<?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">GEP</journal-id><journal-title-group><journal-title>Journal of Geoscience and Environment Protection</journal-title></journal-title-group><issn pub-type="epub">2327-4336</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/gep.2023.116007</article-id><article-id pub-id-type="publisher-id">GEP-125847</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Analyzing of the ENSO Index Using 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></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>13</day><month>06</month><year>2023</year></pub-date><volume>11</volume><issue>06</issue><fpage>96</fpage><lpage>105</lpage><history><date date-type="received"><day>30,</day>	<month>April</month>	<year>2023</year></date><date date-type="rev-recd"><day>25,</day>	<month>June</month>	<year>2023</year>	</date><date date-type="accepted"><day>28,</day>	<month>June</month>	<year>2023</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>
 
 
  We predicted the extreme values of the ENSO index, the Ni
  &amp;#241;o3.4 index, and 
  the Southern Oscillation Index (SOI)
   using extreme value theory. 
  Various diagnostic plots for assessing the accuracy of the 
  Generalized Pareto (GP)
   model fitted to the Ni&amp;#241;o3.4 index and SOI are shown, and all four diagnostic plots support the fitted GP model. Because the shape parameter of the Ni&amp;#241;o3.4 was negative, the Ni&amp;#241;o3.4 index had a finite upper limit. In contrast, that of the SOI was zero, therefore the SOI did not have a finite upper limit, and there is a possibility that a significant risk will occur. We predicted the maximum return level for the return periods of 10, 20, 50, 100, 350, and 500 years and their respective 95% confidence intervals, CI. The 10-year, and 100-year return levels for Ni&amp;#241;o3.4 were estimated to be 2.41, and 2.62, with 95% CI [2.22, 2.59], and [2.58, 2.66], respectively. The Ni&amp;#241;o3.4 index was 2.65 in the 2015/16 super El Ni&amp;#241;o, which is a phenomenon that occurs once every 500 years. The Ni&amp;#241;o3.4 index was 2.51 in the 1982/83, and 1997/98 super El Ni&amp;#241;o, which is a phenomenon that occurs once every 20 years. Recently, a large super El Ni&amp;#241;o event with a small probability of occurrence has occurred. In response to global warming, the super El Ni&amp;#241;o events are becoming more likely to occur.
 
</p></abstract><kwd-group><kwd>Extreme Value Theory</kwd><kwd> GP</kwd><kwd> ENSO</kwd><kwd> Ni&#241;o3.4</kwd><kwd> SOI</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The Ni&#241;o 3.4 index is the most commonly used index to define El Ni&#241;o and La Ni&#241;a events. The Southern Oscillation Index (SOI) is a standardized index based on the observed sea-level pressure differences between Tahiti and Darwin, Australia. The SOI measures the large-scale fluctuations in air pressure occurring between the western and eastern tropical Pacific during El Ni&#241;o and La Ni&#241;a episodes. Generally, the smoothed time series of the SOI corresponds well to changes in ocean temperatures across the eastern tropical Pacific. The negative phase of the SOI represents below-normal air pressure in Tahiti and above-normal air pressure in Darwin. Prolonged periods of negative (positive) SOI values coincide with abnormally warm (cold) ocean waters across the eastern tropical Pacific, which is typical of El Ni&#241;o (La Ni&#241;a) episodes.</p><p>Extreme value theory (EVT) has emerged as an important statistical discipline in applied science. Extreme value techniques are widely used in many other disciplines. For example, portfolio adjustment in the insurance industry, risk assessment in financial markets, and traffic prediction in telecommunications  (Coles, 2001) .</p><p>Statistical approaches focused on extreme values have shown promising results in unusual forecasting events in earth sciences, genetics, and finance. For instance, EVT was developed in the 1920s  (Coles, 2001)  and has been used to predict the occurrence of events, such as droughts and flooding  (Katz et al., 2002)  or financial crashes  (Embrechts et al., 1997) . Additionally, extreme value modeling has been applied in the fields of ocean wave modeling  (Dawson, 2000) , wind engineering  (Harris, 2001) , biomedical data processing  (Roberts, 2000) , earthquake thermodynamics  (Alexandros et al., 2007) , and public health  (Thomas et al., 2016) .