<?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">IJAA</journal-id><journal-title-group><journal-title>International Journal of Astronomy and Astrophysics</journal-title></journal-title-group><issn pub-type="epub">2161-4717</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijaa.2014.44059</article-id><article-id pub-id-type="publisher-id">IJAA-52410</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Radio Signatures of Sunspot NOAA 12192
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>inttu</surname><given-names>Uunila</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Juha</surname><given-names>Kallunki</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Metsahovi Radio Observatory, Aalto University, Kylmala, Finland</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>minttu.uunila@aalto.fi(IU)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>18</day><month>11</month><year>2014</year></pub-date><volume>04</volume><issue>04</issue><fpage>649</fpage><lpage>655</lpage><history><date date-type="received"><day>27</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>25</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>20</day>	<month>November</month>	<year>2014</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>
 
 
  In this paper, we present an overview of radio signatures of sunspot NOAA 12192 measured with various instruments with frequencies of 37 GHz, 11.2 GHz and 200 - 400 MHz at Aalto University Metsahovi Radio Observatory (MRO). The data were observed during October 20 - 29, 2014. In total, 12 solar radio bursts at 11.2 GHz and 8 at 200 - 400 MHz, with varying intensities and properties, were observed. Radio brightening was captured in several solar radio maps. NOAA 12192 is the largest observed sunspot during solar cycle 24. We show that this exceptional radio brightening belongs to the strongest category including less than 5% of radio brightenings ever measured at MRO.
 
</p></abstract><kwd-group><kwd>Solar Activity</kwd><kwd> Solar Flare</kwd><kwd> Solar Cycle</kwd><kwd> Solar Radio Burst</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Sunspot NOAA 12192, <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>, was both active and visible during October 20 - 29, 2014. It is the largest sunspot, with a diameter &gt; 100,000 km, measured in solar cycle 24 regarding the size of the umbra [<xref ref-type="bibr" rid="scirp.52410-ref1">1</xref>] , [<xref ref-type="bibr" rid="scirp.52410-ref2">2</xref>] , and also the largest one observed in 24 years [<xref ref-type="bibr" rid="scirp.52410-ref3">3</xref>] producing tens of solar events [<xref ref-type="bibr" rid="scirp.52410-ref4">4</xref>] . The high activity and unstability of NOAA 12192 shows that the sunspot has a highly complex magnetic structure. The sunspot, on the right side in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>, shows also various flux structures measured with SDO/HMI magnetogram. The black areas have magnetic fields with negative polarity, and white areas have positive polarity. In typical sunspots, like 2194 in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref> on the right side, there is only one negative and one positive polarity area, and they are clearly separated from each other. In the case of NOAA 12192, marked as 2192 in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>, there are several polarity areas. The negative magnetic field in the <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref> is −2.0 kG, and the positive magnetic field is more than 1.7 kG.</p><p>Large sunspots like NOAA 12192 are not usually observed, because they tend to lose their stability as they grow and change into more complex magnetic structure. They usually disintegrate into smaller sunspots accord-</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref></label><caption><title> NOAA 12192 as seen by SDO AIA 1600 &#197;. <xref ref-type="fig" rid="fig">Figure </xref>on the left is courtesy of NASA, ESA and JAXA. The marked area is &gt; 100 000 km. <xref ref-type="fig" rid="fig">Figure </xref>on the right with photosgraphic magnetic field map is measured by SDO/HMI magnetogram (at 6173 &#197;) on October 26, 2014 at 22:01:59 UT, courtesy of NASA/SDO and the AIA, EVE, and HMI science teams.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x5.png"/></fig><fig id ="fig1_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x6.png"/></fig></fig-group><p>ing to Shallow sunspot model [<xref ref-type="bibr" rid="scirp.52410-ref5">5</xref>] , which is the prevailing sunspot model. 