<?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">IJMPCERO</journal-id><journal-title-group><journal-title>International Journal of Medical Physics, Clinical Engineering and Radiation Oncology</journal-title></journal-title-group><issn pub-type="epub">2168-5436</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmpcero.2019.84020</article-id><article-id pub-id-type="publisher-id">IJMPCERO-96372</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Evaluation of Delivery Analysis to Detect Intrafractional Motion during Tomotherapy
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kazuo</surname><given-names>Tarutani</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>Masao</surname><given-names>Tanooka</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Keisuke</surname><given-names>Sano</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Okada</surname><given-names>Wataru</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Masayuki</surname><given-names>Fujiwara</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Koichiro</surname><given-names>Yamakado</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Japan Organization of Occupational Health and Safety Kansai Rousai Hospital, Amagasaki, Japan</addr-line></aff><aff id="aff3"><addr-line>Department of Radiotherapy, Takarazuka City Hospital, Takarazuka, Japan</addr-line></aff><aff id="aff2"><addr-line>Department of Radiology, Hyogo College of Medicine, Nishinomiya, Japan</addr-line></aff><pub-date pub-type="epub"><day>16</day><month>09</month><year>2019</year></pub-date><volume>08</volume><issue>04</issue><fpage>225</fpage><lpage>235</lpage><history><date date-type="received"><day>28,</day>	<month>October</month>	<year>2019</year></date><date date-type="rev-recd"><day>11,</day>	<month>November</month>	<year>2019</year>	</date><date date-type="accepted"><day>14,</day>	<month>November</month>	<year>2019</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The purpose of this study was to investigate the ability of a management system (Delivery Analysis: DA) to detect intrafractional motion during intensity-modulated radiation therapy (IMRT) in tomotherapy mode. Tomotherapy has made it possible to manage internal movements during treatment using software DA, which quantifies using the information of the passing dose obtained during the radiation treatment of patients. First, three treatment plans for the test were created (lumbar spine, prostate, and femur). Second, a pelvis phantom was moved in the X, Y, and Z directions, and a sinogram was acquired. The magnitudes of the movements were 3 mm, 5 mm, and 10 mm, respectively. Finally, the ability of DA to detect the motion was evaluated by comparing the sinogram obtained by moving the phantom with a reference sinogram obtained without movement. The sensitivity of DA could be detected with a shift amount of 3 mm (gamma analysis tolerance 0.3 mm/0.3%). The average gamma analysis of each direction at 0.3 mm/0.3% tolerance at each treatment site was 96.1% for the prostate, 93.5% for the lumbar spine, and 94.4% for the femur. Additionally, the average gamma pass rate results for the pelvic phantom in the X, Y, Z directions for a 10 mm shift were 96.2%, 96.3%, and 95.9%, respectively. DA is a powerful tool with high detection sensitivity and ability to detect body movement during treatment.
 
</p></abstract><kwd-group><kwd>Delivery Analysis (DA)</kwd><kwd> Tomotherapy</kwd><kwd> Sinogram</kwd><kwd> Intra-Fraction Motion</kwd><kwd> Quality Assurance (QA)</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Intensity-modulated radiation therapy (IMRT) is a useful method that can increase dose to tumor tissue while decreasing dose to organs at risk [<xref ref-type="bibr" rid="scirp.96372-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref2">2</xref>]. Tomotherapy (Accuray, Sunnyvale, CA, USA) is one of the modern radiotherapy systems which allow a continuous dose delivery in a helical fashion around the anatomical site to be treated [<xref ref-type="bibr" rid="scirp.96372-ref3">3</xref>].</p><p>Based on a small 6 MV linear accelerator attached to a ring gantry that rotates around the patient as the patient moves around the bore, it is mechanically unique and ultimately produces a helical path for radiation dose delivery. In tomotherapy, this technologically advanced radiation dose delivery system provides pre-treatment quality assurance (QA) which ensures the safety of treatment by performing delivery quality assurance (DQA) [<xref ref-type="bibr" rid="scirp.96372-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref5">5</xref>]. However, this method has not been used during treatment to evaluate intrafractional motion.