<?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">OJER</journal-id><journal-title-group><journal-title>Open Journal of Earthquake Research</journal-title></journal-title-group><issn pub-type="epub">2169-9623</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojer.2020.94018</article-id><article-id pub-id-type="publisher-id">OJER-101827</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>
 
 
  South Atlantic Anomaly Seasonal Seismicity during Two Solar Cycles
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Marilia</surname><given-names>Hagen</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Anibal</surname><given-names>Azevedo</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>1262 Yellowwood Lake Road, Nashville, USA</addr-line></aff><aff id="aff2"><addr-line>Faculdade de Ciências Aplicadas da Unicamp, Limeira, S?o Paulo </addr-line></aff><pub-date pub-type="epub"><day>28</day><month>07</month><year>2020</year></pub-date><volume>09</volume><issue>04</issue><fpage>307</fpage><lpage>322</lpage><history><date date-type="received"><day>22,</day>	<month>May</month>	<year>2020</year></date><date date-type="rev-recd"><day>26,</day>	<month>July</month>	<year>2020</year>	</date><date date-type="accepted"><day>29,</day>	<month>July</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>
 
 
  The aim of this paper is to investigate the effects of Solar cycles and season fluctuations on earthquakes, in a location named South Atlantic anomaly. The area used herein is delimited 0N, ?50S, 40E, ?90W, and is the region with the Earth’s lowest magnetic field, which allows a higher number of ionized particles to reach the ionosphere. The period chosen is 1996-2018, comprising two Solar Cycles and the respective solar maxima in 2000 and 2014. The first results pointed out that occurrences of swarm location depending from the depth search. Shallow earthquakes developed swarms near the shorelines and deep depth inland. A mathematical model was developed to statistically evaluate the changes in the earthquakes increases. The outcome resolutions showed Summer and Fall are the most important seasons for tremors in this region. The period analyzed have an extended solar minimum occurred 2003-2010, we analyzed the evolution of earthquakes occurrences under the South Atlantic anomaly. 
 
</p></abstract><kwd-group><kwd>South Atlantic Anomaly</kwd><kwd> Solar Cycles</kwd><kwd> Seasons</kwd><kwd> Earthquakes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Earth is surrounded by the dipolar or almost-spherical magnetic field, and the Sun sends electromagnetic radiation plus ionized particles towards the Earth and reaches the magnetosphere. Those particles penetrate the poles or other regions of the terrestrial magnetosphere and enter the atmosphere. The Earth’s magnetic field configuration allows the trapping and distribution of energized ionized particles in different layers. The magnitude variation of this field varies from 30,000 nT at the equator to 50,000 nT at the poles [<xref ref-type="bibr" rid="scirp.101827-ref1">1</xref>].</p><p>The South Atlantic Anomaly (SAA) is a low magnetic field area that spans from east of Africa over the Atlantic Ocean and is centered on South America (See <xref ref-type="fig" rid="fig1">Figure 1</xref>). This weak magnetic field region has expanded over time and has also moved westward; it is linked with the geomagnetic field distribution. The SAA is characterized by a lower magnetic intensity and is a location where the inner radiation belts are closest to Earth’s surface. The movement of this anomaly over South America was found as 0.06 N/yr. and 0.28 W/yr [<xref ref-type="bibr" rid="scirp.101827-ref2">2</xref>].</p><p>The energetic particles captured by the geomagnetic field can reach lower altitudes, forming a high radiation region. The SAA, when compared to other locations, indicates a more significant number of energetic particles. The eccentric dipole is currently offset from Earth’s center by about 550 km in a path approximately 22˚N, 140˚E. This distance is steadily increasing, and the location of the eccentric dipole center is drifting westward and slightly northward. In the antipodal route, which corresponds to the location of the SAA, the drift shells get closer to Earth’s surface and move mainly westward and slightly southward. The SAA is approximately centered over Sao Paulo (Brazil) [<xref ref-type="bibr" rid="scirp.101827-ref3">3</xref>].