Radiation dose verification using real tissue phantom in modern radiotherapy techniques
Identifieur interne : 000279 ( Pmc/Corpus ); précédent : 000278; suivant : 000280Radiation dose verification using real tissue phantom in modern radiotherapy techniques
Auteurs : Om Prakash Gurjar ; S. P. Mishra ; Virendra Bhandari ; Pankaj Pathak ; Prapti Patel ; Garima ShrivastavSource :
- Journal of Medical Physics / Association of Medical Physicists of India [ 0971-6203 ] ; 2014.
Abstract
Url:
DOI: 10.4103/0971-6203.125504
PubMed: 24600172
PubMed Central: 3931228
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en">Radiation dose verification using real tissue phantom in modern radiotherapy techniques</title><author><name sortKey="Gurjar, Om Prakash" sort="Gurjar, Om Prakash" uniqKey="Gurjar O" first="Om Prakash" last="Gurjar">Om Prakash Gurjar</name><affiliation><nlm:aff id="aff1">,</nlm:aff></affiliation><affiliation><nlm:aff>NONE</nlm:aff></affiliation></author><author><name sortKey="Mishra, S P" sort="Mishra, S P" uniqKey="Mishra S" first="S. P." last="Mishra">S. P. Mishra</name><affiliation><nlm:aff id="aff3">Department of Radiotherapy, Dr. Ram Manohar Lohia Institute of Medical Sciences, Lucknow, India</nlm:aff></affiliation><affiliation><nlm:aff>NONE</nlm:aff></affiliation></author><author><name sortKey="Bhandari, Virendra" sort="Bhandari, Virendra" uniqKey="Bhandari V" first="Virendra" last="Bhandari">Virendra Bhandari</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Pathak, Pankaj" sort="Pathak, Pankaj" uniqKey="Pathak P" first="Pankaj" last="Pathak">Pankaj Pathak</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Patel, Prapti" sort="Patel, Prapti" uniqKey="Patel P" first="Prapti" last="Patel">Prapti Patel</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Shrivastav, Garima" sort="Shrivastav, Garima" uniqKey="Shrivastav G" first="Garima" last="Shrivastav">Garima Shrivastav</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">PMC</idno><idno type="pmid">24600172</idno><idno type="pmc">3931228</idno><idno type="url">http://www.ncbi.nlm.nih.gov/pmc/articles/PMC3931228</idno><idno type="RBID">PMC:3931228</idno><idno type="doi">10.4103/0971-6203.125504</idno><date when="2014">2014</date><idno type="wicri:Area/Pmc/Corpus">000279</idno><idno type="wicri:explorRef" wicri:stream="Pmc" wicri:step="Corpus" wicri:corpus="PMC">000279</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a" type="main">Radiation dose verification using real tissue phantom in modern radiotherapy techniques</title><author><name sortKey="Gurjar, Om Prakash" sort="Gurjar, Om Prakash" uniqKey="Gurjar O" first="Om Prakash" last="Gurjar">Om Prakash Gurjar</name><affiliation><nlm:aff id="aff1">,</nlm:aff></affiliation><affiliation><nlm:aff>NONE</nlm:aff></affiliation></author><author><name sortKey="Mishra, S P" sort="Mishra, S P" uniqKey="Mishra S" first="S. P." last="Mishra">S. P. Mishra</name><affiliation><nlm:aff id="aff3">Department of Radiotherapy, Dr. Ram Manohar Lohia Institute of Medical Sciences, Lucknow, India</nlm:aff></affiliation><affiliation><nlm:aff>NONE</nlm:aff></affiliation></author><author><name sortKey="Bhandari, Virendra" sort="Bhandari, Virendra" uniqKey="Bhandari V" first="Virendra" last="Bhandari">Virendra Bhandari</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Pathak, Pankaj" sort="Pathak, Pankaj" uniqKey="Pathak P" first="Pankaj" last="Pathak">Pankaj Pathak</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Patel, Prapti" sort="Patel, Prapti" uniqKey="Patel P" first="Prapti" last="Patel">Prapti Patel</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author><author><name sortKey="Shrivastav, Garima" sort="Shrivastav, Garima" uniqKey="Shrivastav G" first="Garima" last="Shrivastav">Garima Shrivastav</name><affiliation><nlm:aff id="aff2">Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</nlm:aff></affiliation></author></analytic><series><title level="j">Journal of Medical Physics / Association of Medical Physicists of India</title><idno type="ISSN">0971-6203</idno><idno type="eISSN">1998-3913</idno><imprint><date when="2014">2014</date></imprint></series></biblStruct></sourceDesc></fileDesc><profileDesc><textClass></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en"><p><italic>In vitro</italic> dosimetric verification prior to patient treatment has a key role in accurate and precision radiotherapy treatment delivery. Most of commercially available dosimetric phantoms have almost homogeneous density throughout their volume, while real interior of patient body has variable and varying densities