<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJAppS</journal-id><journal-title-group><journal-title>Open Journal of Applied Sciences</journal-title></journal-title-group><issn pub-type="epub">2165-3917</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojapps.2020.1012057</article-id><article-id pub-id-type="publisher-id">OJAppS-106047</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Analyzing the Annual Maximum Magnitude of Earthquakes in Japan by Extreme Value Theory
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fumio</surname><given-names>Maruyama</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Sports and Health Science, Matsumoto University, Matsumoto, Japan</addr-line></aff><pub-date pub-type="epub"><day>11</day><month>12</month><year>2020</year></pub-date><volume>10</volume><issue>12</issue><fpage>817</fpage><lpage>824</lpage><history><date date-type="received"><day>2,</day>	<month>November</month>	<year>2020</year></date><date date-type="rev-recd"><day>20,</day>	<month>December</month>	<year>2020</year>	</date><date date-type="accepted"><day>23,</day>	<month>December</month>	<year>2020</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  One of the most important and interesting issues associated with the earthquakes is the long-term trend of the extreme events. Extreme value theory provides methods for analysis of the most extreme parts of data. We estimated the annual maximum magnitude of earthquakes in Japan by extreme value theory using earthquake data between 1900 and 2019. Generalized extreme value (GEV) distribution was applied to fit the extreme indices. The distribution was used to estimate the probability of extreme values in specified time periods. The various diagnostic plots for assessing the accuracy of the GEV model fitted to the magnitude of maximum earthquakes data in Japan gave the validity of the GEV model. The extreme value index, 
  <em>&amp;#958;</em> was evaluated as 
  &amp;#8722;0.163, with a 95% confidence interval of [
  &amp;#8722;0.260, 
  &amp;#8722;0.0174] by the use of profile likelihood. Hence, the annual maximum magnitude of earthquakes has a finite upper limit. We obtained the maximum return level for the return periods of 10, 20, 50, 100 and 500 years along with their respective 95% confidence interval. Further, to get a more accurate confidence interval, we estimated the profile log-likelihood. The return level estimate was obtained as 7.83, 8.60 and 8.99, with a 95% confidence interval of [7.67, 8.06], [8.32, 9.21] and [8.61, 10.0] for the 10-, 100- and 500-year return periods, respectively. Hence, the 2011 off the Pacific coast of Tohoku Earthquake, which was the largest in the observation history of Japan, had a magnitude of 9.0, and it was a phenomenon that occurs once every 500 year.
 
</p></abstract><kwd-group><kwd>Extreme Value Theory</kwd><kwd> Generalized Extreme Value Distribution</kwd><kwd> Earthquakes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Extreme value theory has emerged as one of the most important statistical disciplines for the applied science. Using the extreme value theory, the theoretical distribution and its population parameter that the maximum value follows are estimated from long-term observation data. And the maximum value or a large value that occurs once every 100 years can be predicted based on the estimated result. Extreme value techniques are also becoming widely used for portfolio adjustment in the insurance industry, risk assessment on financial markets, and traffic prediction in telecommunications [<xref ref-type="bibr" rid="scirp.106047-ref1">1</xref>].</p><p>Statistical approaches focused on extreme values have shown promising results in forecasting unusual events in earth sciences, genetics and finance. For instance, Extreme Value Theory (EVT) was developed in the 1920s [<xref ref-type="bibr" rid="scirp.106047-ref1">1</xref>] and has been used to predict the occurrence of events as varied as droughts and flooding [<xref ref-type="bibr" rid="scirp.106047-ref2">2</xref>] or financial crashes [<xref ref-type="bibr" rid="scirp.106047-ref3">3</xref>]. Application of extreme value modeling has been published in the fields of ocean wave modeling [<xref ref-type="bibr" rid="scirp.106047-ref4">4</xref>]; wind engineering [<xref ref-type="bibr" rid="scirp.106047-ref5">5</xref>]; biomedical data processing [<xref ref-type="bibr" rid="scirp.106047-ref6">6</xref>]; thermodynamics of earthquakes [<xref ref-type="bibr" rid="scirp.106047-ref7">7</xref>]; food science [<xref ref-type="bibr" rid="scirp.106047-ref8">8</xref>]; and public health [<xref ref-type="bibr" rid="scirp.106047-ref9">9</xref>].</p><p>Applications of extreme value statistics in geology can be found in the magnitudes of and losses from earthquakes [<xref ref-type="bibr" rid="scirp.106047-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.106047-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.106047-ref12">12</xref>]. The aim of this paper is to predict extreme earthquake events in Japan using extreme value theory.