<?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.2021.102006</article-id><article-id pub-id-type="publisher-id">IJMPCERO-109238</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>
 
 
  A Novel Technique to Validate Dosimetry for Single-Isocenter Multiple-Target VMAT Stereotactic Radiosurgery
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yulin</surname><given-names>Song</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>Miao</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Laszlo</surname><given-names>Voros</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaoli</surname><given-names>Tang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ziad</surname><given-names>Saleh</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Weixing</surname><given-names>Cai</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jeho</surname><given-names>Jeong</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Boris</surname><given-names>Mueller</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>Borys</surname><given-names>Mychalczak</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Radiation Oncology, Memorial Sloan Kettering Cancer Center, New York, USA</addr-line></aff><aff id="aff1"><addr-line>Department of Medical Physics, Memorial Sloan Kettering Cancer Center, New York, USA</addr-line></aff><pub-date pub-type="epub"><day>18</day><month>05</month><year>2021</year></pub-date><volume>10</volume><issue>02</issue><fpage>59</fpage><lpage>68</lpage><history><date date-type="received"><day>25,</day>	<month>March</month>	<year>2021</year></date><date date-type="rev-recd"><day>21,</day>	<month>May</month>	<year>2021</year>	</date><date date-type="accepted"><day>24,</day>	<month>May</month>	<year>2021</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>
 
 
  
    Each year, 170,000 cancer patients in the United States develop brain metastases. Many of them present with multiple small lesions. Historically, Linac-based stereotactic radiosurgery (SRS) was used to treat single solitary brain metastasis with a diameter of less than 3.0 cm, while whole brain radiation therapy (WBRT) was used to treat multiple brain metastases mainly as palliative therapy. Evidence-based practices reveal that WBRT results in poor treatment outcomes, with high local recurrence rates, decreased cognitive function, and even the onset of dementia. Recently, volumetric modulated arc therapy (VMAT) SRS has been tested as an alternative treatment to WBRT. Owing to its inherent complexity and high risk, it is imperative to perform rigorous testing prior to its clinical implementation. In this paper, we present a novel technique for dosimetry validation of VMAT SRS. 
  
 
</p></abstract><kwd-group><kwd>Brain Metastasis</kwd><kwd> VMAT</kwd><kwd> SRS</kwd><kwd> WBRT</kwd><kwd> Film Dosimetry</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It is estimated that about 24% - 45% of all American cancer patients have brain metastases [<xref ref-type="bibr" rid="scirp.109238-ref1">1</xref>]. As patients survive longer, multiple brain metastases are becoming more prevalent. One theory is that more effective systemic therapies may translate into an increase in brain metastases because chemotherapeutic agents do not penetrate the blood-brain barrier (BBB) [<xref ref-type="bibr" rid="scirp.109238-ref2">2</xref>]. These patients often present with subacute symptoms, such as headaches, nausea, vomiting, seizures, cognitive changes, motor dysfunction, and photophobia, depending on the location of metastases [<xref ref-type="bibr" rid="scirp.109238-ref3">3</xref>]. Currently, the most effective non-invasive treatment to relieve these symptoms is stereotactic radiosurgery (SRS) [<xref ref-type="bibr" rid="scirp.109238-ref4">4</xref>]. Traditionally, SRS has been used to treat solitary brain metastases. With the advent of volumetric modulated arc therapy (VMAT), there is growing interest in using VMAT SRS to treat multiple brain targets simultaneously with one single-isocenter plan [<xref ref-type="bibr" rid="scirp.109238-ref5">5</xref>]. This technique has several advantages over the conventional one target-one plan paradigm, including shortened treatment time and reduced integral dose to the normal brain tissue. However, the risk associated with VMAT SRS is also elevated if the precision of the delivery system and auxiliary imaging systems is compromised. One contributing factor to this risk is patient rotation-induced geometric misalignment between the actual treatment field aperture