</p><p>The monthly maximum rainfall data were modeled using the generalized extreme value models  (Yin et al., 2014;   Onwuegbuche et al., 2019) .  Zhang et al. (2010)  fitted the generalized extreme value (GEV) distribution to the winter season maximum daily precipitation at many individual sites over North America with ENSO as a predictor of the parameters of the GEV distribution. This study predicts the extreme values of the Ni&#241;o3.4 index, and SOI using the extreme value theory. An El Ni&#241;o with particularly large amplitude is called super El Ni&#241;o. A super El Ni&#241;o disproportionately affects economies, societies, and ecosystems. Despite their importance, we do not fully understand how super El Ni&#241;o develops its intensity and unique characteristics  (Saji et al., 2018) . The 2015 super El Ni&#241;o event has been widely recognized as comparable to the 1982, and 1997 El Ni&#241;o events  (Ren et al., 2017) . The observational analyses and modeling studies demonstrate that the principal difference between the 2015 and past super El Ni&#241;o events lies in the exceptionally strong and consecutive occurrence of westerly wind burst events  (Chen et al., 2017) . Therefore, it is essential to predict super El Ni&#241;o events.</p></sec><sec id="s2"><title>2. Data and Method of Analysis</title><sec id="s2_1"><title>2.1. Data</title><p>The Ni&#241;o3.4 index and SOI provided by NOAA’s Climate Prediction Center, USA (CPC) were used. The monthly Ni&#241;o3.4 index, which is a measure of the amplitude of an ENSO event, is defined as the monthly sea surface temperature (SST) averaged over the tropical Pacific areas (5˚N - 5˚S, 120˚ - 170˚W). The SOI is a standardized index based on the observed sea-level pressure differences between Tahiti and Darwin, Australia. The negative (positive) SOI values coincide with abnormally warm (cold) ocean waters across the eastern tropical Pacific, which is typical of El Ni&#241;o (La Ni&#241;a) episodes.</p></sec><sec id="s2_2"><title>2.2. Extreme Value Theory</title><sec id="s2_2_1"><title>2.2.1. Generalized Pareto (GP) Distributions</title><p>The modeling only block maxima is a wasteful approach to extreme value analysis if other data on extremes are available. In this technique, the data are collected over a specific threshold value. Modeling the extremes using this method enables a more efficient usage of extreme value information than that given by an analysis of annual maxima data, which excludes many extreme events that did not happen to be the largest annual event. In this study, the data were fitted to the GP distribution:</p><p>G ( z ) = 1 − [ 1 + ξ ( z − u σ ) ] − 1 / ξ , for ξ ≠ 0 ,</p><p>G ( z ) = 1 − exp ( − ( z − u σ ) ) , for ξ = 0 , (1)</p><p>where z is the extreme value from the blocks, u is the known threshold, σ is the scale parameter, and ξ is the shape parameter.</p></sec><sec id="s2_2_2"><title>2.2.2. Return Levels</title><p>The level of return for the GP distribution is formed by the geometric locations of the points (m, x<sub>m</sub>) for large values of m, where x<sub>m</sub> is the return level estimated from the m-observation:</p><p>x m = u + σ ξ [ ( m ζ u ) ξ − 1 ] , for ξ ≠ 0 ,</p><p>x m = u + σ log ( m ζ u ) , for ξ = 0 , (2)</p><p>where u is the selected threshold value, ζ u = Pr ( x &gt; u ) = k / n , k is the number of exceedances, and n is the number of observations.</p><p>Modeling was performed using the evd package in R for GP distribution calculations. Because we want to know how small the value will be as a strong El Ni&#241;o event, we need to multiply the SOI data by –1 to put it in the framework of extremum statistics that considers the maximum.</p></sec></sec></sec><sec id="s3"><title>3. Results</title><sec id="s3_1"><title>3.1. Ni&#241;o3.4 Index</title><p>The Ni&#241;o3.4 index is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the wavelet power spectrum of the Ni&#241;o3.4 index. For 1980-1990, a strong priority over four years was observed.