</p><p>Thermospheric density is directly correlated with the Sun’s activity due to heating driven by Solar radiation and shows the same time evolution as the Solar Cycle. The density of particles increases at high altitudes as the atmosphere expands during Solar maxima, which leads to more frequent collisions between the trapped energetic protons and atmospheric atoms. The trapped protons are depleted during the higher activity of the Solar Cycles.</p><p>Shaeffer et al. [<xref ref-type="bibr" rid="scirp.101827-ref4">4</xref>] showed that the particle hit intensity in the region was anticorrelated with the Solar activity. If there are years of high solar activity, the radiation intensity is lower, while during quiet solar years, the radiation intensity is more powerful. Their data implied the strong solar wind from the Sun sweeps out more low-energy galactic cosmic rays, while the Sun’s smooth winds let more in. The peak of SAA intensity occurs a bit later than the last year of the solar minimum. Their data connected sunspot number minimum occurring in 2009 with the peak of SAA intensity. According with them, Geomagnetic storms charge particles that are precipitated along the magnetic field lines in the auroral zone and also induce photometer counters. The SAA does not remain in a fixed</p><p>geographic location; instead, it tends to drift in a mostly west northeast direction.</p><p>McCracken et al. [<xref ref-type="bibr" rid="scirp.101827-ref5">5</xref>] studied the period 2004 to 2016 that showed particle hit intensity was anticorrelated with solar activity. The authors compared three former minimum named the three Grand Minima, the Spoerer, Maunder and Dalton minima the long sunspot minimum of 2006-2009. The heliospheric magnetic field strength (3.9 nT) observed in 2009 was much more significant than the peak values of 2.0 - 2.9 nT found for the three Grand Minima.</p><p>The evolution of the SAA particle flux can be seen as the result of two main effects: 1) the secular variation of Earth’s core magnetic field and 2) the modulation of the density of the inner radiation belts during the solar cycle, as a function of the L value that characterizes the drift shell where charged particles are trapped [<xref ref-type="bibr" rid="scirp.101827-ref6">6</xref>]. The unusual spatial characteristics for the area indicate that it would be essential to determine if those disturbances would be necessary for the earthquake's evolution. It was found that during the solar minima 2006-2010, there was an indication of higher earthquake activity in the region.</p><p>We also search for the seasonality earthquake variation in the two setups, one for all the tremors that occurred in the area, and another for the depths ≥ 200 km. The first group (all depths) identified earthquakes swarm locations at shorelines in Southern Pacific. The ones with depths ≥ 200 km occurring in a different location inland. Both scenarios, indicated tremors in the region occurring most during Summer and Fall.</p><p>The paper is divided into a brief study of a swarm of earthquakes around the southern Pacific subduction under South America, for all events and deep-depth earthquakes. Catalogs and data for earthquakes are found in [<xref ref-type="bibr" rid="scirp.101827-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref8">8</xref>]. Data for Solar Cycles are found in [<xref ref-type="bibr" rid="scirp.101827-ref9">9</xref>]. Our research considers earthquakes with M ≥ 3 since, in a past paper, we showed that lower magnitudes can be from an anthropogenic origin [<xref ref-type="bibr" rid="scirp.101827-ref10">10</xref>]. We included a section with a dependence of events into depths in this area where anomaly occurrences were found in [<xref ref-type="bibr" rid="scirp.101827-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref12">12</xref>].</p><p>To study the development of these events and parameters, it is necessary to employ a statistical, mathematical model using the number of earthquakes specified, in years and months, for two cycles.