and planned field aperture. This arises from the fact that the isocenter of the delivery system can only be placed at one target center. The remaining targets, therefore, become off-isocenter. Dosimetric perturbation by geometric misalignment is negligible for the one target-one plan technique. This is because most brain metastases have a spherical shape, making them relatively immune to patient rotation in terms of delivered dosimetry. However, in the case of VMAT SRS, the magnitude of geometric misalignment is significantly amplified. It is roughly linearly proportional to the distance between the target center and the isocenter, the patient rotation angles, target distribution, and the target size and shape. Therefore, it is crucial to validate the delivered off-isocenter dosimetry for VMAT SRS prior to its clinical implementation. For this purpose, we have developed a novel, but the practical technique that can be easily reproduced in small community radiation oncology centers. In this paper, we present its detailed clinical implementation.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Dosimetry Verification Phantom</title><p>We used the commercial STEEV Stereotactic End-to-End Verification Phantom (CIRS, Norfolk, Virginia) for dosimetry validation. The STEEV phantom is made of tissue-equivalent materials. Their linear attenuation coefficients are within 1% of actual attenuation for soft tissue and bone. The STEEV phantom contains a 64 &#215; 64 &#215; 64 mm film insert in a rectangular brain cavity as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The cubic film insert has a 30-mm diameter build-in spherical target with +5% contrast. Thus, it appears much brighter than the surrounding material in CT scans. This feature greatly facilitates target delineation. A CIRS Precision Cut EBT3 film can be precisely positioned in the center plane of the target and locked by four pins. The pins prevent the film from moving and being misaligned with the insert edges. The film insert is assembled using four pinholes. The STEEV phantom has several external marks, making phantom setup quick, easy, and reproducible. Before inserting the film into the insert, the film should be marked with correct orientation so that the correct film orientation can be restored during film scanning and post-scanning analysis.</p></sec><sec id="s2_2"><title>2.2. Treatment Planning with Eclipse</title><p>A VMAT SRS verification plan was computed with Eclipse using our VMAT SRS beam model. The model was specifically developed for small target (≥10 mm) dose calculation for TrueBeam linear accelerators equipped with M120 leaf model (Varian Medical Systems, Palo Alto, California, USA). The verification plan consisted of three spherical planning target volumes (PTV) of 12 mm in diameter. The central PTV was located at the Linac isocenter. The two peripheral PTVs were located in the coronal and sagittal planes through the isocenter along the film diagonal direction. There are two primary advantages of this particular PTV distribution: 1) increased distances among PTVs and 2) the higher isodose lines being confined within the film. The PTV center-to-center separation was 20 mm (<xref ref-type="fig" rid="fig2">Figure 2</xref>). The verification plan contained two co-planar long arcs and three non-coplanar short arcs (<xref ref-type="fig" rid="fig3">Figure 3</xref>). All arcs were equally spaced. The plan prescription dose was 1600 cGy, an optimal choice between the response characteristics of EBT3 film and a realistic clinical SRS dose. The volumetric dose calculation was performed with 6&#215; photons using a special SRS small field beam model developed by our department. The prescription dose was normalized to 100% isodose line, a paradigm shift from the traditional 80% normalization methodology.</p></sec><sec id="s2_3"><title>2.3. EBT3 Film Calibration</title><p>EBT3 film strips were calibrated with a 7-point geometric scheme. The 7-dose levels were calculated with FilmQA Pro 2017 with the maximum plan dose as input. This method greatly improved the measurement efficiency and minimized the response uncertainty at high dose region. Its basic principle was that each next higher dose level was 1.4 times the previous one.