A portal dosimetry dose prediction method based on collapsed cone algorithm using the clinical beam model

Purpose Amorphous silicon electronical portal imaging devices (EPIDs) are widely used for dosimetric measurements in Radiation Therapy. The purpose of this work was to determine if a portal dose prediction method can be utilized for dose map calculations based on the linear accelerator model within...

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Veröffentlicht in:Medical physics (Lancaster) 2017-01, Vol.44 (1), p.333-341
Hauptverfasser: Martínez Ortega, J., Gómez González, N., Castro Tejero, P., Pinto Monedero, M., Tolani, N. B., Núñez Martín, L., Sánchez Montero, R.
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container_issue 1
container_start_page 333
container_title Medical physics (Lancaster)
container_volume 44
creator Martínez Ortega, J.
Gómez González, N.
Castro Tejero, P.
Pinto Monedero, M.
Tolani, N. B.
Núñez Martín, L.
Sánchez Montero, R.
description Purpose Amorphous silicon electronical portal imaging devices (EPIDs) are widely used for dosimetric measurements in Radiation Therapy. The purpose of this work was to determine if a portal dose prediction method can be utilized for dose map calculations based on the linear accelerator model within a commercial treatment planning system (Pinnacle3 v8.0 m). Methods The method was developed for a 6 MV photon beam on the Varian Clinac 21‐EX, at a nominal dose rate of 400 MU/min. The Varian aS1000 EPID was unmounted from the linear accelerator and scanned to acquire CT images of the EPID. The CT images were imported into Pinnacle3 and were used as a quality assurance phantom to calculate dose on the EPID setup at a source to detector distance of 105 cm. The best match of the dose distributions was obtained considering the image plane located at 106 cm from the source to detector plane. The EPID was calibrated according to the manufacturer procedure and corrections were made for output factors. Arm‐backscattering effect, based on profile correction curves, has been introduced. Five low‐modulated and three high‐modulated clinical planned treatments were predicted and measured with the method presented here and with MatriXX (IBA Dosimetry, Schwarzenbruck, Germany). Results A portal dose prediction method based on Pinnacle3 was developed without modifying the commissioned parameters of the model in use in the clinic. CT images of the EPID were acquired and used as a quality assurance phantom. The CT images indicated a mean density of 1.16 g/cm3 for the sensitive area of the EPID. Output factor measured with the EPID were lower for small fields and larger for larger fields (beyond 10 × 10 cm2). Arm‐backscatter correction showed a better agreement at the target side of the EPID. Analysis of Gamma index comparison (3%, 3 mm) indicated a minimum of 97.4% pass rate for low modulated and 98.3% for high modulated treatments. Pass rates were similar for MatriXX measurements. ConclusionsThe method developed here can be easily implemented into clinic, as neither additional modeling of the clinical energy nor an independent image prediction algorithm are necessary. The main advantage of this method is that portal dose prediction is calculated with the same algorithm and beam model used for patient dose distribution calculation. This method was independently validated with an ionization chamber matrix.