</p></sec><sec id="s2"><title>2. Swarm of Earthquakes around South America Anomaly</title><p>The following <xref ref-type="table" rid="table1">Table 1</xref> shows the locations under the South Atlantic anomaly with the occurrence of great swarms in the period 1996-2018. <xref ref-type="table" rid="table1">Table 1</xref> has 16 swarm events, which most occurrences were in the Fall, Summer/Fall, or Fall/ Winter. The following years, between 2003-2010, present the highest number of swarms and also correspond to the year of quiet solar activity [<xref ref-type="bibr" rid="scirp.101827-ref5">5</xref>]. In 2006, the swarm had two distinct periods: Fall/Winter and Winter; there were 1118 total events. Such results coinciding with [<xref ref-type="bibr" rid="scirp.101827-ref5">5</xref>] attribute maximum solar radiation during the solar minima years (See <xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>It appears that Fall drives most of the swarm earthquakes from around the</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Data swarms for earthquakes period 1996-2019, all depths</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Anomaly</th><th align="center" valign="middle" >Coordinates</th><th align="center" valign="middle" >Swarm region (number of events)</th></tr></thead><tr><td align="center" valign="middle" >1998</td><td align="center" valign="middle" >Jul-Aug</td><td align="center" valign="middle" >−27.64N, −37.47S, −66.25E, −74.85W</td><td align="center" valign="middle" >Valparaiso-Concepcion (Chile)-324</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >Apr</td><td align="center" valign="middle" >−18.94N, −40.05S, −60.30E, −74.36W</td><td align="center" valign="middle" >Chile coast-294</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >Jun</td><td align="center" valign="middle" >−14.13N, −37.17S, −64.39E, −75.28W</td><td align="center" valign="middle" >Peru/Bol&#237;via-238 -Chile Coast-111</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >Oct</td><td align="center" valign="middle" >− 18.96N, −36,58S, −64.26E, −77.97W</td><td align="center" valign="middle" >Northern/Southern Chile-119</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >Dec</td><td align="center" valign="middle" >−26.81N, −37.70S, −65.71E, −73.09W</td><td align="center" valign="middle" >Northern/Southern Chile-372</td></tr><tr><td align="center" valign="middle" >2002</td><td align="center" valign="middle" >Jan-Apr</td><td align="center" valign="middle" >−2.07N, −41.75S, −63.63E, −82.79W</td><td align="center" valign="middle" >Near coast Ecuador/ South Argentina-1051</td></tr><tr><td align="center" valign="middle" >2003</td><td align="center" valign="middle" >Apr-Jun</td><td align="center" valign="middle" >−18.89N, −39.30S, −63.75E, −73.07W</td><td align="center" valign="middle" >Near Coast Chile, S. Chile/Arg border-1273</td></tr><tr><td align="center" valign="middle" >2005</td><td align="center" valign="middle" >May-Jun</td><td align="center" valign="middle" >−13.48N, −41.43S, −64.26E, −77.27W</td><td align="center" valign="middle" >Central Peru, Near Coast Chile-470</td></tr><tr><td align="center" valign="middle" >2006</td><td align="center" valign="middle" >Apr-May</td><td align="center" valign="middle" >−25.60N, −36.21S, −67.76E, −72.58W</td><td align="center" valign="middle" >Chile/ Arg border, Central Chile-562</td></tr><tr><td align="center" valign="middle" >2006</td><td align="center" valign="middle" >Jul-Aug</td><td align="center" valign="middle" >−27.65N, −37.40S, 67.7E, −72.5W</td><td align="center" valign="middle" >Chile Coast, Central Chile-556</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >May</td><td align="center" valign="middle" >−18N, −38.15S, −62.20E, −74.68W</td><td align="center" valign="middle" >North/Southern Chile-289</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >Jul-Aug</td><td align="center" valign="middle" >−12.33N, −16.08S, −74.8E, −78.05W</td><td align="center" valign="middle" >Peru coast-South/Central Chile-737</td></tr><tr><td align="center" valign="middle" >2010</td><td align="center" valign="middle" >Feb-Apr</td><td align="center" valign="middle" >−32.27N, −39.45S, −70.37E, −75.38W</td><td align="center" valign="middle" >Coast Central Chile-1531</td></tr><tr><td align="center" valign="middle" >2014</td><td align="center" valign="middle" >Mar-Apr</td><td align="center" valign="middle" >−32.27N, −39.45S, −66.46E, −75.38W</td><td align="center" valign="middle" >Coast Central Chile-618</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >Sep-Nov</td><td align="center" valign="middle" >−27.75N, −37.57S, −68.59E, −75.18W</td><td align="center" valign="middle" >Coast and off coast Central Chile-923</td></tr><tr><td align="center" valign="middle" >2017</td><td align="center" valign="middle" >Apr</td><td align="center" valign="middle" >−19.29N, −39.35S, −65.88E, −75.73W</td><td align="center" valign="middle" >Near Coast Central and North Chile, off coast-202</td></tr></tbody></table></table-wrap><p>South Pacific shorelines to South America. The clusters were found in the same region as the entire Chile coast and Central Chile. The location is defined by −20.20N, −39.89S, −69.43E, −74.70W, with the most in-depth event in the area at 213 km.