inside. In this study an attempt has been made to verify the physical dosimetry in actual human body scenario by using goat head as “head phantom” and goat meat as “tissue phantom”. The mean percentage variation between planned and measured doses was found to be 2.48 (standard deviation (SD): 0.74), 2.36 (SD: 0.77), 3.62 (SD: 1.05), and 3.31 (SD: 0.78) for three-dimensional conformal radiotherapy (3DCRT) (head phantom), intensity modulated radiotherapy (IMRT; head phantom), 3DCRT (tissue phantom), and IMRT (tissue phantom), respectively. Although percentage variations in case of head phantom were within tolerance limit (< ± 3%), but still it is higher than the results obtained by using commercially available phantoms. And the percentage variations in most of cases of tissue phantom were out of tolerance limit. On the basis of these preliminary results it is logical and rational to develop radiation dosimetry methods based on real human body and also to develop an artificial phantom which should truly represent the interior of human body.</p></div></front><back><div1 type="bibliography"><listBibl><biblStruct><analytic><author><name sortKey="Khan, Fm" uniqKey="Khan F">FM Khan</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Washington, Cm" uniqKey="Washington C">CM Washington</name></author><author><name sortKey="Leaver, Dt" uniqKey="Leaver D">DT Leaver</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Bouchard, H" uniqKey="Bouchard H">H Bouchard</name></author><author><name sortKey="Seuntjens, J" uniqKey="Seuntjens J">J Seuntjens</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Fraser, D" uniqKey="Fraser D">D Fraser</name></author><author><name sortKey="Parker, W" uniqKey="Parker W">W 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<front><journal-meta><journal-id journal-id-type="nlm-ta">J Med Phys</journal-id><journal-id journal-id-type="iso-abbrev">J Med Phys</journal-id><journal-id journal-id-type="publisher-id">JMP</journal-id><journal-title-group><journal-title>Journal of Medical Physics / Association of Medical Physicists of India</journal-title></journal-title-group><issn pub-type="ppub">0971-6203</issn><issn pub-type="epub">1998-3913</issn><publisher><publisher-name>Medknow Publications & Media Pvt Ltd</publisher-name><publisher-loc>India</publisher-loc></publisher></journal-meta><article-meta><article-id pub-id-type="pmid">24600172</article-id><article-id pub-id-type="pmc">3931228</article-id><article-id pub-id-type="publisher-id">JMP-39-44</article-id><article-id pub-id-type="doi">10.4103/0971-6203.125504</article-id><article-categories><subj-group subj-group-type="heading"><subject>Technical Note</subject></subj-group></article-categories><title-group><article-title>Radiation dose verification using real tissue phantom in modern radiotherapy techniques</article-title></title-group><contrib-group><contrib contrib-type="author"><name><surname>Gurjar</surname><given-names>Om Prakash</given-names></name><xref ref-type="aff" rid="aff1">1</xref><xref ref-type="aff" rid="aff2"></xref><xref ref-type="corresp" rid="cor1"></xref></contrib><contrib contrib-type="author"><name><surname>Mishra</surname><given-names>S. P.</given-names></name><xref ref-type="aff" rid="aff3">3</xref><xref ref-type="aff" rid="aff1"></xref></contrib><contrib contrib-type="author"><name><surname>Bhandari</surname><given-names>Virendra</given-names></name><xref ref-type="aff" rid="aff2">2</xref></contrib><contrib contrib-type="author"><name><surname>Pathak</surname><given-names>Pankaj</given-names></name><xref ref-type="aff" rid="aff2">2</xref></contrib><contrib contrib-type="author"><name><surname>Patel</surname><given-names>Prapti</given-names></name><xref ref-type="aff" rid="aff2">2</xref></contrib><contrib contrib-type="author"><name><surname>Shrivastav</surname><given-names>Garima</given-names></name><xref ref-type="aff" rid="aff2">2</xref></contrib></contrib-group><aff id="aff1"><label>1</label>,<label>3</label>Department of Physics, Mewar University, Chittorgarh, Rajasthan</aff><aff id="aff2"><label>1</label>,<label>2</label>Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore, Madhya Pradesh, India</aff><aff id="aff3"><label>3</label>Department of Radiotherapy, Dr. Ram Manohar Lohia Institute of Medical Sciences, Lucknow, India</aff><author-notes><corresp id="cor1"><bold>Address for correspondence:</bold> Mr. Om Prakash Gurjar, (Ph. D. Scholar - Mewar University), Asstt. Professor (Medical Physics) cum RSO (III) Roentgen-SAIMS Radiation Oncology Centre, Sri Aurobindo Institute of Medical Sciences, Indore - 453 