<?xml version="1.0" encoding="utf-8"?>
<journal>
<title>International Journal of Radiation Research</title>
<title_fa>نشریه پرتو پژوه</title_fa>
<short_title>Int J Radiat Res</short_title>
<subject>Basic Sciences</subject>
<web_url>http://ijrr.com</web_url>
<journal_hbi_system_id>79</journal_hbi_system_id>
<journal_hbi_system_user>journal79</journal_hbi_system_user>
<journal_id_issn>2322-3243</journal_id_issn>
<journal_id_issn_online>2345-4229</journal_id_issn_online>
<journal_id_pii></journal_id_pii>
<journal_id_doi>10.61882/ijrr</journal_id_doi>
<journal_id_iranmedex></journal_id_iranmedex>
<journal_id_magiran></journal_id_magiran>
<journal_id_sid></journal_id_sid>
<journal_id_nlai></journal_id_nlai>
<journal_id_science></journal_id_science>
<language>en</language>
<pubdate>
	<type>jalali</type>
	<year>1383</year>
	<month>12</month>
	<day>1</day>
</pubdate>
<pubdate>
	<type>gregorian</type>
	<year>2005</year>
	<month>3</month>
	<day>1</day>
</pubdate>
<volume>2</volume>
<number>4</number>
<publish_type>online</publish_type>
<publish_edition>1</publish_edition>
<article_type>fulltext</article_type>
<articleset>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>In memory of Professor John R. Cameron (1922-2005) </title>
	<subject_fa>Nuclear Medicine</subject_fa>
	<subject>Nuclear Medicine</subject>
	<content_type_fa>اخبار و تازه‌ها</content_type_fa>
	<content_type>News and Features</content_type>
	<abstract_fa></abstract_fa>
	<abstract></abstract>
	<keyword_fa></keyword_fa>
	<keyword></keyword>
	<start_page>165</start_page>
	<end_page>166</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-81&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>Prof. A. Niroomand-Rad</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>nirooma@gunet.georgetwn.edu</email>
	<code>79003194753284600197</code>
	<orcid>79003194753284600197</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Grid: A location dependent intensity modulated radiotherapy 
for bulky tumors </title>
	<subject_fa>Radiation Oncology</subject_fa>
	<subject>Radiation Oncology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;p&gt;&lt;strong&gt;Background:&lt;/strong&gt; &lt;/p&gt;&lt;p&gt;An effective method for management of large and bulky malignant tumors. This treatment modality is also known as Specially Fractionated Radiation Therapy (SFRT). In this treatment technique a grid block converted the open radiation field into a series of pencil beams. Dosimetric characteristics of an external beam grid radiation field have been investigated using experimental and Monte Carlo simulation technique.&lt;/p&gt;&lt;p&gt;Grid radiation therapy, using the megavoltage X-ray beam, has been proven to be&lt;/p&gt;&lt;p&gt;Materials and Methods: &lt;/p&gt;&lt;p&gt;radiation field have been determined using experimental and Monte Carlo simulation technique, for 6- and 18 MV X-ray beams from a Varian Clinics 2100C/D. The measurements were performed using LiF TLD and film in Solid Water phantom Material. Moreover, the MCNP Monte Carlo code was utilized to calculate the dose distribution in the grid radiation field in the same phantom material. The results of the experimental data were compared to the theoretical values, to validate this technique. Upon the agreement between the two techniques, dose distributions can be calculated for the grid field with different patterns and sizes of holes, in order to find an optimal design of the grid block.&lt;/p&gt;&lt;p&gt;Dose distributions (%DD as well as the beam profiles) of a grid &lt;/p&gt;&lt;p&gt;&lt;strong&gt;Results:&lt;/strong&gt; &lt;/p&gt;&lt;p&gt;simulation technique was in good agreement with the measured data. In addition, the 3D dose distribution of the grid field generated by the Monte Carlo simulation gave more detailed information about the dose pattern of the grid.&lt;/p&gt;&lt;p&gt;The results of dose profiles for 6 MV X-ray beams obtained with the Monte Carlo &lt;/p&gt;&lt;p&gt;&lt;strong&gt;Conclusion:&lt;/strong&gt; &lt;/p&gt;&lt;p&gt;Carlo simulation technique can be utilized to optimize the pattern, size and spacing between the holes, for optimal clinical results. &lt;/p&gt;&lt;p&gt;The grid block can be used as a boost for treatment of bulky tumors. The MonteIran. J. Radiat. Res., 2005 2 (4): 167-174&lt;/p&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,specially fractionated radiation therapy,bulky tumors,Grid</keyword>
	<start_page>167</start_page>
	<end_page>174</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-82&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>A.S. Meigooni</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>alimeig@uky.edu</email>
	<code>79003194753284600229</code>
	<orcid>79003194753284600229</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>U. Malik</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600230</code>
	<orcid>79003194753284600230</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>H. Zhang</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600231</code>
	<orcid>79003194753284600231</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>S.A. Dini</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600232</code>
	<orcid>79003194753284600232</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>N. J. Meigooni</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600233</code>
	<orcid>79003194753284600233</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>K. Komanduri</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600234</code>
	<orcid>79003194753284600234</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Mohiuddin</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600235</code>
	<orcid>79003194753284600235</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>The physical characteristics of a SLIC-EPID for transmitted dosimetry  </title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;p align=&quot;left&quot; &gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;for treatment verification in radiation therapy. Several physical characteristics of Scanning&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Liquid filled Ionization Chamber EPID (SLIC-EPID) including: extra build-up layer,&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;reproducibility and uniformity, and noise level were investigated.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Electronic Portal Imaging Devices (EPIDs) have found an outstanding position&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;equilibrium, 1-30 mm white water materials (RW3) were placed on the EPID cover and the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;variation of pixel values were investigated. To assess the short term reproducibility, a series of&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;10 consecutive Electronic Portal Images (EPIs) were acquired. The variation of pixel values&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;were then determined in irradiated field using MATLAB software. For long term reproducibility,&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;the described above experiment was then repeated seven times. To determine the noise level&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;in EPID images, 10 consecutive flood images were acquired. The measurement was repeated&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;after two days during a fortnight.