</p><p>In volume-modulated arc therapy (VMAT) using a linear accelerator, the various types of pre-treatment QA have led to an improvement in safety [<xref ref-type="bibr" rid="scirp.96372-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref10">10</xref>]. Nevertheless, although these validations improve VMAT’s safety, errors during treatment still produce random and systematic uncertainty [<xref ref-type="bibr" rid="scirp.96372-ref11">11</xref>].</p><p>With traditional pre-treatment QA, it is impossible to predict mechanical errors, inappropriate movements or human errors that occur during treatment [<xref ref-type="bibr" rid="scirp.96372-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref13">13</xref>]. Therefore, methods of dose assessment during treatment have been developed in multiple research facilities [<xref ref-type="bibr" rid="scirp.96372-ref14">14</xref>] - [<xref ref-type="bibr" rid="scirp.96372-ref18">18</xref>], and have been commercialized [<xref ref-type="bibr" rid="scirp.96372-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.96372-ref20">20</xref>]. Ford et al. [<xref ref-type="bibr" rid="scirp.96372-ref21">21</xref>] conducted a validation with an electronic portal imaging device (EPID) during treatment and found multiple errors with potentially major severity. This makes management during treatment very important.</p><p>In a tomotherapy delivery system, delivery analysis (DA) software is implemented during treatment. DA compares pretreatment and measured in-treatment data with information describing the planned treatment delivery.</p><p>Pretreatment assessment provides tools to quickly confirm that the multileaf collimator (MLC) has performed according to the treatment plan and assess any differences in MLC performance that may impact delivery.</p><p>In-treatment assessment monitors the consistency of delivery with particular sensitivity to patient settings and anatomical variations and patient motion during treatment. Tomotherapy can use this feature to enable management during treatment.</p><p>Management during treatment with an EPID with a linear accelerator generally uses integrated data with X-rays transmitted through the patient, which reduces the accuracy of intrafractional motion error detection [<xref ref-type="bibr" rid="scirp.96372-ref22">22</xref>]. However, when DA is used in tomotherapy, data are output as sinogram data, not integrated data. Therefore, in DA, it can be expected that error detectability during treatment can be further improved. To date, however, the clinical significance of differing levels of discrepancy in in-treatment assessment has not been evaluated.</p><p>Therefore, we investigated the motion detectability of the DA management system in-treatment during IMRT treatment with tomotherapy.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Tomotherapy Delivery System, Radixact</title><p>Tomotherapy unit is designed to provide IMRT with 6 MV photon beam and binary 64 MLC [<xref ref-type="bibr" rid="scirp.96372-ref3">3</xref>]. Radixact (Version.1.1.0.1: Accuray, Sunnyvale, CA, USA) is the latest generation of Tomotherapy delivery systems and represents a redesign of both gantry and treatment planning systems. In Radixact, new QA software is renewed and DA is implemented.</p><p>The unit provides both “Tomohelical” and “TomoDirect” modes. Tomotherapy units clinically used three different field widths of 1.0, 2.5, and 5.0 cm, which were defined by jaws along the longitudinal direction.</p></sec><sec id="s2_2"><title>2.2. Delivery Analysis (DA)</title><sec id="s2_2_1"><title>2.2.1. Pre-Treatment Assessment</title><p>Pre-treatment assessment is a tool to assess that collimation is being performed according to the treatment plan. This plan reconstructs a measured MLC leaf open time sinogram by analyzing the pulse-by-pulse data from the detector during delivery and measuring the individual leaf open times using the high-signal pulses for each delivered projection. This assessment also calculates the dose distribution based on the measured MLC leaf open time sinogram, the original plan, and the planning CT, and compares and analyzes the original planned dose and the recalculated dose based on the measured MLC leaf open time sinogram. Because this study was an evaluation during treatment, we excluded this pre-treatment study.</p></sec><sec id="s2_2_2"><title>2.2.2. In-Treatment Assessment</title><p>In-treatment assessment is software that quantifies consistency interfraction motion during treatment using post patient detector signals obtained during patient radiation therapy (<xref ref-type="fig" rid="fig1">Figure 1</xref>). The purpose is to capture changes in the patient’s anatomy or positional misalignments. The data collection method uses a detector to receive X-rays that have passed through the patient’s body during treatment. As soon as the treatment is finished, the data are taken to a stand-alone workstation separate from the treatment system network. This is done automatically. In addition, the consistency of irradiation can be evaluated by managing daily data in a trend graph.