111, Madhya Pradesh, India. E-mail: <email xlink:href="ominbarc@gmail.com">ominbarc@gmail.com</email></corresp></author-notes><pub-date pub-type="ppub"><season>Jan-Mar</season><year>2014</year></pub-date><volume>39</volume><issue>1</issue><fpage>44</fpage><lpage>49</lpage><history><date date-type="received"><day>19</day><month>7</month><year>2013</year></date><date date-type="rev-recd"><day>31</day><month>10</month><year>2013</year></date><date date-type="accepted"><day>31</day><month>10</month><year>2013</year></date></history><permissions><copyright-statement>Copyright: © Journal of Medical Physics</copyright-statement><copyright-year>2014</copyright-year><license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by-nc-sa/3.0"><license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution-Noncommercial-Share Alike 3.0 Unported, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p></license></permissions><abstract><p><italic>In vitro</italic> dosimetric verification prior to patient treatment has a key role in accurate and precision radiotherapy treatment delivery. Most of commercially available dosimetric phantoms have almost homogeneous density throughout their volume, while real interior of patient body has variable and varying densities inside. In this study an attempt has been made to verify the physical dosimetry in actual human body scenario by using goat head as “head phantom” and goat meat as “tissue phantom”. The mean percentage variation between planned and measured doses was found to be 2.48 (standard deviation (SD): 0.74), 2.36 (SD: 0.77), 3.62 (SD: 1.05), and 3.31 (SD: 0.78) for three-dimensional conformal radiotherapy (3DCRT) (head phantom), intensity modulated radiotherapy (IMRT; head phantom), 3DCRT (tissue phantom), and IMRT (tissue phantom), respectively. Although percentage variations in case of head phantom were within tolerance limit (< ± 3%), but still it is higher than the results obtained by using commercially available phantoms. And the percentage variations in most of cases of tissue phantom were out of tolerance limit. On the basis of these preliminary results it is logical and rational to develop radiation dosimetry methods based on real human body and also to develop an artificial phantom which should truly represent the interior of human body.</p></abstract><kwd-group><kwd>Head phantom</kwd><kwd>millennium 80 multileaf collimator system</kwd><kwd>real tissue</kwd><kwd>tissue phantom</kwd></kwd-group></article-meta></front><body><sec id="sec1-1"><title>Introduction</title><p>External radiation therapy has seen improvement in its day-to-day dose delivery technique and continued ascendance for dose escalation in the target volume for enhanced outcome. Initially radiation dose was delivered mostly by simple square open field using mainly cobalt as a radiation source.[<xref rid="ref1" ref-type="bibr">1</xref><xref rid="ref2" ref-type="bibr">2</xref>] Recent innovations have given several options for radiation treatment. A basket of energies are available and selection of suitable beam energy depending on the depth of tumor has become a standard practice to deliver tumoricidal dose. High energy linear accelerator (LA) with on-board imaging (OBI) system and computer-controlled multileaf collimator (MLC) has brought paradigm changes in the practice of radiotherapy. It has become possible to deliver large escalated dose to target and without exceeding the normal organs tolerance. Using these available techniques highly conformal and homogeneous dose can be delivered to target volume with less than 1 mm reproducible position accuracy. Now days, LA with multiple energy X-rays and unfiltered beam with very high dose rate are available. Multiple energy LA has option for selecting low energy or high energy photon beam or combination of both for low or high depth tumors and better homogeneity.[<xref rid="ref2" ref-type="bibr">2</xref>]</p><p>Dose in radiotherapy has connotation of cure. Success of planned dose on treatment planning system (TPS) and its outcome is entirely depended on the delivered dose to the respective site of patient with reproducible accuracy of planned dose or within tolerance. For this, many techniques are available to compare the delivered dose with planned dose. Generally absolute dosimetry is preferred in which point dose is measured at the specified and reference depth using ionization chamber and currently commercially available phantoms like slab phantom.