</p><p>These results indicate a correlation between the earthquakes and the Solar minimum. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the location in South America, where the clusters appeared in the maximum number of happenings.</p>Swarm of Earthquakes in South America for Deep Earthquakes<p><xref ref-type="table" rid="table2">Table 2</xref> exhibits the features for earthquakes with a depth below 200 km. First column is the year of occurrence, then the month, coordinates and swarm regions, and the number of occurrences. Observe that the swarms here are fewer events than those included in <xref ref-type="table" rid="table1">Table 1</xref>. Also, the location of these events is intraplate around Brazil and borders with other South American countries. In this case, there are the maximum number of earthquakes in 2017 (88 tremors) and 2018 (48 shocks).</p><p>Deeper earthquakes indicate that the lithosphere is uneven into these depths and must play a strict rule for the occurrences [<xref ref-type="bibr" rid="scirp.101827-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref13">13</xref>].</p><p>The years with more events were 2017 (Fall/Winter), 2018 (Fall/Winter), and the region reached was the same for both years: Chile/Argentina border, Southern Bolivia, Jujuy, and Salta (Argentina).</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows a rare circumstance of the swarm reaching the highest number of occurrences in South America. The data in the chart is from November 2015. There is a complete absence of events due to the Solar maxima, 2000 and 2014, and the highest number of clusters that happened in the period mentioned as solar minimum. Both <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref> indicate an anomaly number of earthquakes during Fall or Fall/Winter.</p><p>The next section shows the data and techniques for analysis of the earthquakes data set.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Shows data swarm of quakes for depths ≥ 200 km</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Anomaly</th><th align="center" valign="middle" >Coordinates</th><th align="center" valign="middle" >Swarm region (number of events)</th></tr></thead><tr><td align="center" valign="middle" >1997</td><td align="center" valign="middle" >Mar -Fall</td><td align="center" valign="middle" >−7.76N, −10.49S, −69.96E,−72.96W</td><td align="center" valign="middle" >Western Brazil, Peru border (3)</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >Apr-Fall</td><td align="center" valign="middle" >−16.21N, −34.23S, −61.14E,−72.04W</td><td align="center" valign="middle" >Jujuy-Argentina, Southern Bolivia, Chile/Bolivia (20)</td></tr><tr><td align="center" valign="middle" >2005</td><td align="center" valign="middle" >Mar-(Fall)</td><td align="center" valign="middle" >−16.94N, −27.78S, −60.58E,−68.38W</td><td align="center" valign="middle" >Jujuy-Argentina, Chile/Bolivia, Peru/Brazil border (17)</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >May-(Fall)</td><td align="center" valign="middle" >8.49N, −52.21S, −14.03E,−119.15W</td><td align="center" valign="middle" >Chile/Argentina, Western Brazil, S. Peru, Jujuy (13)</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >Aug-winter</td><td align="center" valign="middle" >−18.07N, −27.15S,−64.48E,−68.03W</td><td align="center" valign="middle" >S Bol&#237;via, Argentina border, Jujuy Argentina (13)</td></tr><tr><td align="center" valign="middle" >2010</td><td align="center" valign="middle" >Feb-Summer</td><td align="center" valign="middle" >−18.07N, −25.15S,−64.36E,−69.46W</td><td align="center" valign="middle" >Chile/Argentina, South Bolivia, Jujuy, (15)</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >Feb -Summer</td><td align="center" valign="middle" >−17.6N, −26.74S, −63.86E,−68.15W</td><td align="center" valign="middle" >(Jujuy, Salta) Argentina, Southern Bolivia (13)</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >Nov-Spring</td><td align="center" valign="middle" >−7.58N, −11.39S,−69.56E,−72.33W</td><td align="center" valign="middle" >Peru/Brazil border, Western Brazil (19)</td></tr><tr><td align="center" valign="middle" >2016</td><td align="center" valign="middle" >Oct-Nov Spring</td><td align="center" valign="middle" >−18.07N, −26.36S,−65E,−68W</td><td align="center" valign="middle" >Chile/Argentina border, South Bolivia (23)</td></tr><tr><td align="center" valign="middle" >2017</td><td align="center" valign="middle" >May-Jul Fall-Winter</td><td align="center" valign="middle" >−18.07N, −26.36S,−65E,−68.6</td><td