doi_str_mv 10.1002/mp.12018
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B. ; Núñez Martín, L. ; Sánchez Montero, R.</creator><creatorcontrib>Martínez Ortega, J. ; Gómez González, N. ; Castro Tejero, P. ; Pinto Monedero, M. ; Tolani, N. B. ; Núñez Martín, L. ; Sánchez Montero, R.</creatorcontrib><description>Purpose Amorphous silicon electronical portal imaging devices (EPIDs) are widely used for dosimetric measurements in Radiation Therapy. The purpose of this work was to determine if a portal dose prediction method can be utilized for dose map calculations based on the linear accelerator model within a commercial treatment planning system (Pinnacle3 v8.0 m). Methods The method was developed for a 6 MV photon beam on the Varian Clinac 21‐EX, at a nominal dose rate of 400 MU/min. The Varian aS1000 EPID was unmounted from the linear accelerator and scanned to acquire CT images of the EPID. The CT images were imported into Pinnacle3 and were used as a quality assurance phantom to calculate dose on the EPID setup at a source to detector distance of 105 cm. The best match of the dose distributions was obtained considering the image plane located at 106 cm from the source to detector plane. The EPID was calibrated according to the manufacturer procedure and corrections were made for output factors. Arm‐backscattering effect, based on profile correction curves, has been introduced. Five low‐modulated and three high‐modulated clinical planned treatments were predicted and measured with the method presented here and with MatriXX (IBA Dosimetry, Schwarzenbruck, Germany). Results A portal dose prediction method based on Pinnacle3 was developed without modifying the commissioned parameters of the model in use in the clinic. CT images of the EPID were acquired and used as a quality assurance phantom. The CT images indicated a mean density of 1.16 g/cm3 for the sensitive area of the EPID. Output factor measured with the EPID were lower for small fields and larger for larger fields (beyond 10 × 10 cm2). Arm‐backscatter correction showed a better agreement at the target side of the EPID. Analysis of Gamma index comparison (3%, 3 mm) indicated a minimum of 97.4% pass rate for low modulated and 98.3% for high modulated treatments. Pass rates were similar for MatriXX measurements. ConclusionsThe method developed here can be easily implemented into clinic, as neither additional modeling of the clinical energy nor an independent image prediction algorithm are necessary. The main advantage of this method is that portal dose prediction is calculated with the same algorithm and beam model used for patient dose distribution calculation. This method was independently validated with an ionization chamber matrix.</description><identifier>ISSN: 0094-2405</identifier><identifier>EISSN: 2473-4209</identifier><identifier>DOI: 10.1002/mp.12018</identifier><identifier>PMID: 28102946</identifier><language>eng</language><publisher>United States</publisher><subject>Algorithms ; amorphous silicon ; Calibration ; Electrical Equipment and Supplies ; EPID dosimetry ; Humans ; IMRT ; Particle Accelerators ; portal image prediction ; Radiometry - instrumentation ; Radiotherapy Planning, Computer-Assisted ; Tomography, X-Ray Computed</subject><ispartof>Medical physics (Lancaster), 2017-01, Vol.44 (1), p.333-341</ispartof><rights>2016 American Association of Physicists in Medicine</rights><rights>2016 American Association of Physicists in Medicine.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3218-7508c4f9926f58c98e013287087fc68d437da09b722c7d2ce6cbb0ea26606c9e3</citedby><cites>FETCH-LOGICAL-c3218-7508c4f9926f58c98e013287087fc68d437da09b722c7d2ce6cbb0ea26606c9e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fmp.12018$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fmp.12018$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,777,781,1413,27906,27907,45556,45557</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/28102946$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Martínez Ortega, J.</creatorcontrib><creatorcontrib>Gómez González, N.</creatorcontrib><creatorcontrib>Castro Tejero, P.</creatorcontrib><creatorcontrib>Pinto Monedero, M.</creatorcontrib><creatorcontrib>Tolani, N. B.</creatorcontrib><creatorcontrib>Núñez Martín, L.</creatorcontrib><creatorcontrib>Sánchez Montero, R.