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;To determine the extra build-up layer to reach the electronic&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;No significant variation was observed between the maximum thickness of build-up layer&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;required for the central axis and peripheral points. For reproducibility measurements, no systematic&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;variation was observed between mean, maximum and minimum acquired pixel values.&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Both the long-term and short term reproducibility was found to be less than 1%. The noise level&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;was generally less than 1% and this can be referred as an acceptable dose level&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;5 mm of RW3 material was found to increase the pixel values to the maximum possible.&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;.&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion:&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;can be used for dosimetry. However, for a particular linac energy and EPID image acquisition&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;mode, the extra build-up layer thickness must be known for the EPID to be used for dosimetric&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;purposes&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The physical characteristics, measured in this work, suggest that the SLIC-EPID&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;. Iran. J. Radiat. Res., 2005 2 (4): 175-183&lt;/font&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,transmitted dosimetry,portal dosimetry,physical characteristics,SLIC-EPID</keyword>
	<start_page>175</start_page>
	<end_page>183</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-83&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Mohammadi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>Mahamma@mail.rah.sa.gov.au</email>
	<code>79003194753284600205</code>
	<orcid>79003194753284600205</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>E. Bezak</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600206</code>
	<orcid>79003194753284600206</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Estimation of the effective dose to the radiologists during fluoroscopy
or angiography of abdominal viscera</title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;as fluoroscopy or different angiographies are usually evaluated using TL dosimeter. This&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;method is a time-consuming procedure therefore, radiologists are usually worried and unaware&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;of their exact radiation dose received during each fluoroscopy or angiography. In this study, a&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;new trend for quick estimation of effective dose based on measuring air-absorbed dose of the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;scattered radiations at body surface of the radiologists has been introduced.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The radiation effective dose received by the radiologists during procedures such&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;fluoroscopy unit (Shimatsu, model SF5010MD), and a water phantom (spherical plastic bag 27&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;cm in diameter filled with water up to 22.5 cm height). Radiation field was 20 × 20 cm on the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;bed and X-ray tube had 1.5 and 2 mm of Aluminum as an internal and external filtration&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;respectively. A calibrated survey meter model RDS-110 was used to measure the scattered&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;radiation horizontally and vertically around the phantom at different angles and distances, in&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;front and behind of an apron.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Scattered radiations of abdominal viscera were simulated by a&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;mA, was 451 µGy/h. This value reduced to 4.45 µGy/h by passing through lead ribbons of&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;serigraph and to 1.2 µSv/h behind an apron. The scattered dose rate at different angles above the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;bed was constant and varied by distance from the center of the radiation field. The effective&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;dose received by the radiologist is estimated to be about 174µGy/h, while wearing an apron and&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;staying 50 cm away from the patient during fluoroscopy or angiography of abdominal viscera.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The scattered dose rate at 1 m from the phantom, during fluoroscopy at 83 kVp and 1.7&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt; &lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;different angiographies of abdominal viscera, by determining scatter radiation dose at their body&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;surface and applying factor 0.87 for shielding effect of the body. Equivalent organ dose can also&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;be calculated from dose rate in air after applying factor 0.87 for deep organs or 1.1 (the mass&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;energy absorption coefficient ratio of water/tissue to air) for organs near the surface. &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Radiat. Res., 2005 2 (4): 185-190&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The radiologist can estimate his/her effective dose following a fluoroscopy or&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. &lt;/font&gt;&lt;/i&gt;&lt;/b&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,angiography, fluoroscopy, radiologist,Effective dose, phantom</keyword>
	<start_page>185</start_page>
	<end_page>190</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-84&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Hajizadeh Saffar</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email> hajizadeh@mums.ac.ir</email>
	<code>79003194753284600207</code>
	<orcid>79003194753284600207</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>S. Nekoee</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600208</code>
	<orcid>79003194753284600208</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M.H. Bahrayni-Toosi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600209</code>
	<orcid>79003194753284600209</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>A. Sedghi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600210</code>
	<orcid>79003194753284600210</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Comparison of MCNP4C, 4B and 4A Monte Carlo codes when 