</p><p><xref ref-type="table" rid="table1">Table 1</xref> shows the results of the GP modeling on the Ni&#241;o3.4 index. The model has the scale parameter, σ, and shape parameter, ξ. Because ξ is negative, the Ni&#241;o3.4 index has a finite upper limit.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> GP parameter estimates for the Ni&#241;o3.4</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></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" >1.02</td><td align="center" valign="middle" >–0.880</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.213</td><td align="center" valign="middle" >0.196</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[0.599, 1.43]</td><td align="center" valign="middle" >[–1.26, –0.496]</td></tr></tbody></table></table-wrap><p><xref ref-type="table" rid="table2">Table 2</xref> shows the predicted maximum return levels for the return periods of 10, 20, 50, 100, 350, and 500 years and their respective 95% confidence intervals, CI. The 10-year return level was estimated to be 1.12, with 95% CI [1.04, 1.21]. The 100-year return level was estimated to be 2.13, with 95% CI [1.97, 2.30]. Another way to interpret the plot is to say that there is an approximately 1% chance (1/100) each year that the Ni&#241;o3.4 index will exceed 2.13. There is an approximately 10% chance (1/10) each year that the Ni&#241;o3.4 index will exceed 1.12.</p><p>Various diagnostic plots for the fitted GP distributions are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Straight lines and curves represent the estimated functions. Each point plot represents a realization value. The lines on both sides represent the 95% CI. The output provides little reason to doubt the validity of the GP model. Neither the probability plot nor the quantile plot doubts the validity of the fitted model: each set of plotted points is near-linear. In the return level curve, the estimated curve is not linear because ξ is not close to zero. Finally, the corresponding density estimates are consistent with the data. Consequently, all four diagnostic plots support the fitted GP model. Because there were 39 exceedances of the threshold u = 1.5 in the complete set of 840 observations, the maximum likelihood estimate of the exceedance probability was 0.0473.</p></sec><sec id="s3_2"><title>3.2. SOI</title><p>The SOI is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows the wavelet power spectrum of the SOI. For 1980-1990, a strong priority of four years was observed.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> GP return level estimates for the Ni&#241;o3.4</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" >350</th><th align="center" valign="middle" >500</th></tr></thead><tr><td align="center" valign="middle" >Return level</td><td align="center" valign="middle" >2.41</td><td align="center" valign="middle" >2.52</td><td align="center" valign="middle" >2.59</td><td align="center" valign="middle" >2.62</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" >2.65</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.0935</td><td align="center" valign="middle" >0.0621</td><td align="center" valign="middle" >0.0305</td><td align="center" valign="middle" >0.0186</td><td align="center" valign="middle" >0.0181</td><td align="center" valign="middle" >0.0193</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[2.22, 2.59]</td><td align="center" valign="middle" >[2.40, 2.64]</td><td align="center" valign="middle" >[2.53, 2.65]</td><td align="center" valign="middle" >[2.58, 2.66]</td><td align="center" valign="middle" >[2.61, 2.68]</td><td align="center" valign="middle" >[2.61, 2.68]</td></tr></tbody></table></table-wrap><p><xref ref-type="table" rid="table3">Table 3</xref> shows the results of GP modeling on the SOI. ξ was close to zero (0.0402) and included zero as a confidence interval. Therefore, the SOI does not have a finite upper limit. <xref ref-type="table" rid="table4">Table 4</xref> shows the predicted maximum return levels for the return periods of 10, 20, 50, 100, 350, and 500 years and their respective 95% CI. The 10-year return level was estimated to be –3.94, with 95% CI [–4.48, –3.41]. The 100-year return level was estimated to be –6.26, with 95% CI [–8.49, –4.03].