<?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">WJNST</journal-id><journal-title-group><journal-title>World Journal of Nuclear Science and Technology</journal-title></journal-title-group><issn pub-type="epub">2161-6795</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/wjnst.2013.32011</article-id><article-id pub-id-type="publisher-id">WJNST-30801</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Modelling Natural Radioactivity in Sand Beaches of Guarapari, Esp&#237;rito Santo State, Brazil
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>anilo</surname><given-names>C. Vasconcelos</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>Patricia</surname><given-names>A. L. Reis</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>Claubia</surname><given-names>Pereira</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>Arno</surname><given-names>H. Oliveira</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>Talita</surname><given-names>O. Santos</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>Zildete</surname><given-names>Rocha</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Centro de Desenvolvimento da Tecnologia Nuclear/Comiss?o Nacional de Energia Nuclear (CDTN/CNEN), Laboratório de Trítio, Belo Horizonte, Brasil </addr-line></aff><aff id="aff1"><addr-line>Departamento de Engenharia Nuclear, Escola de Engenharia Universidade Federal de Minas Gerais, Belo Horizonte, Brasil</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>claubia@nuclear.ufmg.br(CP)</email>;<email>rochaz@cdtn.br(ZR)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>04</month><year>2013</year></pub-date><volume>03</volume><issue>02</issue><fpage>65</fpage><lpage>71</lpage><history><date date-type="received"><day>December</day>	<month>8,</month>	<year>2012</year></date><date date-type="rev-recd"><day>February</day>	<month>11,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>4,</month>	<year>2013</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>
 
 
   Using gamma-ray spectrometry, the activity concentration of naturally occurring radionuclides <sup>226</sup>Ra, <sup>212</sup>Pb, <sup>214</sup>Pb, <sup>232</sup>Th, and <sup>40</sup>K was determined in sand beaches samples from different areas in Guarapari, Esp&#237;rito Santo state, from Brazil. The absorbed dose rates and annual effective dose were calculated and the results were compared with the internationally accepted values as well as others high background radiation areas (HBRAs). The activity concentration of the <sup>232</sup>Th in Areia Preta as well as the absorbed dose rates and annual effective dose were higher than the others regions compared. The results show that Areia Preta in Guarapari has higher background found in beaches in world. This work is part of a research project for the natural background determination of the Brazilian coast.  
    
 
</p></abstract><kwd-group><kwd>Gamma-Ray Spectrometry; Beach Sand; Guarapari</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>People are exposed to ionizing radiation from naturally occurring radionuclides that there are in the earth’s environmental. Radionuclides in soils, belonging to <sup>232</sup>Th, <sup>235</sup>U and <sup>238</sup>U series as well as radioisotope of potassium (<sup>40</sup>K) are the major contributors of outdoor terrestrial natural radiation [<xref ref-type="bibr" rid="scirp.30801-ref1">1</xref>]. These radionuclides are not uniformly distributed, their concentration depends upon the local geology of each region in the world [<xref ref-type="bibr" rid="scirp.30801-ref2">2</xref>]. Although their presence result in a relatively small amount of radiation dose, in some regions known for high background radiation levels (HBRA) [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>], the knowledge of their distribution in soil, sand and rock plays an important role in radiation protection and measurement [<xref ref-type="bibr" rid="scirp.30801-ref2">2</xref>]. Ramsar, Iran [<xref ref-type="bibr" rid="scirp.30801-ref4">4</xref>], due to the concentration of <sup>226</sup>Ra and daughters which are brought to Earth’s surface by hot springs, and Orissa and Kerala, India [<xref ref-type="bibr" rid="scirp.30801-ref5">5</xref>], due to the monazite sands, are examples of HBRA. In certain beaches of Brazil, there are areas known for their high background radiation, which geological and geochemical characteristics increase the levels of natural radiation [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>]. Monazite sand is the main source of the high background from Atlantic coast from Brazil and it contributes to increase the environmental dose. The more important area begins below Guarapari, Esp&#237;rito Santo, going up Porto Seguro, Bahia (<xref ref-type="fig" rid="fig1">Figure 1</xref>), and it is formed by pre-Cambrian rocks and Tertiary and Quarternary deposits. In 2009, the Departamento de Engenharia Nuclear (DEN)/Universidade Federal de Minas Gerais (UFMG) and Centro de Desenvolvimento da Tecnologia Nuclear (CDTN)/Comiss&#227;o Nacional de Energia Nuclear (CNEN) began a research to determine reference levels of this region using gamma spectrometry. The first part of this research analysed beach sands from the extreme south of Bahia state, between Porto Seguro and Caravelas (<xref ref-type="fig" rid="fig1">Figure 1</xref>) [<xref ref-type="bibr" rid="scirp.30801-ref6">6</xref>]. The results showed Cumuruxatiba as HBRA region. Continuing in the south direction, Guarapari is a region cited by some studies [2,7,8] by its high environmental radiation. In this work, the same methodology as used in Cumuruxatiba was applied to evaluate the Guarapari area. The gamma-ray activity of radioisotopes such as <sup>232</sup>Th, <sup>226</sup>Ra, and<sup> 40</sup>K, in beach sand samples from Guarapari was measured and the absorbed dose rate and the effective dose rates were calculated and compared with internationally accepted values as well as others HBRAs. The goal is validate the measurement methodology comparing the results obtained in this work with data referenced</p><p>in some studies.</p></sec><sec id="s2"><title>2. Material and Methods</title><p>Beach sand samples were collected in Areia Preta, Praia do Morro and Setiba in Guarapari city, Esp&#237;rito Santo state, in January 2010. The samples were collected from about 10 cm deep. Each sample was collected from an area corresponding to 1 m<sup>2</sup> and were homogenized in situ. This sand mixture, weighing approximately 1.5 kg, was considered representative of the profile, as done by [<xref ref-type="bibr" rid="scirp.30801-ref9">9</xref>]. For each local, twelve samples have been measured. The samples were dried for about 48 hours in an oven at 60˚C. The analytical technique used for the gamma emitters isotopes <sup>214</sup>Bi (<sup>226</sup>Ra), <sup>228</sup>Ac (<sup>232</sup>Th) and <sup>40</sup>K was gammaray spectrometry. <xref ref-type="table" rid="table1">Table 1</xref> shows the radionuclides, the specific gamma-ray line used and the detection limits that were calculated according to procedures and experimental conditions [<xref ref-type="bibr" rid="scirp.30801-ref10">10</xref>].</p><sec id="s2_1"><title>2.1. Gamma-Ray Spectrometry</title><p>The specific activities of the radionuclides <sup>226</sup>Ra and <sup>40</sup>K in the collected samples are determined in a specially reduced background detection system, consisting of a hyper-pure germanium detector (HPGe), coaxial geometry, 15% relative efficiency. The data are treated with Genie 2000 software. The efficiency and energy curves for calibrations are determined using internationally certificate standard solution prepared by PNI/IRD/CDTN (Programa Nacional de Intercompara&#231;&#227;o/Instituto de Radioprote&#231;&#227;o e Dosimetria/Centro de Desenvolvimento da Tecnologia Nuclear). The samples, after being dried and weighed, are transferred to Marinelli beakers (500 mL). Each sample is hermetically and carefully sealed to prevent the escape of gaseous <sup>222</sup>Rn and <sup>220</sup>Rn. It is kept aside for 30 days to reach radioactive equilibrium of the <sup>226</sup>Ra between <sup>214</sup>Pb and <sup>214</sup>Bi radon’s daughters. In <sup>232</sup>Th decay chain the radioactive equilibrium of <sup>232</sup>Th between <sup>228</sup>Ra and <sup>212</sup>Pb is easily reached due the short half-life of</p><p><xref ref-type="table" rid="table1">Table 1</xref>. Gamma-ray lines and detection limits for the radionuclides.</p><disp-formula id="scirp.30801-formula104557"><graphic  xlink:href="5-1090103\ef65dcb7-b1fb-48b8-857e-ceef1786239a.jpg"  xlink:type="simple"/></disp-formula><p><sup>a</sup>The detection limit is given by the equation LD = 2.71 + 4.65δ for 95% confidence limit, where δ is the standard deviation of the background in the peak interval; <sup>b</sup>The gamma-ray lines represent <sup>226</sup>Ra, <sup>212</sup>Pb and <sup>232</sup>Th were determined indirectly by <sup>214</sup>Bi, <sup>224</sup>Ra and <sup>228</sup>Ac respectively.