calculating electron therapy depth doses </title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;1&quot;&gt;&lt;p align=&quot;left&quot; &gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;accurate methods of radiation therapy dose calculation. There are different Monte Carlo codes&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;for simulation of photons, electrons and the coupled transport of electrons and photons. MCNP&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;is a general purpose Monte Carlo code that can be used for electron, photon and coupled&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;photon-electron transport.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Monte Carlo simulation of radiation transport is considered to be one of the most&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;calculating electron beam doses in water. For simulating, the geometry and other parameters&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;were the same for three codes. By choosing two energy indexing algorithm (ITS &amp; MCNP),&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;absorbed doses were scored in water. 10&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;In this study the MCNP4A, 4B and 4C have been compared when&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;6 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Particles were followed in these three cases.&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;used in 4B and 4C versions. There was a good agreement between versions 4B and 4C. For the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;energy spectrum, there were significant differences between these three versions in two planes.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;MCNP4C and 4B gave different results compared to 4A when the ITS algorithm was&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;for electron transport and also requires a shorter time than the two previous versions. These&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;results, in addition to the practical measurements acquired with MCNP4B by other investigators,&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;suggest that in electron transport the user should use the ITS indexing energy&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;algorithm. &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Because of new improvements in electron transport in 4C, this version is reliable&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. Radiat. Res., 2005 2 (4): 191-195&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,BoldItalic&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Keywords:&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt; Radiotherapy, electron therapy, Monte Carlo, absorbed dose, energy spe&lt;/font&gt;&lt;/b&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,absorbed dose,Monte Carlo, electron therapy, Radiotherapy,energy spectrum</keyword>
	<start_page>191</start_page>
	<end_page>195</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-85&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>H. Nedaie</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>nedaieha@sina.tums.ac.ir</email>
	<code>79003194753284600211</code>
	<orcid>79003194753284600211</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Shariary</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600212</code>
	<orcid>79003194753284600212</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>H. Gharaati</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600213</code>
	<orcid>79003194753284600213</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Allahverdi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600214</code>
	<orcid>79003194753284600214</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M.A. Mosleh-Shirazi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600215</code>
	<orcid>79003194753284600215</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Alpha activity in Indian thermal springs </title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;p align=&quot;left&quot; &gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;and soils with which it comes in contact. There is dual exposure from radon in water i.e. due to&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;inhalation of the radon released from the water into the ambient air and through ingestion when&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;water is used for drinking. As radon contaminated water adversely affects the health, it is&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;therefore fundamental from health and hygiene point of view to measure radium concentration&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;and radon exhalation rates in water.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Dissolved radon is contained in natural water due to primordial uranium in rocks&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;radium concentration and radon exhalation rate in water samples collected from various thermal&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;springs. The alpha tracks registered were counted by optical microscope at suitable magnification&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;and converted into radium concentration and subsequently radon exhalation rates were measured.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;: LR-115, Type- II plastic track detectors were used to measure the&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;m&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;varied from 5.65 Bq l&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;exhalation rates varied from 2.37 mBq kg&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;± 0.36 mBq kg&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The radon concentration emanated from water samples (air borne) varied from 84 Bq&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-3 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;to 827 Bq m&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-3 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;with an average of 429 ± 12.72 Bqm&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-3 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;and the dissolved radon concentration&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;to 55.66 Bq l&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;with an average of 28.88± 0.85 Bq l&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;. The radon mass&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;hr&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;to 23.39 mBq kg&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;hr&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;with an average of 12.14&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;hr&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;and surface exhalation rates from 52.34 mBq m&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-2 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;hr&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;to 515.29 mBq m&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-2 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;hr&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;with an average of 267.36 ± 7.93 from different thermal spring water samples.&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;concentration varied from 0.30 Bq l&lt;/p&gt;&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt; &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The radium&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;to 2.93 Bq l&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;with an average of 1.52 ± 0.045 Bq l&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-1&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;.&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;drinking, is safe as far as radium concentration is concerned with the exception of a few isolated&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;thermal spring sources. &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Results indicate that the thermal spring water, which is also being used for&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. Radiat. Res., 2005 2 (4): 197-204&lt;/font&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,SSNTDs,health,thermal spring,radon,Radium</keyword>