</p></sec></sec><sec id="s2_3"><title>2.3. Assessment Method</title><p>We used Radixact and the software used DA Ver1.1. A commercial pelvic phantom (ExacTrac Verification Phantom, BrainLab, Feldkirchen, Germany) was used. The assessment method is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Treatment plan consisted of three parts (lumbar spine and prostate, femur). The pelvic phantom was moved in the X, Y, and Z directions, assuming a body movement for each plan. The magnitudes of the errors to be moved were 3 mm, 5 mm, and 10 mm, respectively. Radixact’s table drive accuracy was &#177; 0.5 mm (display value unit: 0.1 mm). The first irradiation was used as a reference. The phantom was before treatment moved on the assumption of body movement with respect to the base</p><p>sinogram acquired first, and the acquired sinograms were compared. We used gamma analysis [<xref ref-type="bibr" rid="scirp.96372-ref23">23</xref>] as a comparison method. To confirm the sensitivity of gamma analysis tolerances, the setting values were changed to 3 mm/3%, 2 mm/3%, 2 mm/2%, 1 mm/1%, 0.5 mm/0.5%, 0.3 mm/0.3%. We also compared the analysis results.</p><p>In summary, 3 mm, 5 mm, and 10 mm are moved in the X, Y, and Z directions for each part of the lumbar spine, prostate, and femur, and sinogram data was acquired and evaluated by gamma analysis. Also, the influence of the result of the gamma analysis which made variable the tolerance value for each relationship was investigated.</p></sec></sec><sec id="s3"><title>3. Results</title><p><xref ref-type="table" rid="table1">Table 1</xref> shown shows the results of gamma analysis in which the pelvic phantom was moved to 3 mm, 5 mm, and 10 mm for each site. The measurement was performed five times and the average mean value was shown. The variation of the five measurements was small and the standard deviation was negligible. From this table, it is impossible to detect an error of movement at a tolerance of 3 mm/3%. However, when the tolerance is 0.3 mm/0.3% and the shift is a 3 mm error, the result of gamma analysis at the lowest sensitivity is 94.0% for the prostate and 93.3% for the and 93.8% for the femur in and the lumbar spine, respectively. Therefore, in-treatment motion proved to be detectable.</p><sec id="s3_1"><title>3.1. Influence of Result by Movement Amount</title><p>The relationship between the shift amount of the pelvic phantom and the tolerance of gamma analysis is shown (<xref ref-type="fig" rid="fig3">Figure 3</xref>). The tolerance did not change significantly up to 2 mm/2%. When the tolerance was lowered to 1 mm/1%, the results were affected.</p><p>In addition, the amount of movement of the pelvic phantom was lower in gamma passing rate when it was moved by 10 mm compared to 3 mm. Therefore, it was proved that the pass rate decreases in proportion to the magnitude of the shift amount of the pelvic phantom.</p><p>When the tolerance was 0.3 mm/0.3%, the average gamma pass rate was 94.7%, 92.2%, and 89.9% when the shift amount of the pelvis phantom was 3 mm, 5 mm, and 10 mm, respectively. DA was able to detect a 3 mm shift.</p></sec><sec id="s3_2"><title>3.2. Influence of Result by Movement Direction</title><p>The following shows the relationship between the movement direction and the result of gamma analysis (<xref ref-type="fig" rid="fig4">Figure 4</xref>). The average gamma pass rate results for the pelvic phantom for the X, Y, and Z directions for a 10 mm shift were 96.2%, 96.4%, and 95.9%, respectively. No difference was found in the direction of movement.</p></sec><sec id="s3_3"><title>3.3. Influence of Result by Each Treatment Site</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the result of the pass rate of gamma analysis to tolerance at each treatment site. The average gamma analysis for each direction at 0.3 mm/0.3% tolerance was 96.1% for the prostate, 93.5% for the lumbar spine, and 94.4% for the femur. It was confirmed that the sensitivity of the prostate was little lower than other parts.</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The mean value of the gamma analysis (%) that was performed five times and its standard deviation (%). Results of gamma analysis with different tolerance values and phantom movement values for each part (prostate, lumbar vertebra, femur)</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="4"  >Gamma pass rate (%)</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Site</td><td align="center" valign="middle"  colspan="4"  >Prostate</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Shift value</td><td align="center" valign="middle" >0 mm</td><td align="center" valign="middle" >3 mm</td><td align="center" valign="middle" >5 mm</td><td align="center" valign="middle" >10 mm</td></tr><tr><td align="center" valign="middle"  rowspan="18"  >Tolerance</td><td align="center" valign="middle"  rowspan="6"  >X-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.94 