[<xref rid="ref3" ref-type="bibr">3</xref><xref rid="ref4" ref-type="bibr">4</xref>] <italic>In vivo</italic> dosimetry using thermoluminescent dosimeters (TLD) or diodes is also in practice. In this method, TLD or diodes are placed on patient body at reference points and delivered dose is measured. Although in this technique dose is measured at skin and not in depth.[<xref rid="ref5" ref-type="bibr">5</xref>] This technique could be utilized to measure doses in rectum and bladder in patients of pelvic tumors. For reference dosimetry film, quality assurance (QA) is done in which film is placed in slab phantom at a particular depth at which the dose distribution is to be compared, then planned dose is delivered on it and then resultant density of film can be correlated with dose at each point on film which can be compared with the planned dose distribution. The density correlation with dose and comparison is done by commercially available film QA dosimetry systems, for example, OmniPro-I’MRT.[<xref rid="ref6" ref-type="bibr">6</xref><xref rid="ref7" ref-type="bibr">7</xref>] Reference dosimetry is also done using electronic portal imaging device (EPID), where planned dose is delivered by LA and recorded by EPID and then it can be compared with the planned dose distribution.[<xref rid="ref8" ref-type="bibr">8</xref><xref rid="ref9" ref-type="bibr">9</xref>]</p><p>In all above mentioned methods, the medium used is having homogeneous density while actual patient body has heterogeneous medium. International Commission on Radiation Units and Measurements (ICRU) which is an international body to provide guideline for radiation dosimetry and delineation of volumes of interest as elaborated in its report number 50, 62, and 83 (ICRU, 1993; 1999; 2010) have illustrated the mechanism of accurate and clearly target volume delineated.[<xref rid="ref10" ref-type="bibr">10</xref><xref rid="ref11" ref-type="bibr">11</xref><xref rid="ref12" ref-type="bibr">12</xref>] ICRU 83 published in 2010 propounds that single biggest cause of treatment failures are geographical miss due to inaccurate target delineation and dosimetric variation more than 3%.[<xref rid="ref12" ref-type="bibr">12</xref>] To improve the dosimetric part there is a need of improving the dosimetric equipment and procedure of patient specific QA.</p><p>There are various methods to achieve accuracy in dosimetry and they are based on International Atomic Energy Agency (IAEA) recommendations published in technical reports series number 277 and 398.[<xref rid="ref13" ref-type="bibr">13</xref><xref rid="ref14" ref-type="bibr">14</xref>] It is clearly established today that human body comprises of fat, tissue, bones, and air cavities, and they influence the transport of photon and electron energy which results in consequential dose delivery to target volume. It is therefore essential to stabilize a quality dosimetric practices and pretreatment verification.</p><p>The medium of all reference QA phantoms which are in practice is homogeneous like water phantom, slab phantom, acrylic body phantom, etc., that is, medium is made of material with same density throughout its volume. Although the anthropomorphic phantom has heterogeneous medium but it is very basic phantom which cannot be considered similar to human body. The methods mentioned in AAPM Task Group Report 120 (intensity modulated radiotherapy (IMRT) dosimetry tools)[<xref rid="ref15" ref-type="bibr">15</xref>] also prescribes the similar kind of QA procedures.</p></sec><sec sec-type="materials|methods" id="sec1-2"><title>Materials and Methods</title><p>Mammals include most of the animals and human beings and the body tissue actually mimic each other. We used one of the mammals “GOAT” for our study. Goat head and goat meat (with bones and air cavities naturally existing in it) thrown as waste material by meat shops were used to construct two kinds of phantoms namely “head phantom” [<xref ref-type="fig" rid="F1">Figure 1a</xref>] and “tissue phantom” [<xref ref-type="fig" rid="F1">Figure 1b</xref>]. And for dose measurement 0.13 cc ionization chamber (IBA Dosimetry, Germany) and DOSE1 electrometer (IBA Dosimetry, Germany) was utilized.</p><fig id="F1" position="float"><label>Figure 1</label><caption><p>Photographs of the (a) head phantom and (b) tissue phantom</p></caption><graphic xlink:href="JMP-39-44-g001"></graphic></fig><p>Head phantom was goat head wrapped in polythene and tissue phantom was made by goat meat giving it cubic shape of dimension approximately 20 cm × 20 cm × 20 cm by putting it in thermoplastic sheet (Orfit) molded in required shape with having thin polythene pasted inside to hold the tissue in same physical state. Ion chamber was fixed in the cavity prepared by screw driver at approximately geometrical center of phantom volume and was kept at same position till the end of experiment. Three fiducial lead markers were put on two bilateral points and one anterior point on surface of phantom in same cross-sectional plan to make three reference points. Head phantom was utilized for first experiment and tissue phantom was utilized for second experiment. Both experiments were done on 2 different days using same methodology.