	<start_page>197</start_page>
	<end_page>204</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-86&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>K. Kant</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>kkant_67@rediffmail.com</email>
	<code>79003194753284600216</code>
	<orcid>79003194753284600216</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name> S.B. Upadhyay</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600217</code>
	<orcid>79003194753284600217</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>S.K. Chakarvarti</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600218</code>
	<orcid>79003194753284600218</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Application of small angle X-ray scattering (SAXS) for 
differentiation between normal and cancerous breast tissues</title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;1&quot;&gt;&lt;p align=&quot;left&quot; &gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Coherent scattering leads to diffraction effects and especially constructive interferences. These&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;interferences carry some information about the molecular structure of the tissue. As breast cancer is&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;the most widespread cancer in women, this project evaluated the application of small angle&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;X-ray scattering (SAXS) for differentiation between normal and cancerous breast tissues.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Small angle X-ray scattering (to angles less than 10&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;°&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;) is predominantly coherent.&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;primary collimator, sample holder, secondary collimator and HP Ge detector was used. The best&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;constructive interference was found to be at 6.5&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;at several angles of 4, 5, 6, 6.5 and 7.3 degrees. The total number of 99 breast tissue samples,&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;including normal and tumor were studied at the 6.5&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;transfer was obtained for each sample.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The energy dispersive method with a set up including X-ray tube,&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;° &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;after doing experiments on adipose breast tissue&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;°&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;. The corrected intensity versus momentum&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;adipose tissue and mixed tissue (adipose &amp; fibroglandular) from tumor in peak positions (each&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;coherent scattering spectrum has a peak that its position is determined by momentum transfer).&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Furthermore adipose tissue has shown significantly higher peaks than other breast tissues. Benign&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;and malignant breast tissues were differentiated by both peak positions and peak heights (each&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;peak has a height in coherent scattering spectrum). Preservation of samples nitrogen tank had no&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;effects on molecular structure of the breast tissue.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Adipose tissue shows a sharp peak in low momentum transfer region. It is easy to separate&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;between normal, benign and malignant breast tissues. &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;By energy dispersive small angle X-ray scattering, it is possible to differentiate&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. Radiat. Res., 2005 2 (4): 205-210&lt;/font&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,cancerous,normal,breast tissues,Small angle X-ray scattering</keyword>
	<start_page>205</start_page>
	<end_page>210</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-87&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>V. Changizi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>changizi@sina.tums.ac.ir</email>
	<code>79003194753284600219</code>
	<orcid>79003194753284600219</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name> M.A. Oghabian</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600220</code>
	<orcid>79003194753284600220</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name> S. Sarkar</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600221</code>
	<orcid>79003194753284600221</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name> R.D. Speller</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600222</code>
	<orcid>79003194753284600222</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>A. Arab Kheradmand</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600223</code>
	<orcid>79003194753284600223</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Gross beta activities and Beryllium-7 concentrations in surface air </title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>تحقيق بديع</content_type_fa>