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.99 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.99 &#177; 0.00</td><td align="center" valign="middle" >99.93 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.91 &#177; 0.01</td><td align="center" valign="middle" >99.71 &#177; 0.00</td><td align="center" valign="middle" >99.08 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle" >100 &#177; 0.04</td><td align="center" valign="middle" >99.06 &#177; 0.08</td><td align="center" valign="middle" >98.07 &#177; 0.07</td><td align="center" valign="middle" >96.36 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle" >100 &#177; 0.05</td><td align="center" valign="middle" >97.44 &#177; 0.21</td><td align="center" valign="middle" >95.77 &#177; 0.07</td><td align="center" valign="middle" >94.22 &#177; 0.04</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Y-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.90 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.86 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.93 &#177; 0.01</td><td align="center" valign="middle" >99.43 &#177; 0.02</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.74 &#177; 0.00</td><td align="center" valign="middle" >98.48 &#177; 0.05</td><td align="center" valign="middle" >95.80 &#177; 0.02</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle" >100 &#177; 0.03</td><td align="center" valign="middle" >99.60 &#177; 0.06</td><td align="center" valign="middle" >97.75 &#177; 0.02</td><td align="center" valign="middle" >94.17 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle" >100 &#177; 0.05</td><td align="center" valign="middle" >93.97 &#177; 0.05</td><td align="center" valign="middle" >91.88 &#177; 0.06</td><td align="center" valign="middle" >90.51 &#177; 0.01</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Z-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.94 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.92 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.01</td><td align="center" valign="middle" >99.71 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.87 &#177; 0.01</td><td align="center" valign="middle" >99.45 &#177; 0.02</td><td align="center" valign="middle" >98.15 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle" >100 &#177; 0.06</td><td align="center" valign="middle" >98.71 &#177; 0.09</td><td align="center" valign="middle" >97.14 &#177; 0.02</td><td align="center" valign="middle" >94.80 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle" >100 &#177; 0.09</td><td align="center" valign="middle" >96.80 &#177; 0.16</td><td align="center" valign="middle" >94.88 &#177; 0.03</td><td align="center" valign="middle" >92.79 &#177; 0.02</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Site</td><td align="center" valign="middle"  colspan="4"  >Lumbar spine</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Shift value</td><td align="center" valign="middle" >0 mm</td><td align="center" valign="middle" >3 mm</td><td align="center" valign="middle" >5 mm</td><td align="center" valign="middle" >10 mm</td></tr><tr><td align="center" valign="middle"  rowspan="12"  >Tolerance</td><td align="center" valign="middle"  rowspan="6"  >X-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.85 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.81 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.90 &#177; 0.00</td><td align="center" valign="middle" >99.36 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle" >100 &#177; 0.03</td><td align="center" valign="middle" >99.64 &#177; 0.04</td><td align="center" valign="middle" >98.80 &#177; 0.02</td><td align="center" valign="middle" >96.05 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle" >100 &#177; 0.10</td><td align="center" valign="middle" >97.16 &#177; 0.06</td><td align="center" valign="middle" >94.28 &#177; 0.06</td><td align="center" valign="middle" >90.00 &#177; 0.04</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle" >100 &#177; 0.31</td><td align="center" valign="middle" >93.94 &#177; 0.04</td><td align="center" valign="middle" >91.07 &#177; 0.09</td><td align="center" valign="middle" >87.73 &#177; 0.08</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Y-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.96 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.94 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >100 &#177; 0.00</td><td align="center" valign="middle" >99.96 &#177; 0.00</td><td align="center" valign="middle" >99.58 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle" >100 &#177; 0.03</td><td align="center" valign="middle" >99.71 &#177; 0.01</td><td align="center" valign="middle" >98.82 &#177; 0.03</td><td align="center" valign="middle" >96.91 &#177; 0.08</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle" >100 &#177; 0.11</td><td align="center" valign="middle" >96.99 &#177; 0.10</td><td