</creatorcontrib><title>A portal dosimetry dose prediction method based on collapsed cone algorithm using the clinical beam model</title><title>Medical physics (Lancaster)</title><addtitle>Med Phys</addtitle><description>Purpose Amorphous silicon electronical portal imaging devices (EPIDs) are widely used for dosimetric measurements in Radiation Therapy. The purpose of this work was to determine if a portal dose prediction method can be utilized for dose map calculations based on the linear accelerator model within a commercial treatment planning system (Pinnacle3 v8.0 m). Methods The method was developed for a 6 MV photon beam on the Varian Clinac 21‐EX, at a nominal dose rate of 400 MU/min. The Varian aS1000 EPID was unmounted from the linear accelerator and scanned to acquire CT images of the EPID. The CT images were imported into Pinnacle3 and were used as a quality assurance phantom to calculate dose on the EPID setup at a source to detector distance of 105 cm. The best match of the dose distributions was obtained considering the image plane located at 106 cm from the source to detector plane. The EPID was calibrated according to the manufacturer procedure and corrections were made for output factors. Arm‐backscattering effect, based on profile correction curves, has been introduced. Five low‐modulated and three high‐modulated clinical planned treatments were predicted and measured with the method presented here and with MatriXX (IBA Dosimetry, Schwarzenbruck, Germany). Results A portal dose prediction method based on Pinnacle3 was developed without modifying the commissioned parameters of the model in use in the clinic. CT images of the EPID were acquired and used as a quality assurance phantom. The CT images indicated a mean density of 1.16 g/cm3 for the sensitive area of the EPID. Output factor measured with the EPID were lower for small fields and larger for larger fields (beyond 10 × 10 cm2). Arm‐backscatter correction showed a better agreement at the target side of the EPID. Analysis of Gamma index comparison (3%, 3 mm) indicated a minimum of 97.4% pass rate for low modulated and 98.3% for high modulated treatments. Pass rates were similar for MatriXX measurements. ConclusionsThe method developed here can be easily implemented into clinic, as neither additional modeling of the clinical energy nor an independent image prediction algorithm are necessary. The main advantage of this method is that portal dose prediction is calculated with the same algorithm and beam model used for patient dose distribution calculation. This method was independently validated with an ionization chamber matrix.</description><subject>Algorithms</subject><subject>amorphous silicon</subject><subject>Calibration</subject><subject>Electrical Equipment and Supplies</subject><subject>EPID dosimetry</subject><subject>Humans</subject><subject>IMRT</subject><subject>Particle Accelerators</subject><subject>portal image prediction</subject><subject>Radiometry - instrumentation</subject><subject>Radiotherapy Planning, Computer-Assisted</subject><subject>Tomography, X-Ray Computed</subject><issn>0094-2405</issn><issn>2473-4209</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp1kE1LxDAQhoMoun6Av0By9FKdpG2aHBfxC1b0oOeSJlM30jQ16SL77-26fpw8zbzDw8PwEnLK4IIB8Es_XDAOTO6QGS-qPCs4qF0yA1BFxgsoD8hhSm8AIPIS9skBlwy4KsSMuDkdQhx1R21IzuMY15sN6RDROjO60NPpugyWNjqhpVM2oev0sAkm9Eh19xqiG5eerpLrX-m4RGo61zszWRvUnvpgsTsme63uEp58zyPycnP9fHWXLR5v76_mi8zknMmsKkGaolWKi7aURkkElnNZgaxaI6Qt8spqUE3FuaksNyhM0wBqLgQIozA_Iudb7xDD-wrTWHuXDE4v9xhWqWZSsLKSIld_qIkhpYhtPUTndVzXDOpNsbUf6q9iJ_Ts27pqPNpf8KfJCci2wIfrcP2vqH542go_AV0sgWA</recordid><startdate>201701</startdate><enddate>201701</enddate><creator>Martínez Ortega, J.</creator><creator>Gómez González, N.</creator><creator>Castro Tejero, P.</creator><creator>Pinto Monedero, M.</creator><creator>Tolani, N. B.</creator><creator>Núñez Martín, L.</creator><creator>Sánchez Montero, R.</creator><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>201701</creationdate><title>A portal dosimetry dose prediction method based on collapsed cone algorithm using the clinical beam model</title><author>Martínez Ortega, J. ; Gómez González, N. ; Castro Tejero, P. ; Pinto Monedero, M. ; Tolani, N. B. ; Núñez Martín, L. ; Sánchez Montero, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3218-7508c4f9926f58c98e013287087fc68d437da09b722c7d2ce6cbb0ea26606c9e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Algorithms</topic><topic>amorphous silicon</topic><topic>Calibration</topic><topic>Electrical Equipment and Supplies</topic><topic>EPID dosimetry</topic><topic>Humans</topic><topic>IMRT</topic><topic>Particle Accelerators</topic><topic>portal image prediction</topic><topic>Radiometry - instrumentation</topic><topic>Radiotherapy Planning, Computer-Assisted</topic><topic>Tomography, X-Ray Computed</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Martínez Ortega, J.