# The double branching model for earthquake forecast applied to the Japanese seismicity

- Anna Maria Lombardi
^{1}Email author and - Warner Marzocchi
^{1}

**63**:3

https://doi.org/10.5047/eps.2011.02.001

© The Society of Geomagnetism and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; The Geodetic Society of Japan; The Japanese Society for Planetary Sciences; TERRAPUB. 2011

**Received: **1 April 2010

**Accepted: **1 February 2011

**Published: **4 March 2011

## Abstract

The purpose of this work is to apply the Double Branching Model (DBM) to forecast moderate–large Japanese seismicity. The proposed model is time-dependent, since it assumes that each earthquake can generate or is correlated to other earthquakes, through physical mechanisms acting at different spatio-temporal scales. The model is set up through two sequential steps. In the first step, we estimate the well-established short time clustering. Then, we analyze and characterize the declustered catalog through a second order branching process. The inclusion of the second branching is motivated by the statistically significant departure of the declustered catalog from a time-independent model. From a physical point of view, this new branching accounts for possible long-term earthquake interactions. Some recent applications of this model at global and regional scales (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010) have shown that earthquake occurrences tend to have two main time features: a short-term clustering up to months–few years and a longer time modulation of decades (up to few centuries). Here we apply the DBM to the instrumental Japanese database, collected by the Japan Meterological Agency (JMA) (*M* = 5.0). The purpose of this application is twofold. First, we check the existence of two time branchings previously found in other regions. Second, we provide forecasts to be evaluated by the Japanese CSEP (Collaboratory for the Study of Earthquake Predictability) testing center.

## Key words

## 1. Introduction

Earthquake forecasting has a key role in the geophysical investigation. It has direct implications for planning risk mitigation actions, and it yields important contributions for a better understanding of earthquake generation process. Presently, a large variety of models is available; these models are based on different physical and stochastic components and they cover quite different forecasting time windows, from 1 day to years and decades (see, e.g., Kagan and Knopoff, 1981; Ogata, 1988, 1998; Kagan and Jackson, 2000; Rhoades and Evison, 2004; Gerstenberger et al., 2005; Helmstetter et al., 2006; Marzocchi and Lombardi, 2008, 2009; Lombardi and Marzocchi, 2009; Marzocchi et al., 2009; Console et al., 2010).

Despite the efforts devoted to build models, their reliability has been only partially checked (mostly by the same modelers), often using past data and different statistical methodologies. Moreover, very few attempts have been made to compare the forecasting capabilities of different models. The use of different and inhomogeneous procedures leads to an inherent difficulty to judge what is the best performing model, or more generally, to evaluate relative forecasting performances. Only recently, one important international effort, the Collaboratory for the Study of Earthquake Predictability (CSEP; www.cseptesting.org), has been set to create a common platform for testing and comparing forecasting/prediction models. This initiative is a generalization of the experiment carried out in California, named the Regional Earthquake Likelihood Models (RELM, www.relm.org; Schorlemmer et al., 2007). Specifically, CSEP has established different testing regions and testing center for evaluating and comparing forecasting/prediction models on different forecasting time windows (Schorlemmer et al., 2010). Recently, Japan joined the CSEP initiative establishing a testing center and a testing region (Tsuruoka et al., 2008).

The goal of the present paper is twofold. First, we describe the implementation of a recently proposed model, named the Double Branching Model (DBM hereinafter), to forecast earthquakes in the Japan testing region. Second, the comparison of the parameters of the model estimated for Japan and other regions of the world allows us to get some new insights on the nature of the earthquake occurrence process. The DBM takes into account long-term modulation of earthquakes occurrence, beside of the short-term clustering of earthquakes. In other words, compared to the classical ETAS (Epidemic Type-Aftershocks Sequences) model (Ogata, 1998), we relax the assumption of longterm stationary seismic background that has been questioned by many recent studies (Kagan and Jackson, 1991; Rhoades and Evison, 2004; Lombardi and Marzocchi, 2007; Marzocchi and Lombardi, 2008; Marzocchi et al., 2009). These studies emphasizes the existence of significant long-term time modulation of the earthquake occurrence, probably due to fault interaction and stress perturbations on spatio-temporal scales much larger than the ranges interested by aftershock sequences. Other possible departures from a stationary seismic background on a time scale of few days (Hainzl and Ogata, 2005; Lombardi et al., 2006, 2010) are not taken into account by DBM. Notably, the DBM has shown better earthquake forecasting performances for large earthquakes at both worldwide (Marzocchi and Lombardi, 2008) and regional (Lombardi and Marzocchi, 2009, 2010) scales, with respect to models with a time-independent background rate. The forecast method uses earthquake data only, with no explicit use of tectonic, geologic, or geodetic information. The basis underlying this earthquake forecasting method is the popular concept of epidemic process: every earthquake is regarded as a potential triggering event for subsequent earthquakes (Ogata, 1988, 1998; Helmstetter et al., 2006; Lombardi and Marzocchi, 2007) on different spatio-temporal scales. The method does not deal with single earthquake prediction, but quantifies the chance of an earthquake by estimating the mean rate of future seismicity.