</p></sec><sec id="s2"><title>2. Data and Method of Analysis</title><sec id="s2_1"><title>2.1. Data</title><p>We used the annual maximum magnitude of earthquakes in Japan for 1900-2019 by the Japan Meteorological Agency.</p></sec><sec id="s2_2"><title>2.2. Extreme Value Theory (EVT)—The Method of Block Maxima</title><sec id="s2_2_1"><title>2.2.1. General Extreme Value (GEV) Distribution</title><p>When data are taken to be the maxima (or minima) over certain blocks of time (such as annual maximum precipitation), then it is appropriate to use the Generalized Extreme Value (GEV) distribution:</p><p>G ( z ) = { exp { − [ 1 + ξ ( z − μ σ ) ] − 1 / ξ } , f o r ξ ≠ 0 exp { − exp [ − ( z − μ σ ) ] } , f o r ξ = 0 , (1)</p><p>where μ is a location parameter; σ a scale parameter; and ξ a shape parameter. G is defined for all z such that (1 + ξ (z − μ)/σ) &gt; 0 for ξ ≠ 0 and all z for ξ = 0. Three families of GEV distributions are defined depending on the value of ξ. For ξ &gt; 0 we get the Fr&#233;chet distribution with heavy tail, ξ = 0, the Gumbel distribution with lighter tail and ξ &lt; 0 the Weibull distribution with finite tail.</p><p>A method for modelling the extremes of a stationary time series is the method of block maxima, in which consecutive observations are grouped into non-overlapping blocks of length n, generating a series of m block maxima, Mn, 1, …, Mn, m, say, to which the GEV distribution can be fitted for some large value of n. The usual approach is to consider blocks of a given time length, thus yielding maxima at regular intervals [<xref ref-type="bibr" rid="scirp.106047-ref1">1</xref>].</p></sec><sec id="s2_2_2"><title>2.2.2. Return Levels</title><p>Once a GEV distribution is fitted to empirical observations, it becomes possible to estimate the probability of an event that has not been observed yet. Estimates of extreme quantiles of the annual maximum distribution are obtained by inverting Equation (1):</p><p>z p = { μ − σ ξ [ 1 − { − log ( 1 − p ) } − ξ ] , f o r ξ ≠ 0 μ − σ log { − log ( 1 − p ) } , f o r ξ = 0 , (2)</p><p>where G(z<sub>p</sub>) = 1 − p. The return level z<sub>p</sub> is associated with the return period 1/p, since to a reasonable degree of accuracy, the level z<sub>p</sub> is expected to be exceeded on average once every 1/p years. More precisely, z<sub>p</sub> is exceeded by the annual maximum in any particular year with probability p [<xref ref-type="bibr" rid="scirp.106047-ref1">1</xref>].</p><p>Modeling was performed using the ismev package in R for GEV calculations.</p></sec></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>The annual maximum magnitude of earthquakes in Japan was shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and was distributed approximately 6 to 8. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows wavelet power spectrum of the annual maximum magnitude of earthquakes in Japan. For 1950-1970 the strong period of 5 years and for 1970-2010 the strong period of 10 years were observed.</p><p>The various diagnostic plots for assessing the accuracy of the GEV model fitted to the magnitude of maximum earthquakes data in Japan are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Neither the probability plot nor the quantile plot give cause to doubt the validity of the fitted model: each set of plotted points is near-linear. In the return level curve, the estimated curve is not close to linear, since the ξis not close to zero. Finally, the corresponding density estimate seems consistent with the histogram of the data. The various diagnostic plots give little reason to doubt the validity of the GEV model, and also show how the model extrapolates.</p><p><xref ref-type="table" rid="table1">Table 1</xref> indicates the GEV parameter estimates, which were the results of the GEV modelling on the annual maximum magnitude of earthquakes in Japan using the method of block maxima. The GEV parameters were estimated using maximum Likelihood Estimation (MLE). Greater accuracy of confidence intervals can usually be achieved by the use of profile likelihood. <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the profile long-likelihood for ξ, and we estimated ξto be −0.163, with a 95% confidence interval of [−0.260, −0.0174], which is only slightly different to the earlier calculation in <xref ref-type="table" rid="table1">Table 1</xref>. Since ξ&lt; 0, the annual maximum magnitude of earthquakes in Japan has a finite upper limit and it is useful to carry out a detailed influence of the upper limit. <xref ref-type="fig" rid="fig4">Figure 4</xref>, in particular, shows considerable asymmetry in the profile log-likelihood surface, leading to confidence intervals that are asymmetric about the maximum likelihood estimate.