</p><p>Three slabs of 5.0 cm solid water were used in the film calibration. The calibration film was sandwiched in between two slabs of 5.0 cm solid water at 100 cm away from the Linac radiation source. The jaw and MLC were set to 3.0 &#215; 3.0 cm. The calibration film strips were exposed according to the pre-determined 7 dose levels. An unexposed film strip was reserved and used as zero dose exposure. In addition, one piece of film was delivered to 1600 cGy with a field size of 3.0 &#215; 3.0 cm at the same depth for the purpose of calibration validation.</p></sec><sec id="s2_4"><title>2.4. Film Dosimetry Measurement</title><p>The film dosimetry was performed on the latest model TrueBeam Linac equipped with a 6-degrees of freedom (6-DOF) couch (Varian Medical Systems, Palo Alto, CA, USA). The 6-DOF couch is capable of achieving a precision of 0.1 mm in translational shifts and 0.1˚ in rotational shifts. The TrueBeam Linac also has the latest version of the Optical Surface Monitoring System (OSMS). It is an ideal choice for performing both conventional radiotherapy and Linac-based SRS. Prior to film dosimetry measurement, the STEEV SRS phantom was initially aligned with the OSMS to within an accuracy of 1.0 mm in translational shifts and 1.0˚ in rotational shifts and then further fine-aligned with the on-board cone beam CT (CBCT). The CBCT scan was acquired with a high-quality head protocol. The slice thickness was 1.0 mm with a matrix size of 512 &#215; 512. A suitable volume of interest (VOI) was selected for the 3D/3D registration. Mutual information-based auto-registration was then performed for phantom shift calculation. After the shift corrections were applied, a second CBCT scan was acquired to confirm the accuracy of the phantom setup. The plan was then delivered in clinical mode.</p></sec><sec id="s2_5"><title>2.5. Film Dosimetry Analysis</title><p>After a 24-hour color stabilization period, the exposed EBT3 film strips were scanned with a resolution of 450 dpi and initially processed with one-scan protocol using FilmQA Pro 2017. The choice of scanning resolution was crucial because 450 dpi provided target localization accuracy up to 0.056 mm. The dose maps were exported in TIFF format and then analyzed with our in-house film dosimetry analysis software.</p></sec></sec><sec id="s3"><title>3. Results</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the planned (right) and measured film (left) dose distributions in the coronal plane, respectively. The red crosshair in the middle of the PTV1 dose distributions was the Linac isocenter. The grid resolution was 2.0 mm. As EBT3 films were very noisy in the high dose region, a 5 &#215; 5 smoothing filter was applied to the dose maps in order to enhance the signal-to-noise ratio (SNR) of the data. <xref ref-type="fig" rid="fig5">Figure 5</xref> is the overlay of the two dose distributions. The solid curve</p><p>represents the planned dose distribution and the dotted curve represents the measured film dose distribution. The two dose distributions reveal a high degree of dosimetric congruence, in particular, in the high dose region of clinical interest inside the targets. In the area outside the targets, as indicated by the 100% isodose line (cyan color), the two dose distributions still match quite well. Even in the area distant to the targets (near film edges), the geometric agreement between the two distributions is still within our institutional tolerance. The mean spatial separation between the two distributions is less than 1.0 mm, with the measured film dose distribution being slightly smaller at the lower isodose lines (lower than 40%). This is consistent with our past observations in film dosimetry measurements for single target SRS plans calculated with iPlan (BrainLab, Germany).</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows representative dose profiles for PTV1 along the x-axis (left) and y-axis (right), respectively. The white line is the film dosimetry. The white vertical lines indicate the film edges, where the measured isodose lines stop abruptly. Even though the target is quite small, an excellent profile agreement is achieved inside the target. <xref ref-type="fig" rid="fig7">Figure 7</xref> shows representative dose profiles for PTV2. In this case, PTV2 is 20 mm away from the Linac isocenter. Again, we observe an excellent agreement between the two profiles, even in the low dose regions at the film edges.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows the planned (right) and measured film (left) dose distributions in the sagittal plane, respectively. <xref ref-type="fig" rid="fig9">Figure 9</xref> is the overlay of the two dose distributions. The sagittal plane demonstrates the same characteristics of dosimetric and geometric congruence as the coronal plane. <xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows representative dose profiles for PTV1 along the x-axis (left) and y-axis (right), respectively. <xref ref-type="fig" rid="fig1">Figure 1</xref>1 shows representative dose profiles for PTV3 along the x-axis (left) and y-axis (right), respectively.