</p><p>The various diagnostic plots for the fitted GPD are shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>. The output gives little reason to doubt the validity of the GP model. Neither the probability plot nor the quantile plot doubts the validity of the fitted model: each set of plotted points is near-linear. Furthermore, the estimated curve in the return level curve is linear because ξ is close to zero. Finally, the corresponding density estimate is consistent with the data. Consequently, all the four diagnostic plots supported the fitted GP model. Because there were 44 exceedances of the threshold u = 2.2 in the complete set of 804 observations, the maximum likelihood estimate of the exceedance probability was 0.0548.</p></sec></sec><sec id="s4"><title>4. Discussion</title><p>The return level at each return period for Ni&#241;o3.4 is shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. In the case of ξ &lt; 0, for the Ni&#241;o3.4, the plots deviated from a straight line and were convex upward. According to the Ni&#241;o3.4 index, the super El Ni&#241;o was the largest in the 2015/16, followed by the 1982/83, and 1997/98 El Ni&#241;o events. In the 2015/16 case, the amplitude and area of a negative horseshoe-shaped sea surface temperature (SST) anomaly in the Pacific Ocean were the smallest in the three cases, and a negative SST anomaly in the Philippine Sea was weaker than in the previous two cases  (Shiozaki &amp; Enomoto, 2020) . The Ni&#241;o3.4 index was 2.65 in the 2015/16 super El Ni&#241;o, which is a phenomenon that occurs once every 500 years, because the 500-year return level was 2.65 (<xref ref-type="table" rid="table2">Table 2</xref>). The Ni&#241;o3.4 index was 2.51 in the 1982/83, and 1997/98 super El Ni&#241;o, which is a phenomenon that occurs once every 20 years, as shown in <xref ref-type="table" rid="table2">Table 2</xref>. In response to global warming, the super El Ni&#241;o events are becoming more likely to occur.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> GP parameter estimates for the SOI</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></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" >0.890</td><td align="center" valign="middle" >0.0402</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.221</td><td align="center" valign="middle" >0.197</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[0.457, 1.32]</td><td align="center" valign="middle" >[–0.347, 0.427]</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> GP return level estimates for the SOI</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" >350</th><th align="center" valign="middle" >500</th></tr></thead><tr><td align="center" valign="middle" >Return level</td><td align="center" valign="middle" >–3.94</td><td align="center" valign="middle" >–4.62</td><td align="center" valign="middle" >–5.54</td><td align="center" valign="middle" >–6.26</td><td align="center" valign="middle" >–7.61</td><td align="center" valign="middle" >–8.01</td></tr><tr><td align="center" valign="middle" >Standard errors</td><td align="center" valign="middle" >0.273</td><td align="center" valign="middle" >0.411</td><td align="center" valign="middle" >0.748</td><td align="center" valign="middle" >1.14</td><td align="center" valign="middle" >2.14</td><td align="center" valign="middle" >2.50</td></tr><tr><td align="center" valign="middle" >95% CI</td><td align="center" valign="middle" >[–4.48, –3.41]</td><td align="center" valign="middle" >[–5.42, –3.81]</td><td align="center" valign="middle" >[–7.06, –4.07]</td><td align="center" valign="middle" >[–8.49, –4.03]</td><td align="center" valign="middle" >[–11.8, –3.41]</td><td align="center" valign="middle" >[–12.9, –3.10]</td></tr></tbody></table></table-wrap><p><xref ref-type="fig" rid="fig7">Figure 7</xref> also shows the return level for each return period for the SOI. It increased significantly, which