## 2. The Double Branching Model

*t*and

*M*

_{min}is the minimum magnitude of catalog. The parameter

*v*indicates the overall background rate and

*u*(

*x, y*) is the probability density function (PDF) of locations of spontaneous events.

*K*

_{1},

*c*and

*p*are the parameters of the modified Omori Law defining the temporal decaying of short-term triggering effect. The long-term triggering effect is described in time by an inverse exponential function with a characteristic time

*t*. This parameterization aims at reproducing the temporal evolution of the postseismic stress variations. Usually, the latter are modeled by a sum of exponential decays, mimicking different relaxation modes (Pollitz, 1992; Piersanti et al., 1995); in our model we assume that one relaxation mode is predominant. Parameters

*a*

_{1}and

*a*

_{2}define, respectively, the dependence (assumed of exponential type) of short and long-term triggering effect with the magnitude of exciting event. The spatial decays of short and long-term stress variations are described by two inverse power PDF, with parameters (

*d*

_{1},

*q*

_{1}) and (

*d*

_{2},

*q*

_{2}), respectively ( and are the normalization constants and

*r*

_{ i }marks the distance between a general location (

*x*,

*y*) and the epicenter of the i-th earthquake (

*x*

_{ i },

*y*

_{ i })). For all events the magnitude distribution is assumed in agreement with a Gutenberg-Richter law (Gutenberg and Richter, 1954) with a parameter

*ß*=

*b*· ln(10). Finally

*w*

_{ i }is the probability that the

*i*-th event is not coseismically triggered and it is calculated by using the ETAS model. Specifically by Eq. (1) we can compute the probabilities that the

*i*-th event is short-term triggered , is long-term triggered or is most related to tectonic loading . These probabilities are given by:where

*r*

_{ ij }is the distance between the epicenters of

*i*-th and

*j*-th events. The weights

*w*

_{ i }of Eq. (1) are therefore given by:

To estimate the parameters of the model we use the iteration algorithm developed by Zhuang et al. (2002); the method is based on the Maximum Likelihood Method and on a kernel estimation of total seismic rate. Further details on the model and on estimation of its parameters can be found in Marzocchi and Lombardi (2008).

## 3. Application of Double Branching Model to Japanese Catalog

*u*(

*x, y*); see Eq. (1)) by mean of Maximum Likelihood Method. Table 1 lists the inferred values of model parameters together with their errors. The values of parameters that controlling the short-term triggering are in agreement with values found in most tectonic region. The temporal decaying of long-term interaction has a characteristic time

*t*equal to about 30 yrs. The limited temporal window covered by JMA catalog (44 years) could rise some doubts about the reliability of estimated

*t*-parameter. In any case we stress that the value of

*t*estimated in the present study is in agreement with what found in previous studies, both at global and regional scale (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010). In these studies we used datasets covering larger time windows (from one to several centuries), and then more suitable for our investigations. In order to check the reliability of the estimation of

*t*, we have verified that smaller values of

*t*do not provide a better fit of data (in terms of log-likelihood); then, we have investigated the stability of the parameter

*t*by changing the minimum magnitude. The procedure adopted to estimate the best model does not provide significantly different value of

*t*on earthquakes above

*M*5.5 and

*M*6.0 (about 900 and 300 events, respectively).

Maximum Likelihood parameters (with relative errors) of the Double Branching model (seeEq. (1)) for the events of the JMA catalog above 100 km of depth (*M*_{c} = 5.0; Jan 1 1965–Dec 31 2008, 5648 events).

Parameter | Value |
---|---|

| 61 ± 2 year |

| 7.8 ± 0.5 · 10 |

| 1.17 ± 0.01 |

| 7.0 ± 1.0 · 10 |

| 1.40 ± 0.04 |

| 4.6 ± 0.2 km |

| ≡ 1.5 |

| 0.53 ± 0.03 |

| 0.013 ± 0.001 |

| 30 ± 6 year |

| ~ 0.0 |

| 82 ± 7 km |

| 1.5 ± 0.2 |

*a*

_{2}= 0). In Fig. 3 we can see that the short-term triggering effect given by a parent event with magnitude

*M*6.0 is dominant for the first year; afterwards, the long-term magnitude-independent triggering becomes more important. For

*M*7.0, the short-term triggering prevails for the first 10 years. We underline that in Fig. 3 we plot the probabilities of direct triggering, without taking into account secondary triggering effects.