</p><p><xref ref-type="table" rid="table1">Table 1</xref> (upper) shows the mean dose differences between planned and measured film dose distributions in 90% of the region of the interest (ROI). The dosimetric significance of the 90% ROI is that it is slightly larger (~0.75 mm) than the PTV radius and covers the most clinically relevant part of the treatment</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Mean dose differences (upper), γ pass rates (middle), and target localization uncertainties (lower)</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle" >ROI</th><th align="center" valign="middle" >Mean Film Dose (cGy)</th><th align="center" valign="middle" >Mean Eclipse Dose (cGy)</th><th align="center" valign="middle" >Dose Diff (%)</th></tr></thead><tr><td align="center" valign="middle" >90% (Coronal)</td><td align="center" valign="middle" >1788.34</td><td align="center" valign="middle" >1757.58</td><td align="center" valign="middle" >1.750%</td></tr><tr><td align="center" valign="middle" >90% (Sagittal)</td><td align="center" valign="middle" >1753.08</td><td align="center" valign="middle" >1748.85</td><td align="center" valign="middle" >0.242%</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle" >ROI</th><th align="center" valign="middle" >Plan</th><th align="center" valign="middle" >γ-Pass Rate 2% (2 mm)</th></tr></thead><tr><td align="center" valign="middle" >90%</td><td align="center" valign="middle" >Coronal</td><td align="center" valign="middle" >99.86%</td></tr><tr><td align="center" valign="middle" >90%</td><td align="center" valign="middle" >Sagittal</td><td align="center" valign="middle" >99.48%</td></tr></tbody></table></table-wrap><table-wrap id="1_3"><table><tbody><thead><tr><th align="center" valign="middle" >Plane</th><th align="center" valign="middle" >Uncertainty (mm)</th></tr></thead><tr><td align="center" valign="middle" >Anterior-Posterior</td><td align="center" valign="middle" >0.1236</td></tr><tr><td align="center" valign="middle" >Right-Left</td><td align="center" valign="middle" >−0.3133</td></tr><tr><td align="center" valign="middle" >Superior-Inferior</td><td align="center" valign="middle" >−0.5511</td></tr></tbody></table></table-wrap></table-wrap-group><p>volume. In this dosimetry verification test, the mean dose difference for the two planes is 0.996%. <xref ref-type="table" rid="table1">Table 1</xref> (middle) lists the γ pass rates calculated in the 90% ROI with criteria of 2% and 2.0 mm. <xref ref-type="table" rid="table1">Table 1</xref> (lower) lists the target localization uncertainties in the three anatomical directions, determined from the film dosimetry analysis. Our institutional tolerance is less than 1.0 mm.</p></sec><sec id="s4"><title>4. Discussion and Conclusions</title><p>Currently, the primary treatment options for patients with brain metastases include systemic therapy, surgery, stereotactic radiosurgery, WBRT, or some combination of these. For patients with multiple small lesions (≤20, &lt;2.0 cm) or deeply seated lesions and poor performance status, the single-isocenter multiple-target VMAT SRS is an excellent treatment option. An increasing volume of clinical evidence suggests that multiple-target VMAT SRS offers significant benefits in both overall survival (OS) and quality of life (QOL) over conventional WBRT. However, the single-isocenter multiple-target VMAT SRS is a complex treatment modality. It requires that every part of the treatment hardware is tested and verified, including the treatment delivery system, auxiliary imaging systems, patient positioning system, and real-time patient tracking system. A carefully designed off-isocenter multiple target film dosimetry is the most critical component of this process.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This research was funded in part by the NIH/NCI Cancer Center Support Grant P30 CA008748.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Song, Y.L., Zhang, M., Voros, L., Tang, X.L., Saleh, Z., Cai, W.X., Jeong, J., Mueller, B. and Mychalczak, B. (2021) A Novel Technique to Validate Dosimetry for Single-Isocenter Multiple-Target VMAT Stereotactic Radiosurgery. 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