the offshore waveform comparison. In addition, we suggested defining the thresholds for \(\hbox {VRO}(t)\) and \(\hbox {VRC}(t)\) first to constrain the tsunami size, followed by the determination of the threshold for \(\hbox {R}(t)\) to constrain the location of the tsunami source. We showed that, by comparing offshore waveforms, our method can select appropriate tsunami scenarios whose maximum coastal tsunami height distributions are close to those of the pseudoobservation scenario. By adding tsunami inundation components, such as the inundation area and runup heights to the TSB, our method can be expanded for realtime tsunami inundation forecasts.
Abbreviations
 TSB:

Tsunami Scenario Bank
 Snet:

the Seafloor Observation Network for Earthquakes and Tsunamis along the Japan Trench
 GNSS:

Global Navigation Satellite System
 VRO:

variance reduction normalized by observation
 VRC:

variance reduction normalized by calculation
References
Aida I (1978) Reliability of a tsunami source model derived from fault parameters. J Phys Earth 26(1):57–73
Baba T, Cummins PR (2005) Contiguous rupture areas of two Nankai Trough earthquakes revealed by highresolution tsunami waveform inversion. Geophys Res Lett 32(8):L08305
Baba T, Takahashi N, Kaneda Y (2014) Nearfield tsunami amplification factors in the Kii Peninsula, Japan for Dense Oceanfloor Network for Earthquakes and Tsunamis (DONET). Mar Geophys Res 35(3):319–325
Benavente R, Cummins PR (2013) Simple and reliable finite fault solutions for large earthquakes using the wphase: the Maule (mw = 8.8) and Tohoku (mw = 9.0) earthquakes. Geophys Res Lett 40(14):3591–3595
Blewitt G, Hammond WC, Kreemer C, Plag HP, Stein S, Okal E (2009) Gps for realtime earthquake source determination and tsunami warning systems. J Geod 83(3–4):335–343
Cabinet Office, Government of Japan (2012) Tsunami source model of 2011 Tohoku earthquake tsunami (in Japanese). http://www.bousai.go.jp/jishin/nankai/model/12/pdf/sub_1.pdf. Accessed 28 Dec 2015
Chi WC, Dreger D, Kaverina A (2001) Finitesource modeling of the 1999 Taiwan (ChiChi) earthquake derived from a dense strongmotion network. Bull Seismol Soc Am 91(5):1144–1157
Fujii Y, Satake K, Sakai S, Shinohara M, Kanazawa T (2011) Tsunami source of the 2011 off the Pacific coast of Tohoku earthquake. Earth Planets Space 63(7):815–820
Gusman AR, Tanioka Y (2014) W phase inversion and tsunami inundation modeling for tsunami early warning: case study for the 2011 Tohoku event. Pure Appl Geophys 171(7):1409–1422
Gusman AR, Tanioka Y, MacInnes BT, Tsushima H (2014) A methodology for nearfield tsunami inundation forecasting: application to the 2011 Tohoku tsunami. J Geophys Res Solid Earth 119(11):8186–8206
Hartzell SH, Heaton TH (1983) Inversion of strong ground motion and teleseismic waveform data for the fault rupture history of the 1979 Imperial Valley, California, earthquake. Bull Seismol Soc Am 73(6A):1553–1583
Hirata K, Fujiwara H, Nakamura H, Osada M, Ohsumi T, Morikawa N, Kawai S, Aoi S, Yamamoto N, Matsuyama H, Toyama N, Kito T, Murashima Y, Murata Y, Inoue T, Saito R, Akiyama S, Korenaga M, Abe Y, Hashimoto N (2014) Nationwide tsunami hazard assessment project in Japan. In: Abstract NH12A03 presented at 2014 Fall Meeting, AGU, San Francisco, CA, 15–10 Dec
Hossen MJ, Cummins PR, Dettmer J, Baba T (2015) Tsunami waveform inversion for sea surface displacement following the 2011 Tohoku earthquake: importance of dispersion and source kinematics. J Geophys Res Solid Earth 120(9):6452–6473
Kamigaichi O (2009) Tsunami forecasting and warning. In: Meyers RA (ed) Encyclopedia of complexity and systems science. Springer, Berlin, pp 9592–9618
Kanamori H (1972) Mechanism of tsunami earthquakes. Phys Earth Planet Inter 6(5):346–359
Kanamori H (1993) W phase. Geophys Res Lett 20(16):1691–1694
Kanazawa T (2013) Japan Trench earthquake and tsunami monitoring network of cablelinked 150 ocean bottom observatories and its impact to earth disaster science. In: 2013 IEEE international underwater technology symposium (UT). IEEE, pp 1–5
Kaneda Y, Kawaguchi K, Araki E, Sakuma A, Matsumoto H, Nakamura T, Kamiya S, Ariyoshi K, Baba T, Ohori M, Hori T (2009) Dense Ocean floor Network for Earthquakes and Tsunamis (DONET)—development and data application for the mega thrust earthquakes around the Nankai Trough. In: AGU Fall Meeting abstracts, vol 1, p 1453