5 Mm is the largest stable sunspot with B<sub>o</sub> ≈ 2.6 - 2.7 kG according to the model. In this article we will show multiple results regarding the sunspot, and the radio flares and and other types of activity it produced, at various radio frequencies measured with MRO radio telescopes. We will compare the results to previous studies presented in [<xref ref-type="bibr" rid="scirp.52410-ref6">6</xref>] and [<xref ref-type="bibr" rid="scirp.52410-ref7">7</xref>] and show that NOAA 12192’s activity was exceptional as it produced several flares during the ten days of its visibility.</p></sec><sec id="s2"><title>2. Instrumentation</title><p>Solar maps at 37 GHz are produced with the 13.7-meter radio telescope, RT-14, which is a cassegain type antenna. RT-14 is located at Mets&#228;hovi Radio Observatory (MRO), Aalto University (Helsinki Region, Finland, GPS: N 60 13.04 E 24 23.35). The radio telescope provides full disk solar mapping, partial solar mapping, and, additionally, the ability to track any selected point on the solar disk. The beam size of the telescope is 2.4 arcmin at 37 GHz. The receiver is a Dicke type radiometer, thus, the radiometer’s own noise will be filtered out. For the temperature stabilization of the receiver, a Peltier element is used. The noise temperature of the 37 GHz receiver is around 280 K, and the temporal resolution during the observations is 0.1 s or less. The radio emission comes from the solar chromosphere (transition region), and is recorded as intensity. More information about the Mets&#228;hovi RT-14 can be found in [<xref ref-type="bibr" rid="scirp.52410-ref7">7</xref>] and [<xref ref-type="bibr" rid="scirp.52410-ref8">8</xref>] .</p><p>Mets&#228;hovi RT-1.8 is a radio telescope with a 1.8 m dish diameter dedicated for continuous solar observations. The telescope has a beam size of 81.6 arc min and its system noise temperature is 270 K. It observes the total radiation of the Sun at a frequency of 11.2 GHz. The emission measured at 11.2 GHz originates from lower corona. The Quiet Sun Level (QSL) is around 12,000 K at 11.2 GHz. The radiotelescope is used for observing solar radio bursts, as it acts as a detector of general solar activity. Also studies on solar oscillations have been done. High sampling rate (5 kHz) enables studying flare fine structure, including short periodic oscillation phenomena. The radio telescope has no protective radome, therefore it is vulnerable to prevailing weather conditions. Around 200 solar radio bursts have been detected since its launch in 2001. Full documentation of the Mets&#228;hovi RT-1.8 can be found in [<xref ref-type="bibr" rid="scirp.52410-ref9">9</xref>] . The telescope has a logarithmic output which can be utilized in the case of strong bursts.</p><p>MRO joined the worldwide solar radio burst observing network, e-Callisto, in the fall of 2010 [<xref ref-type="bibr" rid="scirp.52410-ref10">10</xref>] . The network is coordinated by ETH Z&#252;rich and it consists of 69 instruments in 38 locations all over the world, covering solar radio spectral observations 24 hours a day throughout the year [<xref ref-type="bibr" rid="scirp.52410-ref11">11</xref>] . The network focuses on the decimeter and meter wavelength range. The first radio emission coming from the solar corona observed with the Callisto system was measured on September 24, 2010 [<xref ref-type="bibr" rid="scirp.52410-ref10">10</xref>] . The current frequency coverage in Mets&#228;hovi is 50 - 1450 MHz (the lower band is 50 - 846 MHz and the higher band 790 - 1447.250 MHz). Due to the low instrumental sensitivity studies of the quiet Sun are not possible.</p><p>The changing radio emission indicates variation of solar magnetic activity. The birth of radio emission is affected by all plasma parameters, for example, temperature and density. This signifies the importance of radio observations and introduces interesting information on the subject. Gyromotion of thermal electrons in a presence of a magnetic field causes thermal gyroresonance emission. In active regions the magnetic field may have the strength to render the corona optically thick to enable gyroresonance absorption at the frequency range of 1 - 18 GHz. Plasma emission is the most prevailing emission mechanism in solar flares up to 3 GHz [<xref ref-type="bibr" rid="scirp.52410-ref12">12</xref>] . At mm- wavelengths gyro-resonance emission above the sunspot [<xref ref-type="bibr" rid="scirp.52410-ref13">13</xref>] and free-free radiation from plasma in active region loops are found [<xref ref-type="bibr" rid="scirp.52410-ref14">14</xref>] .</p></sec><sec id="s3"><title>3. Observations</title><sec id="s3_1"><title>3.1. Solar Radio Maps at 37 GHz</title><p>Both variations in brightness and in size of the radio brightening can be derived from the MRO 37 GHz observations. It should be noted, that the radio brightening located at the same location as the sunspot NOAA 12192. The 37 GHz results are described in the two following subsections.