{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,29]],"date-time":"2026-09-29T00:16:22Z","timestamp":1790640982310,"version":"4.1.0"},"reference-count":30,"publisher":"Wiley","issue":"9","license":[{"start":{"date-parts":[[2018,7,27]],"date-time":"2018-07-27T00:00:00Z","timestamp":1532649600000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"funder":[{"DOI":"10.13039\/100007210","name":"Varian Medical Systems","doi-asserted-by":"publisher","id":[{"id":"10.13039\/100007210","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["aapm.onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Medical Physics"],"published-print":{"date-parts":[[2018,9]]},"abstract":"<jats:sec><jats:title>Purpose<\/jats:title><jats:p>Although volumetric modulated arc therapy (<jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content>) is a well\u2010accepted treatment technique in radiotherapy using a coplanar delivery approach, <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> might be further improved by including dynamic table and collimator rotations leading to dynamic trajectory radiotherapy (<jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content>). In this work, an optimization procedure for <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> was developed and the potential benefit of <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> was investigated for different treatment sites.<\/jats:p><\/jats:sec><jats:sec><jats:title>Methods<\/jats:title><jats:p>For this purpose, a dedicated optimization framework for <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> was developed using the Eclipse Scripting Research Application Programming Interface (<jats:styled-content style=\"fixed-case\">ESRAPI<\/jats:styled-content>). The contours of the target and organs at risk (<jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content>s) structures were exported by applying the <jats:styled-content style=\"fixed-case\">ESRAPI<\/jats:styled-content> and were used to determine the fractional volume\u2010overlap of the <jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content>s with the target from several potential beam directions. Thereby, an additional weighting was applied taking into account the relative position of the <jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content> with respect to the target and radiation beam, that is, penalizing directions where the <jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content> is proximal to the target. The resulting two\u2010dimensional gantry\u2010table map was used as input for an A* path finding algorithm returning an optimized gantry\u2010table path. Thereby, the process is also taking into account <jats:styled-content style=\"fixed-case\">CT<\/jats:styled-content> scan length and collision restrictions. The A* algorithm was used again to determine the dynamic collimator angle path by optimizing the area between the <jats:styled-content style=\"fixed-case\">MLC<\/jats:styled-content> leaves and the target contour for each gantry\u2010table path leading to gantry\u2010collimator paths. The resulting gantry\u2010table and gantry\u2010collimator paths are combined and serve as input for the intensity modulation optimization using a research <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> optimizer and the <jats:styled-content style=\"fixed-case\">ESRAPI<\/jats:styled-content> resulting in dynamic trajectories. This procedure was evaluated for five clinically motivated cases: two head and neck, one lung, one esophagus, and one prostate. Final dose calculations were performed using the Swiss Monte Carlo Plan (<jats:styled-content style=\"fixed-case\">SMCP<\/jats:styled-content>). Resulting dose distributions for the <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> treatment plans and for the standard <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> plans were compared based on dose distributions and dose volume histogram (<jats:styled-content style=\"fixed-case\">DVH<\/jats:styled-content>) parameters. For this comparison, the dose distribution for the <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> plans were recalculated using the <jats:styled-content style=\"fixed-case\">SMCP<\/jats:styled-content>. In addition, the suitability of the delivery of a <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> treatment plan was demonstrated by means of gafchromic film measurements on a TrueBeam linear accelerator.<\/jats:p><\/jats:sec><jats:sec><jats:title>Results<\/jats:title><jats:p><jats:styled-content style=\"fixed-case\">DVH<\/jats:styled-content>s for the target volumes showed similar or improved coverage and dose homogeneity for <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> compared with <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> using equal or less number of dynamic trajectories for <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> than arcs for <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> for all cases studied. Depending on the case, improvements in mean and maximum dose for the <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> plans were achieved for almost all <jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content>s compared with the <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> plans. Improvements in <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> treatment plans for mean and maximum dose compared to <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> plans were up to 16% and 38% relative to the prescribed dose, respectively. The measured and calculated dose values resulted in a passing rate of more than 99.5% for the two\u2010dimensional gamma analysis using 2% and 2\u00a0mm criteria and a threshold of 10%.