align="center" valign="middle" >Chile/Argentina border, S.Bolivia, Salta, Jujuy, Mendoza (65)</td></tr><tr><td align="center" valign="middle" >2017</td><td align="center" valign="middle" >Dec Summer</td><td align="center" valign="middle" >−18.54N, −25.06S,−65.37E,−68.97W</td><td align="center" valign="middle" >Bolivia (Central, South), Jujuy, Salta, Mendoza (Argentina) (13)</td></tr><tr><td align="center" valign="middle" >2018</td><td align="center" valign="middle" >Apr-Jul Fall-Winter</td><td align="center" valign="middle" >−18.07, −27.15S,−64.48E,−69.03W</td><td align="center" valign="middle" >Jujuy, Salta, Chile/Argentina border, South Bolivia (41)</td></tr><tr><td align="center" valign="middle" >2019</td><td align="center" valign="middle" >Dec-Summer</td><td align="center" valign="middle" >−19.12N, −25.30S,−64.13E,−70.1W</td><td align="center" valign="middle" >Chile/Argentina, Jujuy (11)</td></tr></tbody></table></table-wrap></sec><sec id="s3"><title>3. Data, Techniques for Analysis</title><p>This paper is focused on a region that has earthquakes rising in different locations; part of them are at the Southern Pacific side, part in the Atlantic Ridge, and a few earthquakes in Africa. The coordinates are 0 N, -50 S, 40 E, -90W. The seasons in the Southern Hemisphere are in <xref ref-type="table" rid="table3">Table 3</xref>. The catalogs for earthquakes are from USGS and IRIS, both offering different approaches, and only USGS can map the region and display the data [<xref ref-type="bibr" rid="scirp.101827-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.101827-ref8">8</xref>].</p><sec id="s3_1"><title>3.1. Mathematical Method</title><p>The following is our method to determine if earthquakes increase, decrease, or remain constant in each region and depth: First, we collected the data for shallow earthquakes occurring at the South Atlantic anomaly; the dimensions for depth is d ≤ 200 km. Assessed events are with typical magnitudes of M ≥ 3 during the period 1996-2018. This defines the last Solar Cycles 23 and 24, the year maxima are 2000 and 2014, and the minima are 1996 and 2008. Our data offers the year, month, and number of earthquakes for each. The average is found by dividing the total amount per month by 22, which is the total number of years in the period. The tables constructed will show the year, month, and correlated number of events, on average.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Seasons in the southern hemisphere</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >South Hemisphere</th><th align="center" valign="middle" >Range</th></tr></thead><tr><td align="center" valign="middle" >Spring</td><td align="center" valign="middle" >Sept 1-Nov 30</td></tr><tr><td align="center" valign="middle" >Summer</td><td align="center" valign="middle" >Dec 1-Feb 28</td></tr><tr><td align="center" valign="middle" >Fall</td><td align="center" valign="middle" >March 1-May 30</td></tr><tr><td align="center" valign="middle" >Winter</td><td align="center" valign="middle" >Jun 1-Aug 31</td></tr></tbody></table></table-wrap></sec><sec id="s3_2"><title>3.2. Construction of Tables and Plots</title><p>The data set comprises earthquakes recorded during the period 1996-2018.</p><p>The raw data shows that several months had earthquake event anomalies, either positive or negative. It shows two types of anomalies: positive and negative. Positive anomalies are when the number of events is above average, and negative when the number of earthquakes is below average. The ones we can reveal are the positive anomalies.</p><p>Our plots are most intended to show how Solar Cycles and seasonal changes can relate to event variations. The South Atlantic Anomaly has a tight connection with geomagnetic storms which leans toward a region with a weaker magnetic field. The raw data is impossible to be studied, and it is necessary to adjust this data mathematically to find any valuable variance or connection with the described factors above.</p><p>The data values are described by year and month and they are collected for all depths during these 22 years.</p><p>∑ n 0 n n Y n = y n 0 + y n 1 + ⋅ ⋅ ⋅ + y n n ′ (1)</p><p>where n = 1996 ∙∙∙ 2018, and n ′ is 22 years.</p><p>The mean is defined as</p><p>Mean = A = ∑ n 0 n n Y n 22 (2)</p><p>Datavalue − mean = Y n ′ (3)</p><p>If Y n ′ &gt; A , the value is greater than one during that year, and it means the number of earthquakes exceeds the average. It is divided by the number/average and it gives how much the events surpassed the standard. The results are discussed in the next section. On the other hand, if Y n ′ &lt; A , the number will be less than one during that year, demonstrating that the number of earthquakes was below average.