</p><p>Siemens SOMATOM Definition AS scanner (Siemens Medical Systems, Germany) has been utilized for computed tomography (CT) of both the phantoms and CT images of 3 mm slice thickness were taken for planning purpose. Then phantom along with ion chamber and attached accessories was kept in freezer during the period of treatment planning to prevent decomposition and the tissue conditions remain same throughout the period of experiment.</p><p>The CT images were imported on TPS Eclipse version 8.9 (Varian Medical Systems, Palo Alto, CA) and various types of plans already done for actual patients were exported on phantom and dose was calculated using anisotropic analytical algorithm (AAA) version 8.9.08 with grid size of 0.25 cc.</p><p>The patient plans selected for head phantom were those planned for brain and head-and-neck (H and N) tumors and the plans selected for tissue phantom were for lung, breast, and pelvic tumors. Field arrangement for IMRT plans was done in such a way that all fields were coplanar (CP) with couch angle 0° and no parallel opposed fields were placed, some plans for brain tumors had one none-CP (NCP) field with couch angle 90°/270° and gantry angle from 330°/30° to 350°/10°. Two fields at each gantry angle were also used in some plans which had large target volumes, as if field exceeds 14.5 cm in x-direction it gets split in two fields automatically. The splitting is because of the limitation that is present in MLC, where in the maximum distance between the most retracted and extended MLC, cannot be more than 14.5 cm. And in this way maximum of 18 fields at nine gantry angles were used in some plans.</p><p>Dose constraints and adequate weights were given for organs at risk (OAR) and target volumes (planning target volume (PTV), clinical target volume (CTV), and gross tumor volume (GTV)). Varian leaf motion calculator version 8.9.08 was utilized to calculate leaf motion for dynamic dose delivery. All IMRT plans were done with 6 MV photon beam and dose volume optimizer (DVO) was used for plan optimization. AAA was used to calculate doses with grid size of 0.25 cc.</p><p>Three-dimensional conformal radiotherapy (3DCRT) plans were generated by simple two to five fields in single plane with couch angle 0°, some plans for brain cases had NCP field with couch angle 90°/270° and gantry angle from 330°/30° to 350°/10°. Two plans with junction fields were also chosen for this study in which plans were made by 3DCRT technique for carcinoma of breast under which two tangential fields (couch 0°, gantry angles 310°/50°−325°/35° and 130°/230°−145°/215°) with collimator Y2 fully closed and one anterior field (couch angle 0°, gantry angle 0°) with collimator Y1 fully closed were used. The isocenter of plan was placed at junction of PTV for chest wall and PTV for supraclavicle region. All plans were generated without wedges.</p><p>All 3DCRT plans were done by using 6 MV, 15 MV, or combination of both photon energies. Doses were calculated by using AAA with 0.25 cc grid size. Weight of particular fields in some plans was decreased/increased by changing monitoring units (MU) wherever required to manage hot/cold spot and dose homogeneity.</p><p>Figure <xref ref-type="fig" rid="F2">2a</xref> and <xref ref-type="fig" rid="F2">b</xref> shows the dose distribution on CT slices of head phantom and tissue phantom. After approving all the plans were exported to high energy medical LA Clinac DMX (Varian Medical Systems, Palo Alto, CA) having photon energies of 6 and 15 MV and electron energies of 6, 9, 12, and 15 MeV. This LA is equipped with Millennium 80 MLC. Millennium 80 MLC system has 40 pairs of leaves and MLC leaf width projected at isocenter is 1 cm. The MLC leaf ends are rounded. The interleaf leakage is minimized by tongue and groove arrangement. In dynamic/moving window treatment mode, standard MLC leaf speed is 2.5 cm/s. The MLC workstation records the system status (MLC leaf positions) during MLC treatment delivery. TPS and 4-dimensional treatment console (4DTC) systems are networked through networking system ARIA.