	<content_type>Original Research</content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;1&quot;&gt;&lt;p align=&quot;left&quot; &gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Background: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;were made each week during year 2002 from samples of atmospheric aerosols filtered from the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;air at Tehran Nuclear Research Center.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Measurement of gross beta activities and cosmogenic Beryllium-7 concentrations&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Materials and Methods&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;sampler at the Nuclear Research Center meteorological station in Tehran (40&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;contents of samples were determined with semiconductor gamma spectrometry. The long-lived&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;beta activity, i.e. total beta activity measured four days after the end of sampling (after decay of&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;: The aerosol samples were collected weekly with high-volume air&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;o &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;35. N). The &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;7&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Be&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;&lt;p align=&quot;left&quot;&gt;220&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;The long-lived beta activity consists mainly of &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;amount of artificial radionuclides in the air is negligible.&lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Rn progeny and short-lived &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;220&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Rn progeny), was assessed with an automatic beta analyzer.&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;210&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Bi, the daughter nuclide of &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;210&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Pb, as the&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Results: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;lognormal distribution during the study period 2002. The arithmetic mean of annual concentrations&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;of &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;The air concentrations of both the &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;7&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Be and the long-lived beta activity displayed a&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;7&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Be and &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;210 &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Pb was 6.30 and 0.50 mBqm&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;-3&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;, respectively .&lt;/font&gt;&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Conclusion: &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;beta activities are partially correlated. Both have maximum concentrations during warm&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;mid-year months. &lt;/p&gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Despite the different origins, the concentrations of both the &lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;1&quot;&gt;7&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;Be and the long.lived&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. Radiat. Res., 2005 2 (4): 211-213&lt;/font&gt;&lt;/i&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,lead-210,gamma spectrometry,gross beta activity,Beryllium-7 concentrations</keyword>
	<start_page>211</start_page>
	<end_page>213</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-88&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>F. Arkian</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>arkian 1@yahoo.com</email>
	<code>79003194753284600224</code>
	<orcid>79003194753284600224</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>J. Amidi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600225</code>
	<orcid>79003194753284600225</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
	<article>


	<language>en</language>
	<article_id_doi></article_id_doi>
	<title_fa></title_fa>
	<title>Cardiac angiosarcoma Report of a case </title>
	<subject_fa>Radiation Biology</subject_fa>
	<subject>Radiation Biology</subject>
	<content_type_fa>گزارش کوتاه</content_type_fa>
	<content_type>Short Report </content_type>
	<abstract_fa></abstract_fa>
	<abstract>&lt;b&gt;&lt;font face=&quot;TimesNewRoman,Bold&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;ABSTRACT &lt;/p&gt;&lt;p align=&quot;left&quot; &gt;&lt;/font&gt;&lt;font face=&quot;TimesNewRoman&quot; size=&quot;3&quot;&gt;&lt;p align=&quot;left&quot;&gt;Sarcomas are the most malignant tumors in the myocardium. Most common sarcoma is the&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;angiosarcoma, classically located in the right atrium. Surgical resection is the primary treatment&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;of choice for these patients. In July 2003, an 18 years old man with chest pain and dyspnea,&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;referred to the Imam Khomeini Hospital. Chest X-ray showed cardiac enlargement and&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;transthoracic echocardiography demonstrated a large lobulated tumoral mass in right atrium.&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Cytologic examination of the pericardial effusion reported as no evidence of malignancy and&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;chest CT scan showed cardiac dilatation with blood density and pericardial effusion. The patient&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;underwent operation and tumor bulk was resected. Based on histological examination and&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;immunohistochemistry, diagnosis of cardiac angiosarcoma was made and the patient received&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;postoperative radiotherapy through parallel-opposed AP-PA cobalt beam technique. After&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;combined modality treatment with surgery and postoperative radiotherapy, symptoms were&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;disappeared and after 20 month follow up patient is symptom free. Despite of the ominous&lt;/p&gt;&lt;p align=&quot;left&quot;&gt;outcome of this malignancy an multimodality approach is worthy of consideration. &lt;/p&gt;&lt;p align=&quot;left&quot;&gt;Radiat. Res., 2005 2 (4): 215-218&lt;/p&gt;&lt;/font&gt;&lt;i&gt;&lt;font face=&quot;TimesNewRoman,Italic&quot; size=&quot;3&quot;&gt;Iran. J. &lt;/font&gt;&lt;/i&gt;&lt;/b&gt;</abstract>
	<keyword_fa></keyword_fa>
	<keyword>,immunohistochemistry,adjuvant radiotherapy, Cardiac angiosarcoma</keyword>
	<start_page>215</start_page>
	<end_page>218</end_page>
	<web_url>http://ijrr.com/browse.php?a_code=A-10-1-89&amp;slc_lang=en&amp;sid=1</web_url>


<author_list>
	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>M. Sardari Kermani</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email>Sardarik@sina.tums.ac.ir</email>
	<code>79003194753284600226</code>
	<orcid>79003194753284600226</orcid>
	<coreauthor>Yes
</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>F. Razi</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600227</code>
	<orcid>79003194753284600227</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


	<author>
	<first_name></first_name>
	<middle_name></middle_name>
	<last_name>E. Esmati</last_name>
	<suffix></suffix>
	<first_name_fa></first_name_fa>
	<middle_name_fa></middle_name_fa>
	<last_name_fa></last_name_fa>
	<suffix_fa></suffix_fa>
	<email></email>
	<code>79003194753284600228</code>
	<orcid>79003194753284600228</orcid>
	<coreauthor>No</coreauthor>
	<affiliation></affiliation>
	<affiliation_fa></affiliation_fa>
	 </author>


</author_list>


	</article>
</articleset>
</journal>