</p><p>the decay products of <sup>228</sup>Th. In environment, <sup>226</sup>Ra is in equilibrium with <sup>238</sup>U and <sup>228</sup>Ra is in equilibrium with <sup>232</sup>Th only if no occur leaching <sup>226</sup>Ra, <sup>228</sup>Ra and its parents. After, all samples are submitted to gamma-ray spectrometry. The samples are counted for 24 hours in order to obtain statistically small uncertainty for the gamma-ray peak of interest.</p><p>Following the spectrum analysis, count rates for each detected photo peak and activity concentration in units of Becquerel per kilogram for each nuclide are calculated based on the Equation (1):</p><disp-formula id="scirp.30801-formula104558"><label>(1)</label><graphic position="anchor" xlink:href="5-1090103\b1232d7a-b1ae-4684-8392-bc092b19d848.jpg"  xlink:type="simple"/></disp-formula><p>where N<sub>Ei</sub> is the net peak area at energy E<sub>i</sub> of radionuclide i; t the counting time in seconds; m is the mass of samples in kg;&#160;ɛ<sub>Ei</sub> and γ<sub>Ei</sub> are detection efficiency and emission probability of gamma-ray, respectively.</p></sec><sec id="s2_2"><title>2.2. Calibration</title><p>Energy calibration was performed in the energy range using point sources from 0.1 to 2 MeV made by Institute of Isotopes Co., Ltd., Budapest, Hungary. The following photon emissions and radionuclides were used: <sup>241</sup>Am, <sup>133</sup>Ba, <sup>152</sup>Eu, <sup>109</sup>Cd and <sup>60</sup>Co. The efficiency calibration curve, showed in <xref ref-type="fig" rid="fig2">Figure 2</xref>, was determined using a standard solution made by the National Institute of Standards and Technology (NIST) and reference materials with densities and compositions similar to the samples that will be measured after pulverization. Marinelli beakers of 500 mL were also used for the reference materials. Each sand sample, of approximately 1.0 kg, was counted for 86,400 s. All samples were measured in a low background spectrometry system inside a special counting room, shielded by water all around, over and below. The background spectrum collected from the standard solution for 24 hours is show in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p></sec><sec id="s2_3"><title>2.3. Dose Calculation</title><p>The total air absorbed dose rate (nGy&#183;h<sup>−1</sup>) 1 m above the ground due to the specific activities of <sup>226</sup>Ra, <sup>232</sup>Th and <sup>40</sup>K (Bq&#183;kg<sup>−1</sup>) was calculated using the Equation (2) [2,3]</p><disp-formula id="scirp.30801-formula104559"><label>(2)</label><graphic position="anchor" xlink:href="5-1090103\cb259390-2de7-4baf-b555-e508ffd86b47.jpg"  xlink:type="simple"/></disp-formula><p>where D is the absorbed dose rate, A<sub>K</sub>, A<sub>Ra</sub> and A<sub>Th</sub> are the activity concentrations for <sup>40</sup>K, <sup>226</sup>Ra and <sup>232</sup>Th respectively.</p><p>To estimate the annual effective dose rates, the conversion coefficient from absorbed dose in air to effective dose (0.7 Sv&#183;Gy<sup>−1</sup>) and outdoor occupancy factor (0.2) proposed by [<xref ref-type="bibr" rid="scirp.30801-ref10">10</xref>] were used. The effective dose rate in units of mSv&#183;y<sup>−1</sup> was calculated by following Equation (3):</p><disp-formula id="scirp.30801-formula104560"><label>. (3)</label><graphic position="anchor" xlink:href="5-1090103\93b46cce-140e-4c77-9a93-05edba1cdbc2.jpg"  xlink:type="simple"/></disp-formula><p>where D is the calculated dose rate (in nGy&#183;h<sup>−1</sup>), T is the outdoor occupancy time (24 h &#215; 365.25 days &#215; 0.2 = 1753 h&#183;y<sup>−1</sup>), and F is the conversion factor (0.7 Sv&#183;Gy<sup>−1</sup>).</p></sec></sec><sec id="s3"><title>3. Results and Discussions</title><p>The activity concentrations of radionuclides measured in beach sand samples from Guarapari, Brazil are presented in <xref ref-type="table" rid="table2">Table 2</xref>. The naturally occurring <sup>226</sup>Ra, <sup>214</sup>Pb, <sup>232</sup>Th, <sup>212</sup>Pb and <sup>40</sup>K in beach sands ranged from 6.0 to 4100, 6.0 to 3600, 20 to 57,000, 17 to 47,500 and 73 to 3000 Bq&#183;kg<sup>−1</sup> respectively. All radionuclides found in these beaches sand samples are radioisotopes from the uranium, thorium and actinium decay series plus the <sup>40</sup>K. The radioisotopes <sup>226</sup>Ra, <sup>214</sup>Pb and <sup>212</sup>Pb are the daughter products of the <sup>232</sup>Th and <sup>238</sup>U decay series.