</p><p><xref ref-type="table" rid="table2">Table 2</xref> shows the predicted maximum return level for the return periods of 10, 20, 50, 100 and 500 years along with their respective 95% confidence interval. For the 10-year return period, we estimated return level to be 7.84, with a 95% confidence interval of [7.65, 8.22]. For the 100-year return period, we estimated return level to be 8.60, with a 95% confidence interval of [8.22, 8.99]. Another way to interpret the plot is to say that there is approximately a 1% chance (1/100) each year that the magnitude of earthquake will exceed 8.60. There is approximately a 10% chance (1/10) each year that the magnitude of earthquake will exceed 7.84. For the 500-year return period, we estimated return level to be 8.99, with a 95% confidence interval of [8.40, 9.58].</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> GEV parameter estimates</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >μ</th><th align="center" valign="middle" >σ</th><th align="center" valign="middle" >ξ</th></tr></thead><tr><td align="center" valign="middle" >Parameter estimate</td><td align="center" valign="middle" >6.78</td><td align="center" valign="middle" >0.561</td><td align="center" valign="middle" >−0.159</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.0622</td><td align="center" valign="middle" >0.0437</td><td align="center" valign="middle" >0.0611</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[6.65, 6.90]</td><td align="center" valign="middle" >[0.475, 0.646]</td><td align="center" valign="middle" >[−0.279, −0.0397]</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> GEV return level estimates</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Return period (year)</th><th align="center" valign="middle" >10</th><th align="center" valign="middle" >20</th><th align="center" valign="middle" >50</th><th align="center" valign="middle" >100</th><th align="center" valign="middle" >500</th></tr></thead><tr><td align="center" valign="middle" >Return level</td><td align="center" valign="middle" >7.84</td><td align="center" valign="middle" >8.10</td><td align="center" valign="middle" >8.41</td><td align="center" valign="middle" >8.60</td><td align="center" valign="middle" >8.99</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.0950</td><td align="center" valign="middle" >0.117</td><td align="center" valign="middle" >0.159</td><td align="center" valign="middle" >0.197</td><td align="center" valign="middle" >0.300</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[7.65, 8.22]</td><td align="center" valign="middle" >[7.87, 8.33]</td><td align="center" valign="middle" >[8.09, 8.72]</td><td align="center" valign="middle" >[8.22, 8.99]</td><td align="center" valign="middle" >[8.40, 9.58]</td></tr></tbody></table></table-wrap><p>To get a more accurate confidence interval, we estimated the profile log-likelihood for the 10-, 100- and 500-year return periods in the annual magnitude of maximum earthquakes in Japan. From <xref ref-type="fig" rid="fig5">Figure 5</xref>, for the 10-year return period, the estimate was obtained as 7.83, with a 95% confidence interval of [7.67, 8.06]. From <xref ref-type="fig" rid="fig6">Figure 6</xref>, for the 100-year return period, the estimate was obtained as 8.60, with a 95% confidence interval of [8.32, 9.21]. From <xref ref-type="fig" rid="fig7">Figure 7</xref>, for the 500-year return period, the estimate was obtained as 8.99, with a 95% confidence interval of [8.61, 10.0]. Those results were only slightly different to the earlier calculations. The 2011 off the Pacific coast of Tohoku Earthquake, which was the largest in the observation history of Japan, had a magnitude of 9.0. It is a phenomenon that occurs once every 500 year. The 1995 Southern Hyogo Prefecture Earthquake and the 2016 Kumamoto Earthquake had a magnitude of 7.3. It is a phenomenon that occurs once every 3.5 year.</p></sec><sec id="s4"><title>4. Conclusions</title><p>We estimated the annual maximum magnitude of earthquakes in Japan by extreme value theory using earthquake data between 1900 and 2019. The GEV distribution was applied to fit the extreme indices. Our results are summarized as follows:</p><p>1) The various diagnostic plots for assessing the accuracy of the GEV model fitted to the magnitude of maximum earthquakes data in Japan gave the validity of the GEV model.</p><p>2) The extreme value index, ξ was evaluated as −0.163, with a 95% confidence interval of [−0.260, −0.0174] by the use of profile likelihood. Hence, the annual maximum magnitude of earthquakes has a finite upper limit.</p><p>3) We obtained the maximum return level for the return periods of 10, 20, 50, 100 and 500 years along with their respective 95% confidence interval.</p><p>4) To get a more accurate confidence interval, we estimated the profile log-likelihood. For the 10-, 100- and 500-year return periods, the return level estimate was obtained as 7.83, 8.60 and 8.99, with a 95% confidence interval of [7.67, 8.06], [8.32, 9.21] and [8.61, 10.0], respectively. Hence, the 2011 off the Pacific coast of Tohoku Earthquake, which was the largest in the observation history of Japan, had a magnitude of 9.0, and it was a phenomenon that occurs once every 500 year.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Maruyama, F. (2020) Analyzing the Annual Maximum Magnitude of Earthquakes in Japan by Extreme Value Theory. 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