</p><sec id="s3_1_1"><title>3.1.1. Variation in Brightness</title><p>Variation in brightness temperature of the radio brightening is listed in the <xref ref-type="table" rid="table1">Table 1</xref>. The largest values are measured on October 26, 2014, when the brightness temperature is close to 200% compared to the Quiet Sun Level (QSL), which is 7800 K. On other days within the duration of the radio brightenings activity the level is between about 120 and 140% compared to QSL.</p></sec><sec id="s3_1_2"><title>3.1.2. Variation in Size</title><p>Four selected solar radio maps during October 20 - 29, 2014 when the NOAA 12192 sunspot was both active and visible, measured at 37 GHz are shown in <xref ref-type="fig" rid="fig">Figure </xref>2. It can clearly be seen that the size of the radio brightenings varies with about the factor of 2.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Brightness temperature, in per cents compared to QSL, of the radio brightening measured at 37 GHz from solar maps. Duration of each solar map scan is 7 min</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Date</th><th align="center" valign="middle" >Start time</th><th align="center" valign="middle" >Temperature</th><th align="center" valign="middle" >Date</th><th align="center" valign="middle" >Start time</th><th align="center" valign="middle" >Temperature</th></tr></thead><tr><td align="center" valign="middle" >20.10.2014</td><td align="center" valign="middle" >09:50:24</td><td align="center" valign="middle" >103.23</td><td align="center" valign="middle" >25.10.2014</td><td align="center" valign="middle" >08:59:51</td><td align="center" valign="middle" >137.69</td></tr><tr><td align="center" valign="middle" >20.10.2014</td><td align="center" valign="middle" >10:00:49</td><td align="center" valign="middle" >124.06</td><td align="center" valign="middle" >25.10.2014</td><td align="center" valign="middle" >09:27:19</td><td align="center" valign="middle" >134.81</td></tr><tr><td align="center" valign="middle" >20.10.2014</td><td align="center" valign="middle" >10:10:48</td><td align="center" valign="middle" >122.55</td><td align="center" valign="middle" >25.10.2014</td><td align="center" valign="middle" >12:16:33</td><td align="center" valign="middle" >125.48</td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >08:40:29</td><td align="center" valign="middle" >119.81</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >10:28:44</td><td align="center" valign="middle" >149.03</td></tr><tr><td align="center" valign="middle" >22.10.2014</td><td align="center" valign="middle" >08:03:19</td><td align="center" valign="middle" >125.37</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >10:59:57</td><td align="center" valign="middle" >199.07</td></tr><tr><td align="center" valign="middle" >22.10.2014</td><td align="center" valign="middle" >08:21:49</td><td align="center" valign="middle" >125.83</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >11:12:50</td><td align="center" valign="middle" >188.81</td></tr><tr><td align="center" valign="middle" >22.10.2014</td><td align="center" valign="middle" >11:10:11</td><td align="center" valign="middle" >122.64</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >11:22:48</td><td align="center" valign="middle" >176.08</td></tr><tr><td align="center" valign="middle" >22.10.2014</td><td align="center" valign="middle" >12:04:49</td><td align="center" valign="middle" >121.93</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >11:32:13</td><td align="center" valign="middle" >174.24</td></tr><tr><td align="center" valign="middle" >23.10.2014</td><td align="center" valign="middle" >10:07:36</td><td align="center" valign="middle" >120.79</td><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >11:49:31</td><td align="center" valign="middle" >188.87</td></tr><tr><td align="center" valign="middle" >23.10.2014</td><td align="center" valign="middle" >10:18:53</td><td align="center" valign="middle" >119.78</td><td align="center" valign="middle" >28.10.2014</td><td align="center" valign="middle" >10:20:27</td><td align="center" valign="middle" >126.04</td></tr><tr><td align="center" valign="middle" >23.10.2014</td><td align="center" valign="middle" >12:22:47</td><td align="center" valign="middle" >118.03</td><td align="center" valign="middle" >28.10.2014</td><td align="center" valign="middle" >10:28:49</td><td align="center" valign="middle" >128.41</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:31:01</td><td align="center" valign="middle" >121.77</td><td align="center" valign="middle" >28.10.2014</td><td align="center" valign="middle" >11:55:21</td><td align="center" valign="middle" >128.06</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:40:02</td><td align="center" valign="middle" >144.28</td><td align="center" valign="middle" >29.10.2014</td><td align="center" valign="middle" >09:16:01</td><td align="center" valign="middle" >128.06</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:50:10</td><td