corresponded to have no upper limit in the case of ξ = 0. The ξ = 0 case exhibited a heavy-tailed distribution. In the ξ = 0 case, the upper limit is infinite, therefore there is a possibility that a significant risk will occur. According to the SOI, the super El Ni&#241;o was the largest in the 1982/83, followed by the 1997/98, and 2015/16 cases. The SOI in the 2015/16 El Ni&#241;o was large, because the Walker circulation was weakened in narrower zonal extent owing to the westernmost positive SST anomaly in the eastern Pacific Ocean than in the 1982/83, and 1997/98 El Ni&#241;o  (Shiozaki &amp; Enomoto, 2020) . The SOI was –3.6 in the 2015/16 super El Ni&#241;o, which is a phenomenon that occurs once every 10 years, is shown in <xref ref-type="table" rid="table2">Table 2</xref>. The SOI were –6 and –4.4 in the 1982/83, and 1997/98 super El Ni&#241;o, respectively, which is a phenomenon that occurs once every 100, and 20 years, as shown in <xref ref-type="table" rid="table4">Table 4</xref>.</p></sec><sec id="s5"><title>5. Conclusion</title><p>We predicted the extreme values of the Ni&#241;o3.4 index and SOI using the extreme value theory. The main findings are summarized as follows:</p><p>1) Various diagnostic plots for assessing the accuracy of the GP model fitted to the Ni&#241;o3.4 index and SOI are shown, and all four diagnostic plots support the fitted GP model. Because the shape parameter of the Ni&#241;o3.4 was negative, the Ni&#241;o3.4 index had a finite upper limit. In contrast, that of the SOI was zero, so the SOI did not have a finite upper limit, and there is a possibility that a significant risk will occur.</p><p>2) We predicted the maximum return level for the return periods of 10, 20, 50, 100, 350, and 500 years along with their respective 95% confidence intervals. As a result, the 10-year and 100-year return levels for Ni&#241;o3.4 were estimated to be 2.41 and 2.62, with 95% CI [2.22, 2.59], and [2.58, 2.66], respectively.</p><p>3) The Ni&#241;o3.4 index was 2.65 in the 2015/16 super El Ni&#241;o, which is a phenomenon that occurs once every 500 years. The Ni&#241;o3.4 index was 2.51 in the 1982/83, and 1997/98 super El Ni&#241;o, which is a phenomenon that occurs once every 20 years. Recently, a large super El Ni&#241;o with small probability of occurrence has occurred. In response to global warming, super El Ni&#241;o events are becoming more likely to occur.</p><p>We want to make more accurate super El Ni&#241;o predictions.</p><p>4) The return level at each return period for the Ni&#241;o3.4 deviated from the straight line and was convex upward, corresponding to having an upper limit in the case of ξ &lt; 0. On the other hand, that of SOI increased cleanly, and it corresponded to having no upper limit in the case of ξ = 0.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Maruyama, F. (2023). Analyzing of the ENSO Index Using Extreme Value Theory. Journal of Geoscience and Environment Protection, 11, 96-105. https://doi.org/10.4236/gep.2023.116007</p></sec></body><back><ref-list><title>References</title><ref id="scirp.125847-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Alexandros, A. Z., Nickolaos, E. F., &amp; Athanasios, A. P. (2007). Modeling Earthquake Risk via Extreme Value Theory and Pricing the Respective Catastrophe Bonds. ASTIN Bulletin, 37, 163-183. https://doi.org/10.2143/AST.37.1.2020804</mixed-citation></ref><ref id="scirp.125847-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Chen, L., Li, T., Wang, B., &amp; Wang, L. (2017). Formation Mechanism for 2015/16 Super El Ni&amp;#241;o. Scientific Reports, 7, Article No. 2975. https://doi.org/10.1038/s41598-017-02926-3</mixed-citation></ref><ref id="scirp.125847-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Coles, S. (2001). An Introduction to Statistical Modeling of Extreme Values. Springer-Verlag. https://doi.org/10.1007/978-1-4471-3675-0</mixed-citation></ref><ref id="scirp.125847-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Dawson, T. H. (2000). Maximum Wave Crests in Heavy Seas. Journal of Offshore Mechanics and Arctic Engineering-Transactions of the AMSE, 122, 