</p><p>As shows in <xref ref-type="table" rid="table2">Table 2</xref>, determination of the activity of some <sup>238</sup>U and <sup>232</sup>Th decay products shows that radionuclides are in secular equilibrium. For example, the value for <sup>214</sup>Pb activity (end of the <sup>238</sup>U decay chain) is equal to the <sup>226</sup>Ra activity (beginning in the decay chain). Thus, these data do not show any evidence of disequilibrium between radionuclide activities. The values of <sup>226</sup>Ra, <sup>232</sup>Th and <sup>40</sup>K in Areia Preta are higher than the range of the corresponding typical world values. However, the values of radionuclides in Praia do Morro and Setiba are lower than the range of the corresponding typical world values. The determination of <sup>232</sup>Th/<sup>238</sup>U and <sup>238</sup>U/<sup>214</sup>Pb ratios is pertinent in understanding the status of secular equilibrium. If <sup>226</sup>Ra, or daughters, are in secular equilibrium with <sup>238</sup>U, their activity ratios and of their daughters, would be equal to unity [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>]. According to [<xref ref-type="bibr" rid="scirp.30801-ref15">15</xref>], the analysis of the naturally occurring radioactive materials (NORM) relative abundance (Th/U, K/U and K/Th ratios) may give information on the enrichment/depletion processes as a result of the complex metamorphic history, alteration and/or weathering, which affected the investigated rocks. The <sup>232</sup>Th/<sup>238</sup>U ratio calculated in Areia Preta was of 13.9. This value shows that there is much more <sup>232</sup>Th in samples compared to <sup>238</sup>U and it is much higher than the continental crustal average concentration of 3.82 reported by [<xref ref-type="bibr" rid="scirp.30801-ref16">16</xref>]. The <sup>40</sup>K/<sup>238</sup>U and <sup>40</sup>K/<sup>232</sup>Th ratios are 0.73 and 0.05 respectively, but it must be highlighted that these values are highly variables. The <sup>226</sup>Ra/ <sup>214</sup>Pb ratio calculated was of 1.1. This ratio shows a radioactive equilibrium. <xref ref-type="fig" rid="fig4">Figure 4</xref> shows an acceptably correlation between activity concentration of <sup>238</sup>U (<sup>226</sup>Ra) and <sup>232</sup>Th in the beach sand samples from Areia Preta, with a linear coefficient of 0.821.</p><p><xref ref-type="table" rid="table3">Table 3</xref> shows the results of the total absorbed dose rate in the air due to gamma-ray radiation (D) and the outdoor annual effective dose rate (H<sub>E</sub>) assessment for beach sand samples.</p><p>As can be observed in <xref ref-type="table" rid="table3">Table 3</xref>, only the values of the absorbed dose rates in Areia Preta are higher than the estimate of average global primordial radiation of 59 nGy&#183;h<sup>−1 </sup>and the world range (10 - 200 nGy&#183;h<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>]. The results show that the absorbed dose rates range from 18 - 37,500 nGy&#183;h<sup>−1</sup>. The largest contribution from natural radionuclides in Areia Preta to the absorbed dose rate in air is due to <sup>232</sup>Th, about 94.7% and <sup>226</sup>Ra contributes about 5%. The contribution of <sup>40</sup>K is negligible. Adopting the conversion factor that converts the absorbed dose rate in air to human effective dose equivalent, an outdoor occupancy factor which is the fraction of time spent outdoors as recommended by [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>], and the mean value of absorbed dose rate obtained in the present study, the average annual outdoor effective dose is computed to be 43.00 in Areia Preta. This value is much greater than the world average value assessed by [<xref ref-type="bibr" rid="scirp.30801-ref3">3</xref>]. Presence of mineral monazite is the cause of the high dose. Monazite is a monoclinic mineral consisting of 70% of rare earths phosphates; thorium oxide 4% - 6% and uranium oxide 0.15% - 0.25% [<xref ref-type="bibr" rid="scirp.30801-ref7">7</xref>]. The ilmenite and monazite rich sands of Guarapari have attracted tourists because of their supposed therapeutic properties.</p><p><xref ref-type="table" rid="table4">Table 4</xref> shows the activity concentrations of the <sup>226</sup>Ra, <sup>232</sup>Th and <sup>40</sup>K measure in some works in Areia Preta beach from Guarapari, Brazil. The region already is well studied, therefore is an ideal local for comparison of the measures. Our measurements of <sup>226</sup>Ra and <sup>232</sup>Th from Areia Preta agree with the values measured by [<xref ref-type="bibr" rid="scirp.30801-ref2">2</xref>], al-</p><p><xref ref-type="table" rid="table2">Table 2</xref>. Concentration of radionuclides in beach sand samples.