*vu*(

*x, y*), panel a), of short term triggering rate (first sum of Eq. (1), panel b) and of long-term triggering rate (second sum of Eq. (1), panel c) in the forecast region. The main contribution to overall seismicity is given by tectonic loading (35%; panel a) and short-term triggering rate (50%; panel b), but the effect of long-term triggering is not negligible (15% of the overall rate). The long-term triggered seismicity appears to be more diffuse than short term triggered events. This is due to different distances involved by two triggering mechanisms. The viscoelastic relaxation, that we hypothesize to be a possible cause of long-term interactions, decays less rapidly than co-seismic effects with distance (see Marzocchi et al., 2003). Moreover the limited duration of the JMA catalog causes a lower spatial resolution of the long-term triggering respect to the analogous and stronger short-term effect.

## 4. Checking the Model

*M*= 5.0 and at depth of 100 km or less that occurred in the same period inside the CSEP background-region and collected by the CMT (Centroid Moment Tensor, http://www.globalcmt.org/) database (67 events). All events occurred in cells with relatively high forecast rates. We remark that the forecasted rates are computed without taking into account the triggering effect of real events occurred during the year 2009. Including this effect in forecasting calculations might improve further these results.

*t*to a new scale by the increasing functionwhere

*T*

_{start}is the starting time of observation history, is the region under study and is the conditional intensity of the model, parameterized by maximum likelihood parameters.

*Λ*(

*t*) is the expected number of events since time

*T*

_{start}up to time

*t*, given the occurrence history . If the model describes well the temporal evolution of seismicity, the transformed data (residuals) are expected to behave like a stationary Poisson process with the unit rate (Papangelou, 1972; Ogata, 1988). We apply the one-sample Kolmogorov-Smirnov test (KS1) (Gibbons and Chakraborti, 2003) on residuals of the ETAS model (

*K*

_{2}= 0, see Eq. (1)) of the JMA catalog, used to set up the DBM model. We find that the Poisson hypothesis for the variable can be rejected at a significance level of 0.04. This means that the ETAS Model probably does not capture all basic features of seismicity collected into JMA catalog. On the other hand we find also that the log-likelihood of the ETAS model is larger then the log-likelihood of more sophisticated DBM, showing that the DBM does not improve the fit of the data respect to the ETAS model. This result is in disagreement with what found in other regions (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010).

We argue that the scarce fit of the ETAS model and the lack of improvement with the DBM might be due to two different factors. First, probably there may be a bias into the distance between earthquakes; in fact, both ETAS and DBM consider only epicentral distances, neglecting the depth, whereas the latter can reach up to 100 km. Second, offshore and deep earthquakes may have different features compared to crustal inland earthquakes; this difference may come up from a different resolution in monitoring (Nanjo et al., 2010); or may reflect a real physical difference between these two kind of earthquakes.

*t*, equal to about 8 years, is significantly smaller than values, all close to 30 years, estimated at local and global scale for the shallow seismicity (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010). Both the ETAS model and the DBM pass the KS1 test on residuals, but the DBM improves the likelihood on data.

Maximum Likelihood parameters (with relative errors) of the Double Branching model (see Eq. (1)) for the events of the JMA catalog above 30 km of depth (*M*_{c} = 5.0; Jan 1 1965-Dec 31 2008, 1935 events).

Parameter | Value |
---|---|

| 11 ± 1 year |

| 1.1 ±0.1 · 10 |

| 1.16 ± 0.01 |

| 6.0 ± 1.0 · 10 |

| 1.20 ± 0.04 |

| 4.6 ± 0.2 km |

| ≡ 1.5 |

| 0.53 ± 0.03 |

| 0.09 ± 0.01 |

| 8 ± 1 year |

| ~0.0 |

| 24 ± 4 km |

| 2.0 ± 0.2 |

*N*) into database

*k*

_{dbm}and

*k*

_{etas}are the numbers of free parameters for DBM and ETAS model, respectively. Therefore a better indicator of the improvement in predictability is given by

To compare real and simulated values of , we can simply translate the values of IGpe shown in Fig. 6 by the factor . So the conclusions on the significance of the improvement of DBM do not change.