align="center" valign="middle" >94.48 &#177; 0.15</td><td align="center" valign="middle" >91.13 &#177; 0.13</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle" >100 &#177; 0.22</td><td align="center" valign="middle" >93.37 &#177; 0.15</td><td align="center" valign="middle" >90.70 &#177; 0.18</td><td align="center" valign="middle" >88.16 &#177; 0.09</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="6"  ></th><th align="center" valign="middle"  rowspan="6"  >Z-direction</th><th align="center" valign="middle" >3 mm/3%</th><th align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</th><th align="center" valign="middle"  colspan="2"  >99.99 &#177; 0.00</th><th align="center" valign="middle"  colspan="2"  >99.90 &#177; 0.00</th><th align="center" valign="middle" >99.51 &#177; 0.00</th></tr></thead><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.99 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.86 &#177; 0.00</td><td align="center" valign="middle" >99.38 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.89 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.61 &#177; 0.01</td><td align="center" valign="middle" >98.63 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.13 &#177; 0.01</td><td align="center" valign="middle"  colspan="2"  >97.78 &#177; 0.04</td><td align="center" valign="middle" >95.10 &#177; 0.02</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.07</td><td align="center" valign="middle"  colspan="2"  >96.23 &#177; 0.09</td><td align="center" valign="middle"  colspan="2"  >93.12 &#177; 0.27</td><td align="center" valign="middle" >89.43 &#177; 0.07</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.20</td><td align="center" valign="middle"  colspan="2"  >93.26 &#177; 0.13</td><td align="center" valign="middle"  colspan="2"  >89.94 &#177; 0.41</td><td align="center" valign="middle" >86.91 &#177; 0.05</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Site</td><td align="center" valign="middle"  colspan="7"  >Femur</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Shift value</td><td align="center" valign="middle" >0 mm</td><td align="center" valign="middle"  colspan="2"  >3 mm</td><td align="center" valign="middle"  colspan="2"  >5 mm</td><td align="center" valign="middle"  colspan="2"  >10 mm</td></tr><tr><td align="center" valign="middle"  rowspan="18"  >Tolerance</td><td align="center" valign="middle"  rowspan="6"  >X-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.83 &#177; 0.00</td><td align="center" valign="middle" >98.74 &#177; 0.06</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.79 &#177; 0.00</td><td align="center" valign="middle" >98.46 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.89 &#177; 0.02</td><td align="center" valign="middle"  colspan="2"  >99.19 &#177; 0.01</td><td align="center" valign="middle" >97.36 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >98.53 &#177; 0.04</td><td align="center" valign="middle"  colspan="2"  >96.73 &#177; 0.01</td><td align="center" valign="middle" >94.56 &#177; 0.02</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >95.48 &#177; 0.03</td><td align="center" valign="middle"  colspan="2"  >93.29 &#177; 0.04</td><td align="center" valign="middle" >90.82 &#177; 0.04</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.04</td><td align="center" valign="middle"  colspan="2"  >94.31 &#177; 0.49</td><td align="center" valign="middle"  colspan="2"  >91.73 &#177; 0.01</td><td align="center" valign="middle" >89.03 &#177; 0.07</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Y-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.94 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.82 &#177; 0.00</td><td align="center" valign="middle" >99.46 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.93 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.80 &#177; 0.00</td><td align="center" valign="middle" >99.40 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.81 &#177; 0.01</td><td align="center" valign="middle"  colspan="2"  >99.54 &#177; 0.00</td><td align="center" valign="middle" >98.74 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.16 &#177; 0.02</td><td align="center" valign="middle"  colspan="2"  >98.08 &#177; 0.02</td><td align="center" valign="middle" >96.19 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.02 &#177; 0.03</td><td align="center" valign="middle"  colspan="2"  >97.67 &#177; 0.04</td><td align="center" valign="middle" >95.16 &#177; 0.04</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.03</td><td align="center" valign="middle"  colspan="2"  >95.18 &#177; 0.01</td><td align="center" valign="middle"  colspan="2"  >92.58 &#177; 0.00</td><td align="center" valign="middle" >90.14 &#177; 0.05</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Z-direction</td><td align="center" valign="middle" >3 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.92 