222-224. https://doi.org/10.1115/1.1287039</mixed-citation></ref><ref id="scirp.125847-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Embrechts, P., Kluppelberg, C., &amp; Mikosch, T. (1997). Modeling Extremal Events for Insurance and Finance. Springer-Verlag. https://doi.org/10.1007/978-3-642-33483-2</mixed-citation></ref><ref id="scirp.125847-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Harris, R. I. (2001). The Accuracy of Design Values Predicted from Extreme Value Analysis. Journal of Wind Engineering and Industrial Aerodynamics, 89, 153-164. https://doi.org/10.1016/S0167-6105(00)00060-X</mixed-citation></ref><ref id="scirp.125847-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Katz, R. W, Parlange, M. B., &amp; Naveau, P. (2002). Statistics of Extremes in Hydrology. Advances in Water Resources, 25, 1287-304. https://doi.org/10.1016/S0309-1708(02)00056-8</mixed-citation></ref><ref id="scirp.125847-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Onwuegbuche, F. C., Kenyatta, A. B., Affognon, S. B., Enock, E. P., &amp; Akinade, M. O. (2019). Application of Extreme Value Theory in Predicting Climate Change Induced Extreme Rainfall in Kenya. International Journal of Statistics and Probability, 8, 85-94. https://doi.org/10.5539/ijsp.v8n4p85</mixed-citation></ref><ref id="scirp.125847-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Ren, H. L., Wang, R., Zhai, P., Ding, Y., &amp; Lu, B. (2017). Upper-Ocean Dynamical Features and Prediction of the Super El Nino in 2015/16: A Comparison with the Cases in 1982/83 and 1997/98. Journal of Meteorological Research, 31, 278-294. https://doi.org/10.1007/s13351-017-6194-3</mixed-citation></ref><ref id="scirp.125847-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Roberts, S. J. (2000). Extreme Value Statistics for Novelty Detection in Biomedical Data Processing. IEE Proceedings—Science Measurement and Technology, 147, 363-367. https://doi.org/10.1049/ip-smt:20000841</mixed-citation></ref><ref id="scirp.125847-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Saji, N. H., Jin, D., &amp; Thilakan, V. (2018). A Model for Super El Ninos. Nature Communications, 9, 2528-2515. https://doi.org/10.1038/s41467-018-04803-7</mixed-citation></ref><ref id="scirp.125847-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Shiozaki, M., &amp; Enomoto, T. (2020). Comparison of the 2015/16 El Ni&amp;#241;o with the Two Previous Strongest Events. SOLA, 16, 12-16. https://doi.org/10.2151/sola.2020-003</mixed-citation></ref><ref id="scirp.125847-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Thomas, M., Lemaitre, M., Wilson, M. L., Vibound, C., Yordanov, Y., Wackernagel, H., &amp; Carrat, F. (2016). Applications of Extreme Value Theory in Public Health. PLOS ONE, 11, e0159312. https://doi.org/10.1371/journal.pone.0159312</mixed-citation></ref><ref id="scirp.125847-ref14"><label>14</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Yin</surname><given-names> Y.</given-names></name>,<name name-style="western"><surname> Xu</surname><given-names> C. Y.</given-names></name>,<name name-style="western"><surname> Chen</surname><given-names> H.</given-names></name>,<name name-style="western"><surname> Li</surname><given-names> L.</given-names></name>,<name name-style="western"><surname> Li</surname><given-names> H.</given-names></name>,<name name-style="western"><surname> &amp; Xu</surname><given-names> H. </given-names></name>,<etal>et al</etal>. (<year>2014</year>)<article-title>. Modeling the Extreme Precipitation Using the Generalized Extreme Value Models with Southern Oscillation Index (SOI) as a Covariate in the Beas Basin, India</article-title><source> Geophysical Research Abstracts</source><volume> 16</volume>,<fpage> EGU2014</fpage>-<lpage>6751</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.125847-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, X., Wang, J., Zwiers, F. W., &amp; Groisman, P. Y. (2010). The Influence of Large Scale Climate Variability on Winter Maximum Daily Precipitation over North America. Journal of Climate, 23, 2902-2915. https://doi.org/10.1175/2010JCLI3249.1</mixed-citation></ref></ref-list></back></article>