<fig id="F2" position="float"><label>Figure 2</label><caption><p>Dose distribution in case of (a) head phantom and (b) tissue phantom</p></caption><graphic xlink:href="JMP-39-44-g002"></graphic></fig></p><p>The phantom was taken out of the freezer and was set on LA-couch with the help of reference points in same position as it was on CT-couch. To verify the position cone beam CT (CBCT) images were obtained using OBI system (Varian Medical Systems, Palo Alto, CA) with half bow-tie filter and compared with reference CT images. The minor shift in position was corrected.</p><p>After position verification all IMRT plans were delivered by LA with dynamic dose delivery technique and 3DCRT plans with planned open field technique along with accessories. Dose for each plan was measured using electrometer connected to the ion chamber which was fixed in phantom. These measured doses were compared with doses planned on TPS.</p></sec><sec id="sec1-3"><title>Results and Discussion</title><p>A study on patient specific absolute dosimetry using goat head and goat meat for improvement in dosimetry in modern radiotherapy techniques has been done to evaluate the outcome of real tissue based measurements. The mean % variation between planned doses and measured doses was noted as 2.48 (standard deviation (SD): 0.74), 2.36 (SD: 0.77), 3.62 (SD: 1.05), and 3.31 (SD: 0.78) for 3DCRT (head phantom), IMRT (head phantom), 3DCRT (tissue phantom), and IMRT (tissue phantom), respectively.</p><p>Although % variations in case of head phantom were within tolerance limit (< ± 3%) prescribed in ICRU 83, but still it is higher than the results obtained by using routine QA phantoms of homogeneous density. Percentage variations in case of tissue phantom were higher, although the higher variations in this case may have minor contribution of possibility of small change in volume during the period of around 3 h from CT scan to dose delivery. Measurements of this study indicate that most of variations are higher than recommended by international body of < ± 3% (ICRU 83).[<xref rid="ref12" ref-type="bibr">12</xref>] Such variations may have large implication in treatment outcome in modern radiotherapy. While in case of routine patient specific absolute dosimetry using commercially available slab phantom the variation between measured and TPS calculated dose values is always found within ± 3%, and in most of the cases it comes within ± 1%, while rarely goes above ± 2%. It is as the medium in slab phantom is made of material with same density throughout its volume.</p><p>Phantoms used in this study had been made of goat head (head phantom) and goat meat (tissue phantom) which had inhomogeneous medium having bones, tissues, and air cavities same as in human body. Although pig tissue structure is more similar to human tissue structure but due to easy availability of goat meat in India, it has been selected for this study.[<xref rid="ref16" ref-type="bibr">16</xref>] Although the interaction of therapeutic radiation with every type of tissue in human body is of same kind that is predominantly Compton scattering. The number of secondary electrons produced depends on density of medium and hence following points could be made out.</p><sec id="sec2-1"><title></title><sec id="sec3-1"><title>Soft tissue-bone interface</title><p>As density of soft tissue is lesser than bone so lesser number of secondary electrons is produced and when they enter in bone some of them reflect back. In this way reflected electrons deposit dose in soft tissue near interface area, while dose deposited in bone is comparatively less.</p></sec><sec id="sec3-2"><title>Bone-soft tissue interface</title><p>Since density of bone is high so production of secondary electrons is also higher, thus dose deposited in soft tissue near to interface area is higher.</p><p>Similar phenomenon in the case of air cavity-bone interface, air cavity-soft tissue interface, and vice versa is seen.[<xref rid="ref17" ref-type="bibr">17</xref><xref rid="ref18" ref-type="bibr">18</xref>]</p><p>The density of frequently used materials for dosimetry and components of human body is as shown in <xref ref-type="table" rid="T1">Table 1</xref>.