</p><p>There are two kinds of possible anomalies in the data, positive and negative. The positive anomaly is a result that is higher than the average number considered as 1. There is only one negative number found, −0.5, and it means the number of events was half of the average.</p><p>For example, in <xref ref-type="table" rid="table4">Table 4</xref>, a negative anomaly appeared in January 2010, of −0.5. This means was half of the average which is 1, considering the given month and year. The positive anomalies are numbered above 1, for example. January</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> The evolution of earthquake events for all depths period 1996-2018</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Jan</th><th align="center" valign="middle" >Feb</th><th align="center" valign="middle" >Mar</th><th align="center" valign="middle" >Apr</th><th align="center" valign="middle" >May</th><th align="center" valign="middle" >Jun</th><th align="center" valign="middle" >Jul</th><th align="center" valign="middle" >Aug</th><th align="center" valign="middle" >Sep</th><th align="center" valign="middle" >Oct</th><th align="center" valign="middle" >Nov</th><th align="center" valign="middle" >Dec</th></tr></thead><tr><td align="center" valign="middle" >1996</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >1997</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >1998</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >1999</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >−0.5</td></tr><tr><td align="center" valign="middle" >2000</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.4</td></tr><tr><td align="center" valign="middle" >2002</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2003</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2004</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >2005</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td></tr><tr><td align="center" valign="middle" >2006</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >2008</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.2</td></tr><tr><td align="center" valign="middle" >2009</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >2010</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >−0.5</td></tr><tr><td align="center" valign="middle" >2011</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td></tr><tr><td align="center" valign="middle" >2012</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2013</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.2</td></tr><tr><td align="center" valign="middle" >2014</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >2.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >2016</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2017</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2018</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td></tr></tbody></table></table-wrap><p>2011, of 1.6. It means the number of earthquakes during this month and year was 0.6 above the average number 1. The only negative anomaly allows with physical meaning is −0.5; anything lower could not be evaluated. Negative numbers below this value are regarded as zero variation for physical connotation.</p><p>Examining <xref ref-type="table" rid="table4">Table 4</xref>, in 2015, we observed four negative anomalies occurrencing during Fall and Winter and a peak in the Spring (Sept, Oct, Nov). However, 2015 is one year after a solar maximum in 2014. <xref ref-type="table" rid="table5">Table 5</xref> shows the quakes with the deepest depth and displays similar behavior in 2015, but only positive anomalies for the seasons, especially during the Spring. Both <xref ref-type="table" rid="table4">Table 4</xref> and <xref ref-type="table" rid="table5">Table 5</xref> display the evolution of earthquakes by months.