<\/jats:p><\/jats:sec><jats:sec><jats:title>Conclusions<\/jats:title><jats:p><jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> plans for different treatment sites were generated and compared with <jats:styled-content style=\"fixed-case\">VMAT<\/jats:styled-content> plans. The delivery is suitable and dose comparisons demonstrate a high potential of <jats:styled-content style=\"fixed-case\">DTRT<\/jats:styled-content> to reduce dose to <jats:styled-content style=\"fixed-case\">OAR<\/jats:styled-content>s using less dynamic trajectories than arcs, while target coverage is preserved.<\/jats:p><\/jats:sec>","DOI":"10.1002\/mp.13086","type":"journal-article","created":{"date-parts":[[2018,7,11]],"date-time":"2018-07-11T02:32:26Z","timestamp":1531276346000},"page":"4201-4212","update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":45,"title":["Part 1: Optimization and evaluation of dynamic trajectory radiotherapy"],"prefix":"10.1002","volume":"45","author":[{"given":"Michael K.","family":"Fix","sequence":"first","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Daniel","family":"Frei","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Werner","family":"Volken","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Dario","family":"Terribilini","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Silvan","family":"Mueller","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Olgun","family":"Elicin","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Hossein","family":"Hemmatazad","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Daniel M.","family":"Aebersold","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Peter","family":"Manser","sequence":"additional","affiliation":[{"name":"Division of Medical Radiation Physics Department of Radiation Oncology Inselspital, Bern University Hospital University of Bern CH\u20103010 Bern Switzerland"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"311","published-online":{"date-parts":[[2018,7,27]]},"reference":[{"key":"e_1_2_6_2_1","doi-asserted-by":"publisher","DOI":"10.1088\/0031-9155\/40\/9\/004"},{"key":"e_1_2_6_3_1","doi-asserted-by":"publisher","DOI":"10.1118\/1.597345"},{"key":"e_1_2_6_4_1","doi-asserted-by":"publisher","DOI":"10.1118\/1.2818738"},{"key":"e_1_2_6_5_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2008.12.033"},{"key":"e_1_2_6_6_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2014.09.043"},{"key":"e_1_2_6_7_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2013.02.002"},{"key":"e_1_2_6_8_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2012.09.028"},{"key":"e_1_2_6_9_1","doi-asserted-by":"publisher","DOI":"10.1186\/s13014-014-0239-x"},{"key":"e_1_2_6_10_1","doi-asserted-by":"publisher","DOI":"10.1118\/1.4917165"},{"key":"e_1_2_6_11_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2015.04.034"},{"key":"e_1_2_6_12_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.radonc.2013.10.031"},{"key":"e_1_2_6_13_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2010.03.004"},{"key":"e_1_2_6_14_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.radonc.2006.09.004"},{"key":"e_1_2_6_15_1","doi-asserted-by":"publisher","DOI":"10.1088\/0031-9155\/60\/13\/5179"},{"key":"e_1_2_6_16_1","doi-asserted-by":"publisher","DOI":"10.1088\/0031-9155\/58\/22\/8163"},{"key":"e_1_2_6_17_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.radonc.2016.07.014"},{"key":"e_1_2_6_18_1","doi-asserted-by":"publisher","DOI":"10.1118\/1.4914863"},{"key":"e_1_2_6_19_1","doi-asserted-by":"publisher","DOI":"10.1016\/0360-3016(88)90059-4"},{"key":"e_1_2_6_20_1","doi-asserted-by":"publisher","DOI":"10.1120\/jacmp.v14i1.4035"},{"key":"e_1_2_6_21_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2009.08.056"},{"key":"e_1_2_6_22_1","doi-asserted-by":"publisher","DOI":"10.1002\/mp.12648"},{"key":"e_1_2_6_23_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijrobp.2010.10.016"},{"key":"e_1_2_6_24_1","doi-asserted-by":"publisher","DOI":"10.1002\/mp.12270"},{"key":"e_1_2_6_25_1","doi-asserted-by":"publisher","DOI":"10.1088\/0031-9155\/52\/19\/N01"},{"key":"e_1_2_6_26_1","doi-asserted-by":"publisher","DOI":"10.1088\/0031-9155\/53\/19\/N01"},{"key":"e_1_2_6_27_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.zemedi.2010.10.010"},{"key":"e_1_2_6_28_1","doi-asserted-by":"publisher","DOI":"10.1016\/S0167-8140(15)30382-0"},{"key":"e_1_2_6_29_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.zemedi.2018.03.002"},{"key":"e_1_2_6_30_1","doi-asserted-by":"publisher","DOI":"10.1109\/TSSC.1968.300136"},{"key":"e_1_2_6_31_1","doi-asserted-by":"publisher","DOI":"10.1109\/IEMBS.2000.898024"}],"container-title":["Medical Physics"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1002%2Fmp.13086","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/aapm.onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/mp.13086","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,9,18]],"date-time":"2023-09-18T09:25:09Z","timestamp":1695029109000},"score":1,"resource":{"primary":{"URL":"https:\/\/aapm.onlinelibrary.wiley.com\/doi\/10.1002\/mp.13086"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2018,7,27]]},"references-count":30,"journal-issue":{"issue":"9","published-print":{"date-parts":[[2018,9]]}},"alternative-id":["10.1002\/mp.13086"],"URL":"https:\/\/doi.org\/10.1002\/mp.13086","archive":["Portico"],"relation":{},"ISSN":["0094-2405","2473-4209"],"issn-type":[{"value":"0094-2405","type":"print"},{"value":"2473-4209","type":"electronic"}],"subject":[],"published":{"date-parts":[[2018,7,27]]},"assertion":[{"value":"2018-03-09","order":0,"name":"received","label":"Received","group":{"name":"publication_history","label":"Publication History"}},{"value":"2018-06-28","order":1,"name":"accepted","label":"Accepted","group":{"name":"publication_history","label":"Publication History"}},{"value":"2018-07-27","order":2,"name":"published","label":"Published","group":{"name":"publication_history","label":"Publication History"}}]}}