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.71 &#177; 0.00</td><td align="center" valign="middle" >99.26 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.90 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.66 &#177; 0.00</td><td align="center" valign="middle" >99.11 &#177; 0.00</td></tr><tr><td align="center" valign="middle" >2 mm/2%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.74 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.27 &#177; 0.00</td><td align="center" valign="middle" >98.15 &#177; 0.02</td></tr><tr><td align="center" valign="middle" >1 mm/1%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >99.00 &#177; 0.02</td><td align="center" valign="middle"  colspan="2"  >97.00 &#177; 0.03</td><td align="center" valign="middle" >94.77 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.5 mm/0.5%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.04</td><td align="center" valign="middle"  colspan="2"  >96.07 &#177; 0.01</td><td align="center" valign="middle"  colspan="2"  >93.02 &#177; 0.01</td><td align="center" valign="middle" >91.00 &#177; 0.01</td></tr><tr><td align="center" valign="middle" >0.3 mm/0.3%</td><td align="center" valign="middle"  colspan="2"  >100 &#177; 0.00</td><td align="center" valign="middle"  colspan="2"  >93.77 &#177; 0.04</td><td align="center" valign="middle"  colspan="2"  >91.02 &#177; 0.04</td><td align="center" valign="middle" >89.09 &#177; 0.04</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap></table-wrap-group></sec></sec><sec id="s4"><title>4. Discussion</title><p>This study showed that body movement can be detected by setting tolerance to 0.3 mm/0.3% even with 3 mm shift using in-treatment assessment. In other words, it is possible to detect movement and shape change using in-treatment assessment.</p><p>However, in-treatment assessment can automatically send data to a stand-alone workstation when treatment is complete and can then be analyzed. If treatment is not complete, it cannot be analyzed. Therefore, current systems cannot manage in real time. In the future, if a system that can display sinograms in real time and output analysis results simultaneously is implemented, management during treatment in real time will be possible.</p><p>If the first reference image is an image that contains many errors, all subsequent data will continue to generate errors. Therefore, in order to use in-treatment assessment, it is considered that selection of a reference image needs attention.</p><p>In this study, we used a rigid pelvic phantom. In actual treatment, the patient’s body shape may change, and gas in the abdominal cavity may move. This study did not take into account changes in the body shape or gas in the abdominal cavity. Therefore, the analysis results in the clinic will include more uncertainty, and it is expected that a larger error will occur. Therefore, in the future, it is necessary to evaluate during treatment of body shape changes from clinical data, not phantom studies.</p><p>This in-treatment assessment confirms the variation from the first reference sinogram. Additionally, a system is also being developed to calculate and evaluate the dose distribution in the body using in vivo calculated images that have been generated [<xref ref-type="bibr" rid="scirp.96372-ref24">24</xref>]. In this software, the sinogram is deconvoluted by a kernel specifically adapted to the MVCT detector to obtain the corresponding primary treatment fluence map. Using this, a dose distribution in the body is created from the planned CT image of the patient. It is also necessary to predict clinical impact while using such software simultaneously.</p><p>In this study, we proved that using in-treatment assessment can capture movement during treatment. In the future, if a system that can display sinograms in real time and output analysis results simultaneously is implemented, management during treatment in real time will be possible. If possible, the uncertainty during treatment can be reduced and reliable radiation therapy can be performed.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In-treatment assessment provides high detection sensitivity, and is a powerful tool that can manage body movement during treatment.</p></sec><sec id="s6"><title>Acknowledgements</title><p>We would like to thank DMC Corp. (https://dmed.co.jp/) for English language editing.</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Tarutani, K., Tanooka, M., Sano, K., Wataru, O., Fujiwara, M. and Yamakado, K. (2019) Evaluation of Delivery Analysis to Detect Intrafractional Motion during Tomotherapy. International Journal of Medical Physics, Clinical Engineering and Radiation Oncology, 8, 225-235. https://doi.org/10.4236/ijmpcero.2019.84020</p></sec></body><back><ref-list><title>References</title><ref id="scirp.96372-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Staffurth, J. 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