</p></sec></sec><sec id="s4"><title>4. Discussion of Solar Cycles</title><p>For this part of this study we use the calculations performed in Section 2 to search the variations in the earthquakes in the area defined by 0N, −50S, 40E,</p><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Showing the results for depths ≥ 200 km</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Jan</th><th align="center" valign="middle" >Feb</th><th align="center" valign="middle" >Mar</th><th align="center" valign="middle" >Apr</th><th align="center" valign="middle" >May</th><th align="center" valign="middle" >Jun</th><th align="center" valign="middle" >Jul</th><th align="center" valign="middle" >Aug</th><th align="center" valign="middle" >Sep</th><th align="center" valign="middle" >Oct</th><th align="center" valign="middle" >Nov</th><th align="center" valign="middle" >Dec</th></tr></thead><tr><td align="center" valign="middle" >1996</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >1997</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >1998</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >1999</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2000</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >2001</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2002</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2003</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2004</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−0.6</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2005</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2006</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2007</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2008</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >2009</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−0.5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >−0.5</td></tr><tr><td align="center" valign="middle" >2010</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >2011</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2012</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >2013</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >2014</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td></tr><tr><td align="center" valign="middle" >2016</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2017</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.4</td></tr><tr><td align="center" valign="middle" >2018</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1.3</td></tr></tbody></table></table-wrap><p>and −90W. The South Atlantic Anomaly, characterized by these coordinates, indicates a domain with the lowest magnetic field that is dependent from the Solar Cycles maxima and minima (1996-2018).</p><p>As recently established, the Van Allen belts receive ionized particles from two sources: 1) in the poles by magnetic reconnection in the dayside and 2) by the reconnection at the night side when there is a rupture of the magnetic lines and ionized particles are launched inside the Van Allen belts.</p><p>The only questionable area is the South Atlantic Anomaly, when the ionized particles hit a weaker field created by the internal dynamo misalignment. These particles are unable to be trapped by the weaker field, eventually being released through plasma instabilities to the Earth’s surface. The questions here are: Are the variations in the density of the anomaly able to cause disturbances on the Earth’s surface? Are these disturbances able to affect seismologic events? The answer depends on the earth’s crustal surface and the tectonics in the area. At first, it seems that the location under the South Atlantic Anomaly with more seismic variations is situated at the shorelines of South America, between Peru and Chile. The triple junction is highly active during the period searched.</p><p>For this part of this study, we are using the calculations performed in section 2 to search the variations in earthquakes in the area defined by 0N, −50S, 40E, and −90W. Scrutinizing the data from the perspective of Solar Cycles, the years of peaks, 2000 and 2014, did not show significant variations. Instead, significant variates occurred during a minimum, as in 2010, and one year after 2014 (maximum) in 2015. Actually, the years of minima, 2003 and 2010, showed more prominent negative anomalies and also higher positive disturbances.</p></sec><sec id="s5"><title>5. Data Discussion by Seasons</title><p>With the datasets in <xref ref-type="table" rid="table4">Table 4</xref> and <xref ref-type="table" rid="table5">Table 5</xref>, we can construct the next plots for seismic event variation during seasons [<xref ref-type="bibr" rid="scirp.101827-ref14">14</xref>]. Figures 4-7 are season variations for earthquakes with magnitudes M3 or higher, all depths, during 1996 to 2018.</p><p>Spring—The highest anomaly occurred in Sep (2015), around 2.3 times the average in the period analyzed. The negative anomaly happened in Nov (2010).</p><p>Summer—The highest anomalies occurred in Feb (2010) when the intensity of earthquakes reached four times the average. In the same period, there occurred three negative irregularities Dec (1999, 2010), Jan (2010), and Feb (2014). The years of solar maxima, 2000 and 2014, did not enhance the events.