*learning*dataset, can be used to set up the model and a second, the

*testing*dataset, to check its reliability. In this case the forecasts have zero degrees of freedom, since each model uses information available before the starting time of each test day. Therefore comparing the model likelihoods is sufficient. We set the

*learning*dataset as the part of the JMA catalog spanning the time interval 1965–2005 and the

*testing*dataset as the subset of events occurred from 2006 to 2008. We do not find any significant change into parameters of both ETAS model and DBM. In Fig. 7 we show the comparison of the real and simulated values of the IGpe, which remarkably confirms the significance of the improvement of DBM, respect to ETAS model.

## 5. Forecasting Maps

*M*= 5.0 and depth lower than 100 km, within a zone of 0.1° × 0.1°, in the next 5 (January 2010–December 2014) years in Japan. We stress that the magnitude range and the spatial boundaries are in agreement with choices adopted for the CSEP Japan experiment, which has mostly motivated this study. To produce forecasting calculations the DBM requires to take into account the triggering effect of seismicity occurred both before and during the forecast interval. Since this last is unknown, we simulate 10000 different stochastic realizations along the forecasting time window. For this purpose we use the thinning method proposed by Ogata (1998) and the intensity function formulated in Eq. (1). Then, we average predictions coming from each of these synthetic catalogs. Results are shown in Fig. 8. The DBM identifies as most dangerous zones the north-western coast of the testing region. One of most hazardous zones on the mainland is the region near Tokyo city and the Tokai region, in which a strong earthquake is expected in short on the basis of different models (Rikitake, 1999; Mogi, 1987).

## 6. Discussion and Conclusions

The main goal of the present paper has been to describe the DBM applied to Japanese seismicity. This study has been mainly motivated by the participation to the CSEP experiment for the Japanese testing region. From a seismolog-ical point of view, the results obtained in the present study basically confirm the main finding of previous analyses (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010). Large earthquakes in Japan tend to cluster in time and space at different time scales. Besides the short-term clustering described by the ETAS model, we have found also a significant time clustering longer than typical aftershock sequences. Notably, we have found that the DBM has a different forecasting performance on shallow and deep seismicity. Specifically the DBM has a poor reliability on seismicity with a depth up to 100 km, whereas it works significantly better than ETAS model for shallow seismic events (up to 30 km of depth). The scarce fitting with DBM and ETAS model is probably due to the use of epicentral distances; neglecting depth may alter significantly the real distance between earthquakes. Another possibility is that offshore and deeper earthquakes have different features compared to crustal inland earthquakes. The characteristic time of the second branching for the crustal earthquakes (*t* ~ 8 years) seems to be smaller than the characteristic time found in other regions (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010). We explain this shorter time length as due to the high seismic background for Japanese seismicity. In fact, the time decay of the long-term interaction will fade sooner into the background seismicity when the latter is higher. In any case the value of *t* is in agreement with Lombardi and Marzocchi (2007), which founded a significant variation of background seismicity in Japan about every 10 years.

In all our previous analyses (Marzocchi and Lombardi, 2008; Lombardi and Marzocchi, 2009, 2010), as well as in the present study, we find a low value for *a*_{2}, not statistically significant from zero. This implies that the postseis-mic triggering capability of an event is independent by its magnitude. By a physical point a view, we explain this finding with the not-suitability of the available data to provide the actual value of *a*_{2}. In fact, whereas the coseismic stress transfer is a phenomenon spanning all magnitude scales, the postseismic effects are likely mostly caused by the strongest events (Piersanti et al., 1997; Pollitz et al., 1998). The mag-nitudo range recovered by JMA and by all previously analyzed catalogs is rather small and the proportion of giant events (*M* = 8.0) is negligible. This could be the origin of the indeterminateness of the *a*_{2}-value. By a statistical point of view, we have shown that a further explanation for the uncertain estimate of the *a*_{2}-value could be the inefficiency of data to reveal its actual value (Lombardi and Marzocchi, 2009). Specifically we have shown that the probability to estimate a null value for *a*_{2} is not negligible also for a class of synthetic catalogs with *a*_{2} significantly different from 1.0 and a size comparable with the available real datasets. This is clear evidence that the limited number of data of a catalog might prevent to find a positive value of *a*_{2} significantly different from zero.

The first version of the DBM submitted for CSEP Japanese laboratory is focused on providing earthquakes forecast until 100 km depth. The results of this analysis has encouraged us to submit a new version of DBM focused only on the crustal inland earthquakes. We expect that this second version of the DBM should work better than classical ETAS models. The results of the CSEP experiment in the Japanese testing region will provide us interesting insights on this topic.

## Declarations

### Acknowledgments

The authors thank the editor and the two reviewers for useful comments and suggestions.

## Authors’ Affiliations

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