[<xref rid="ref1" ref-type="bibr">1</xref><xref rid="ref19" ref-type="bibr">19</xref><xref rid="ref20" ref-type="bibr">20</xref>]</p><p><xref ref-type="table" rid="T1">Table 1</xref> shows density, atomic number, and electron density of various materials where it can be clearly seen that electron density varies in all the materials by a significant number, hence most of the phantoms which are currently in use do not represent the actual human body.</p><table-wrap id="T1" position="float"><label>Table 1</label><caption><p>Number of electrons per gram of various materials</p></caption><graphic xlink:href="JMP-39-44-g003"></graphic></table-wrap><p><xref ref-type="table" rid="T2">Table 2</xref> compares the density of some organs of goat and human, where density of each organ was calculated with the help of Hounsfield units (HU) measured from TPS and HU-density conversion formula H = 1000.((ρ/ρ<sub>w</sub>) - 1.0).[<xref rid="ref21" ref-type="bibr">21</xref>]</p><table-wrap id="T2" position="float"><label>Table 2</label><caption><p>Mass density of some organs of human and goat</p></caption><graphic xlink:href="JMP-39-44-g004"></graphic></table-wrap><p>We can see in above table that density of respective organs of human and goat are approximately same. So using the mentioned head and tissue phantom for primary study was a good choice and similar artificial phantom will be very useful in such kind of dosimetry.</p><p>Tables <xref ref-type="table" rid="T3">3</xref>–<xref ref-type="table" rid="T6">6</xref> show the measurements and results of this study. <xref ref-type="fig" rid="F3">Figure 3</xref> shows the graphical comparison of % variations between planned and measured doses in all four kind of experiments.</p><table-wrap id="T3" position="float"><label>Table 3</label><caption><p>In 3DCRT plans % variation between planned dose on treatment planning system and measured dose on linear accelerator using head phantom</p></caption><graphic xlink:href="JMP-39-44-g005"></graphic></table-wrap><table-wrap id="T4" position="float"><label>Table 4</label><caption><p>In IMRT plans % variation between planned dose on treatment planning system and measured dose on linear accelerator using head phantom</p></caption><graphic xlink:href="JMP-39-44-g006"></graphic></table-wrap><table-wrap id="T5" position="float"><label>Table 5</label><caption><p>In 3DCRT plans % variation between planned dose on treatment planning system and measured dose on linear accelerator using tissue phantom</p></caption><graphic xlink:href="JMP-39-44-g007"></graphic></table-wrap><table-wrap id="T6" position="float"><label>Table 6</label><caption><p>In IMRT plans % variation between planned dose on treatment planning system and measured dose on linear accelerator using tissue phantom</p></caption><graphic xlink:href="JMP-39-44-g008"></graphic></table-wrap><fig id="F3" position="float"><label>Figure 3</label><caption><p>Graphical comparison of % variations between planned doses (on treatment planning system) and measured doses (on linear accelerator) in four types of measurements viz. three-dimensional conformal radiotherapy plans using head phantom, intensity modulated radiotherapy plans using head phantom, 3DCRT plans using tissue phantom, and IMRT plans using tissue phantom</p></caption><graphic xlink:href="JMP-39-44-g009"></graphic></fig></sec></sec></sec><sec sec-type="conclusions" id="sec1-4"><title>Conclusions</title><p>Dose verification measurements for modern radiotherapy techniques (3DCRT, IMRT, and image-guided radiation therapy (IGRT)) were carried out using head (goat head) and tissue (goat meat) phantoms. The results of these measurements were comparatively higher than the results of routine dose verification using commercially available phantoms and some results are higher than tolerance limit (< ± 3%) prescribed in ICRU 83. This study makes a strong case to develop radiation dosimetry methods based on real human body and also to develop an artificial phantom which should truly represent the interior of human body.</p></sec></body><back><ack><title>Acknowledgment</title><p>We would like to express our thanks to director, Roentgen Oncologic Solutions Pvt. Ltd. and Chairman, Sri Aurobindo Institute of Medical Sciences for permitting and encouraging the study. We would also like to express our appreciation for the Radiotherapy Technologists R. Bornare and team for their support.</p></ack><fn-group><fn fn-type="supported-by"><p><bold>Source of Support:</bold> Equipment support from Roentgen Oncologic Solutions Pvt. 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