align="center" valign="middle" >145.07</td><td align="center" valign="middle" >29.10.2014</td><td align="center" valign="middle" >09:24:23</td><td align="center" valign="middle" >127.44</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:58:58</td><td align="center" valign="middle" >124.88</td><td align="center" valign="middle" >29.10.2014</td><td align="center" valign="middle" >10:48:32</td><td align="center" valign="middle" >118.22</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >10:43:27</td><td align="center" valign="middle" >124.43</td><td align="center" valign="middle" >29.10.2014</td><td align="center" valign="middle" >10:56:53</td><td align="center" valign="middle" >120.40</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >11:42:48</td><td align="center" valign="middle" >125.62</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><fig-group id="fig2"><label><xref ref-type="fig" rid="fig">Figure </xref>2</label><caption><title> Solar radio maps measured on October 20, 23, 26 and 29, 2014.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x8.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x7.png"/></fig><fig id ="fig2_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x10.png"/></fig><fig id ="fig2_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x9.png"/></fig></fig-group></sec></sec><sec id="s3_2"><title>3.2. Measurements at 11.2 GHz</title><p>We have listed all flares that exceed 100 Solar Flux Units (SFU) in <xref ref-type="table" rid="table2">Table 2</xref>. Peak flux values are estimations with errors approximately &#177;10%. An example of a solar radio burst measured with RT-1.8 on October 24, 2014 is in <xref ref-type="fig" rid="fig">Figure </xref>3. Observed solar radio bursts are associated with certain solar flares listed in <xref ref-type="table" rid="table2">Table 2</xref>. According to [<xref ref-type="bibr" rid="scirp.52410-ref15">15</xref>] about 20% of all X-class flares have strength of X2.0 - X2.9. When we take into account all possible flares, only less than 1% are X-class flares. The strongest of the now observed radio bursts at 2100 SFU is also rare in the long time series measured at MRO [<xref ref-type="bibr" rid="scirp.52410-ref6">6</xref>] . However, the previous time series did not include calibrated flux values.</p></sec><sec id="s3_3"><title>3.3. Measurements with Callisto</title><p>In total, eight type III solar radio bursts listed in <xref ref-type="table" rid="table3">Table 3</xref> were recorded at 200 - 400 MHz band of the e-Callisto. Also some events were recorded at lower frequencies, which are not included in this study. An example of a Callisto recording measured on October 24, 2014 is shown in <xref ref-type="fig" rid="fig">Figure </xref>4. The radio bursts were also observed with several other e-Callisto stations all around the world [<xref ref-type="bibr" rid="scirp.52410-ref11">11</xref>] .</p></sec><sec id="s3_4"><title>3.4. Comparison with Long Time Series Measured at MRO</title><p>In comparison in [<xref ref-type="bibr" rid="scirp.52410-ref6">6</xref>] , for example, in August, 2008, which was the most active month within the time series, 22 solar radio flares were measured. During other months in the time series, from January, 2000 to January, 2014, the number of flares exceeded ten only six times at the integration time of a month. During the ten days in October, 2014, 12 flares were measured at 11.2 GHz.</p><p>We also compared to the long time series study in [<xref ref-type="bibr" rid="scirp.52410-ref7">7</xref>] , which includes data from 1978 to 2011 (solar cycles 21-14). In the study the strongest solar radio brightenings are 145% to QSL (11300 K). During October 26,</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Estimated maximum peak flux values at 11.2 GHz. Total of 12 flares were recorded at 11.2 GHz</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Date</th><th align="center" valign="middle" >Time</th><th align="center" valign="middle" >Estimated peak flux (SFU)</th><th align="center" valign="middle" >Solar flare classification [<xref ref-type="bibr" rid="scirp.52410-ref4">4</xref>]</th></tr></thead><tr><td align="center" valign="middle" >20.10.2014</td><td align="center" valign="middle" >06:36 - 06:48</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >C6.3</td></tr><tr><td align="center" valign="middle" >20.10.2014</td><td align="center" valign="middle" >09:03 - 09:14</td><td align="center" valign="middle" >1600</td><td align="center" valign="middle" >M3.9</td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >10:28 - 10:37</td><td align="center" valign="middle" >180</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >10:48 - 10:50</td><td align="center" valign="middle" >170</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >12:27 - 12:29</td><td