</p><p><xref ref-type="table" rid="table3">Table 3</xref>. Average total absorbed dose rate in air from natural radionuclides <sup>226</sup>Ra, <sup>232</sup>Th and <sup>40</sup>K and annual effective dose in beach sands of Guarapari.</p><disp-formula id="scirp.30801-formula104561"><graphic  xlink:href="5-1090103\0b3af428-ac6f-4fff-bcd8-53e9f812e22a.jpg"  xlink:type="simple"/></disp-formula><p><sup>a</sup>Values higher than the world range (10 - 200 nGy&#183;h<sup>−1</sup>); <sup>b</sup>Values higher than worldwide average (0.07 mSv&#183;y<sup>−1</sup>).</p><p>though the value of <sup>40</sup>K is disagreement. This is expected because there are variations in environment potassium due to the variation of the organic matter. Works of more 10 years ago have lower values for <sup>226</sup>Ra and <sup>232</sup>Th than the recent works.</p><p>In <xref ref-type="table" rid="table5">Table 5</xref>, a summary of results on natural gammaray radioactivity levels derived from similar investigation conducted in some of world regions and around the Atlantic coast of Brazil is presented. Activity concentrations of <sup>226</sup>Ra (<sup>238</sup>U daughter) from Cumuruxatiba, Bahia state, is higher than the others locals showed in the summary. According to [<xref ref-type="bibr" rid="scirp.30801-ref6">6</xref>], Cumuruxatiba is a place which has a large amount of monazite sand (4500 t) and indicates that the monazite deposit in Cumuruxatiba is more extensive than Guarapari. However, the highest activity concentration of <sup>232</sup>Th was found in Guarapari. On the</p><p><xref ref-type="table" rid="table4">Table 4</xref>. Comparison of the activity concentrations of the main radionuclides gamma-ray emitter measure in some works in Areia Preta beach, Guarapari, Brazil.</p><p><img src="5-1090103\071720b2-5cde-49f5-9c69-c9652a29583a.jpg" /></p><p><xref ref-type="table" rid="table5">Table 5</xref>. Summary of activity concentrations and dose rates of natural radioisotopes in soil and sand samples in some of the world regions; (-) not determined.</p><disp-formula id="scirp.30801-formula104562"><graphic  xlink:href="5-1090103\ad0bfc7e-bdc6-4ce0-ac4f-7b9631cebed2.jpg"  xlink:type="simple"/></disp-formula><p><sup>*</sup>Maximum value.</p><p>other hand, <sup>238</sup>U concentration is highest in Cumuruxatiba. The activity concentration of <sup>40</sup>K from Cumuruxatiba is higher than the others regions and slightly higher than Guarapari. Values of total air absorbed dose rate (D) and annual effective dose (H<sub>E</sub>) from Guarapari are very higher than the values from Orissa, India [<xref ref-type="bibr" rid="scirp.30801-ref5">5</xref>] and Cumuruxatiba, Brazil [<xref ref-type="bibr" rid="scirp.30801-ref6">6</xref>]. Orissa and Cumuruxatiba are HBRAs.</p></sec><sec id="s4"><title>4. Conclusion</title><p>The exposure level due to monazite sand radiation in Areia Preta beach, Guarapari, is high. The activity concentration of <sup>232</sup>Th in Areia Preta is higher than others beaches in world studied and others regions from coast Brazilian such as Cumuruxatiba and Porto Seguro although the activity concentration of <sup>238</sup>U is lower than Cumuruxatiba. The values of the absorbed dose rate in air and outdoor annual effective dose rate in Areia Preta beach are higher than the world averages due the content of <sup>232</sup>Th. Areia Preta has the highest background found in beaches in world and beside Cumuruxatiba are highest background from coast Brazilian with values much higher than worldwide average. The measured values in Areia Preta agree with values found by others studies which validate our methodology.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>The authors thank to the Centro de Desenvolvimento da Tecnologia Nuclear—CDTN/CNEN, where this study was carried out. The authors also are grateful to FAPEMIG, CNPq and CAPES for financial assistance.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.30801-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">F. S. Erees, S. Akozcan, Y. Parlak and S. Cam, “Assessment of Dose Rates around Manisa (Turkey),” Radiation Measurements, Vol. 41, No. 5, 2006, pp. 598-601.  
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