Koshimura S, Hino R, Ohta Y, Kobayashi H, Musa A, Murashima Y (2014) Realtime tsunami inundation forecasting and damage mapping towards enhancing tsunami disaster resiliency. In: Abstract MH23B05 presented at 2014 Fall Meeting, AGU, San Francisco, CA, 15–10 Dec
Ktenidou OJ, ChávezGarcía FJ, Pitilakis KD (2011) Variance reduction and signaltonoise ratio: reducing uncertainty in spectral ratios. Bull Seismol Soc Am 101(2):619–634
Kubo A, Fukuyama E, Kawai H, Nonomura K (2002) NIED seismic moment tensor catalogue for regional earthquakes around Japan: quality test and application. Tectonophysics 356(1):23–48
Maeda T, Obara K, Shinohara M, Kanazawa T, Uehira K (2015) Successive estimation of a tsunami wavefield without earthquake source data: a data assimilation approach toward realtime tsunami forecasting. Geophys Res Lett 42(19):7923–7932
Mulia IE, Asano T (2016) Initial tsunami source estimation by inversion with an intelligent selection of model parameters and time delays. J Geophys Res Oceans 121(1):441–456
Ohta Y, Kobayashi T, Tsushima H, Miura S, Hino R, Takasu T, Fujimoto H, Iinuma T, Tachibana K, Demachi T et al (2012) Quasi realtime fault model estimation for nearfield tsunami forecasting based on RTKGPS analysis: application to the 2011 TohokuOki earthquake (mw 9.0). J Geophys Res Solid Earth 117(B2):B02311
Oishi Y, Imamura F, Sugawara D (2015) Nearfield tsunami inundation forecast using the parallel TUNAMIN2 model: application to the 2011 TohokuOki earthquake combined with source inversions. Geophys Res Lett 42(4):1083–1091
Okada Y (1985) Surface deformation due to shear and tensile faults in a halfspace. Bull Seismoll Soc Am 75(4):1135–1154
Satake K, Fujii Y, Harada T, Namegaya Y (2013) Time and space distribution of coseismic slip of the 2011 Tohoku earthquake as inferred from tsunami waveform data. Bull Seismol Soc Am 103(2B):1473–1492
Tanioka Y, Satake K, Ruff L (1995) Total analysis of the 1993 Hokkaido NanseiOki earthquake using seismic wave, tsunami, and geodetic data. Geophys Res Lett 22(1):9–12
Tatehata H (1997) The new tsunami warning system of the Japan meterological agency. Tsunami Hazards 16(1):39–49
Tatsumi D, Tomita T (2013) Development and implementation of realtime tsunami inundation prediction method. J Jpn Soc Civ Eng Ser B2 Coast Eng 69(1):34–47 (in Japanese with English abstract)
Tsushima H, Ohta Y (2014) Review on nearfield tsunami forecasting from offshore tsunami data and onshore GNSS data for tsunami early warning. J Disaster Res 9(3):339–357
Tsushima H, Hino R, Fujimoto H, Tanioka Y, Imamura F (2009) Nearfield tsunami forecasting from cabled ocean bottom pressure data. J Geophys Res Solid Earth 114(B6):B03311
Uehira K, Kanazawa T, Noguchi S, Aoi S, Kunugi T, Matsumoto T, Okada Y, Sekiguchi S, Shiomi K, Shinohara M, Yamada T (2012) Ocean bottom seismic and tsunami network along the Japan Trench. In: Abstract OS41C1736 presented at 2012 Fall Meeting, AGU, San Francisco, CA, 3–7 Dec
Yamamoto N, Hirata K, Aoi S, Suzuki W, Nakamura H, Kunugi T (2016) Rapid estimation of tsunami source centroid location using a dense offshore observation network. Geophys Res Lett 43(9):4263–4269
Authors’ contributions
NY proposed the ideas for this study, analyzed the data, and drafted the manuscript. SA initiated and managed the project, which is supported by SIP and related to this study. SA and KH prepared the data used in this study. All authors participated extensively in the design of this method and revisions of the manuscript. All authors read and approved the final manuscript.
Acknowledgements
We thank Editor Takuto Maeda and two anonymous reviewers for their thorough reviews and valuable suggestions on improving the quality of this article. This work was supported in part by the Council for Science, Technology, and Innovation (CSTI) through the Crossministerial Strategic Innovation Promotion Program (SIP), entitled “Enhancement of societal resiliency against natural disasters” (Funding agency: JST).
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The authors declare that they have no competing interests.
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Yamamoto, N., Aoi, S., Hirata, K. et al. Multiindex method using offshore oceanbottom pressure data for realtime tsunami forecast. Earth Planet Sp 68, 128 (2016). https://doi.org/10.1186/s4062301605007
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Keywords
 Realtime tsunami forecast
 Multiindex
 Variance reduction
 Tsunami Scenario Bank
 Snet