</creatorcontrib><creatorcontrib>Gómez González, N.</creatorcontrib><creatorcontrib>Castro Tejero, P.</creatorcontrib><creatorcontrib>Pinto Monedero, M.</creatorcontrib><creatorcontrib>Tolani, N. B.</creatorcontrib><creatorcontrib>Núñez Martín, L.</creatorcontrib><creatorcontrib>Sánchez Montero, R.</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Medical physics (Lancaster)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Martínez Ortega, J.</au><au>Gómez González, N.</au><au>Castro Tejero, P.</au><au>Pinto Monedero, M.</au><au>Tolani, N. B.</au><au>Núñez Martín, L.</au><au>Sánchez Montero, R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A portal dosimetry dose prediction method based on collapsed cone algorithm using the clinical beam model</atitle><jtitle>Medical physics (Lancaster)</jtitle><addtitle>Med Phys</addtitle><date>2017-01</date><risdate>2017</risdate><volume>44</volume><issue>1</issue><spage>333</spage><epage>341</epage><pages>333-341</pages><issn>0094-2405</issn><eissn>2473-4209</eissn><abstract>Purpose Amorphous silicon electronical portal imaging devices (EPIDs) are widely used for dosimetric measurements in Radiation Therapy. The purpose of this work was to determine if a portal dose prediction method can be utilized for dose map calculations based on the linear accelerator model within a commercial treatment planning system (Pinnacle3 v8.0 m). Methods The method was developed for a 6 MV photon beam on the Varian Clinac 21‐EX, at a nominal dose rate of 400 MU/min. The Varian aS1000 EPID was unmounted from the linear accelerator and scanned to acquire CT images of the EPID. The CT images were imported into Pinnacle3 and were used as a quality assurance phantom to calculate dose on the EPID setup at a source to detector distance of 105 cm. The best match of the dose distributions was obtained considering the image plane located at 106 cm from the source to detector plane. The EPID was calibrated according to the manufacturer procedure and corrections were made for output factors. Arm‐backscattering effect, based on profile correction curves, has been introduced. Five low‐modulated and three high‐modulated clinical planned treatments were predicted and measured with the method presented here and with MatriXX (IBA Dosimetry, Schwarzenbruck, Germany). Results A portal dose prediction method based on Pinnacle3 was developed without modifying the commissioned parameters of the model in use in the clinic. CT images of the EPID were acquired and used as a quality assurance phantom. The CT images indicated a mean density of 1.16 g/cm3 for the sensitive area of the EPID. Output factor measured with the EPID were lower for small fields and larger for larger fields (beyond 10 × 10 cm2). Arm‐backscatter correction showed a better agreement at the target side of the EPID. Analysis of Gamma index comparison (3%, 3 mm) indicated a minimum of 97.4% pass rate for low modulated and 98.3% for high modulated treatments. Pass rates were similar for MatriXX measurements. ConclusionsThe method developed here can be easily implemented into clinic, as neither additional modeling of the clinical energy nor an independent image prediction algorithm are necessary. The main advantage of this method is that portal dose prediction is calculated with the same algorithm and beam model used for patient dose distribution calculation. This method was independently validated with an ionization chamber matrix.</abstract><cop>United States</cop><pmid>28102946</pmid><doi>10.1002/mp.12018</doi><tpages>9</tpages></addata></record>
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source MEDLINE; Wiley Online Library Journals Frontfile Complete; Alma/SFX Local Collection
subjects Algorithms
amorphous silicon
Calibration
Electrical Equipment and Supplies
EPID dosimetry
Humans
IMRT
Particle Accelerators
portal image prediction
Radiometry - instrumentation
Radiotherapy Planning, Computer-Assisted
Tomography, X-Ray Computed
title A portal dosimetry dose prediction method based on collapsed cone algorithm using the clinical beam model
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