</p><p>Fall—The highest positive anomaly for all seasons and years occurred in Mar (2010) when it became 5.5 times the average. Negative points occurred in Mar (2001) and Apr and May (2015). During the years of maximum, 2000 and 2014, the peak of events happened in Apr (2014).</p><p>Winter—The enhancement of events occurred in Aug (2007), with the highest number of occurrences. The lowest anomalies in July and Aug (2015). Nevertheless, it is the season that had the weakest variations in the period searched.</p>Discussions on Seasons for All Depths<p>In comparing the dataset for Spring, Summer, Fall, and Winter, we find Fall has the highest anomalies in the period 2010-2017. For the seasons when this occurred, there was an increase in events during Summer-Fall and a decrease during Winter. For the Summer of Feb (2010), the positive anomaly was four times the average of events. For the Fall of March (2010), the positive irregularity was five times the average.</p></sec><sec id="s6"><title>6. Seasonal Variation for Depths &gt; 200 km</title><p>Figures 8-11 show the seasonal variations for events with depths ≥ 200 km.</p><p>Spring—The enhancement of earthquakes was in Nov (2015), while negative anomalies happened in Nov (1996) and September (2002).</p><p>Summer—Positive anomalies occurred in Feb (2010). Negative variances were more frequent and happened in Feb (2002, 2004), Jan (2003), and Dec (2009).</p><p>Fall—Positive anomalies happened in May (2008) and April (2015). Negative anomalies occurred in Mar (1997), Mar and Apr (2003), and Apr (2009). Any increase in earthquakes during this season was smooth.</p><p>Winter—There were the highest positive disturbance in 2000 (Jun), and negative in 2016 (2016). During the winter, June, July and August all the positive tremors anomalies were below two, in the period searched.</p>Discussions on Seasons for Depths &gt; 200 km<p>Comparing the datasets for Spring, Summer, Fall, and Winter for depths &gt; 200 km, we find an increase below three, for any season. There were two exceptions during Spring and Summer during Nov (2015) and Feb (2010).</p><p>For the Fall and Winter, the earthquakes did not reach an increase above two. However, Fall, for this depth, presented four negative anomalies; these variations occurred for the years of minima in 1997, 2003, and 2009. This was similar to Summer, but different years, 2002 and 2009. Overall, the investigation of the activity pointed out that the period 2000 to 2009 had significance for number variation in the plots.</p></sec><sec id="s7"><title>7. Conclusion</title><p>Our research follows the evolution of earthquakes during two Solar Cycles (23 and 24). We found that the Solar Minima was the period when earthquakes presented more variations between 2002 and 2010. The same search for the seasons pointed out that the seasons with more occurrences of earthquakes are Summer and Fall. Some of the data available for the deepest earthquakes also pointed to an uneven lithosphere as what makes the phenomena not well related to the Solar Cycles for those found to all depths. Overall, the South America Anomaly region does not present as many events as other locations around the Ring of Fire in the Pacific.</p></sec><sec id="s8"><title>Acknowledgements</title><p>I am grateful to the anonymous publishing supervisor who made valuable suggestions to this paper.</p></sec><sec id="s9"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s10"><title>Cite this paper</title><p>Hagen, M. and Azevedo, A. (2020) South Atlantic Anomaly Seasonal Seismicity during Two Solar Cycles. Open Journal of Earthquake Research, 9, 307-322. https://doi.org/10.4236/ojer.2020.94018</p></sec></body><back><ref-list><title>References</title><ref id="scirp.101827-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hudson, M.K., et al. (2008) Relationship of Van Allen Radiation Belts to Solar Wind Drivers. Journal of Atmospheric and Solar-Terrestrial Physics, 70, 708-729. https://doi.org/10.1016/j.jastp.2007.11.003</mixed-citation></ref><ref id="scirp.101827-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Nasuddin, K.A., et al. (2019) Characterization of the South Atlantic Anomaly. Nonlinear Processes Geophys, 26, 25-35. https://doi.org/10.5194/npg-26-25-2019</mixed-citation></ref><ref id="scirp.101827-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Aisikinen, T. and Mursula, K. 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