align="center" valign="middle" >340</td><td align="center" valign="middle" >C4.4</td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >13:17 - 13:20</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >13:37 - 13:38</td><td align="center" valign="middle" >940</td><td align="center" valign="middle" >M1.2</td></tr><tr><td align="center" valign="middle" >23.10.2014</td><td align="center" valign="middle" >09:44 - 09:52</td><td align="center" valign="middle" >510</td><td align="center" valign="middle" >M1.1</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:40 - 07:46</td><td align="center" valign="middle" >1600</td><td align="center" valign="middle" >M4.0</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >08:02 - 08:03</td><td align="center" valign="middle" >170</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >10:34 - 12:30</td><td align="center" valign="middle" >2100</td><td align="center" valign="middle" >X2.0</td></tr><tr><td align="center" valign="middle" >27.10.2014</td><td align="center" valign="middle" >09:20 - 11:00</td><td align="center" valign="middle" >no calibration available</td><td align="center" valign="middle" >M6.7</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Solar radio bursts, including the burst type, measured with the Callisto system (200 - 400 MHz)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Date</th><th align="center" valign="middle" >Time</th><th align="center" valign="middle" >Type</th></tr></thead><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >10:01:11 - 10:02:13</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >10:48:01 - 10:49:45</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >21.10.2014</td><td align="center" valign="middle" >13:36:02 - 13:37:57</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >23.10.2014</td><td align="center" valign="middle" >11:43:48 - 11:44:00</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >07:39:34 - 07:41:43</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >08:02:04 - 08:04:35</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >24.10.2014</td><td align="center" valign="middle" >10:01:36 - 10:02:05</td><td align="center" valign="middle" >III</td></tr><tr><td align="center" valign="middle" >26.10.2014</td><td align="center" valign="middle" >10:57:37 - 10:58:05</td><td align="center" valign="middle" >III</td></tr></tbody></table></table-wrap><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>3</label><caption><title> Two solar radio bursts on October 24, 2014 were measured at 11.2 GHz. The last wide spike is due to the calibration of the system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x11.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>4</label><caption><title> Type III solar radio burst measured with the Callisto system at 200 - 500 MHz on October 24, 2014. The large horizontal anomaly at about 400 MHz is due to RFI</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-4500381x12.png"/></fig><p>2014 145% QSL limit was exceeded on six occasions, and on its strongest point it reached about 200% QSL. The now recorded radio brightening belongs to the strongest category including less than 5% of radio brightenings ever measured at MRO.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>In this article we have shown a review of radio signatures of NOAA 12192 measured at MRO at various instruments and radio frequencies. The radio brightening is remarkable even when the long time series measured at MRO are considered. The number of flares measured with RT-1.8 was 12 during the active period of the brightening, October 20 - 29, 2014, which makes this brightening one of the most active during the long time series ever measured at MRO. In comparison in [<xref ref-type="bibr" rid="scirp.52410-ref6">6</xref>] , for example, in August, 2008, which was the most active month within the time series, 22 solar radio flares were measured. When the results were compared to the long time series [<xref ref-type="bibr" rid="scirp.52410-ref7">7</xref>] , it can be concluded that the now recorded radio brightening belongs to the strongest category including less than 5% of radio brightenings ever measured at MRO.</p><p>This exceptional sunspot will lead to follow-up studies. For example, several of the events measured at 11.2 GHz revealed interesting double-peak structures. Further studies of the double-peak structures will be conducted by the authors in the near future.</p></sec><sec id="s5"><title>Acknowledgements</title><p>NOAA 12192 image created using the ESA and NASA funded Helioviewer Project.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.52410-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kiess, C., Rezaei, R. and Schmidt, W. (2014) Properties of sunspot umbrae observed in cycle 24. 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