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| 001 | 178611 | ||
| 005 | 20241220120849.0 | ||
| 024 | 7 | _ | |a 10.1002/mp.15480 |2 doi |
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| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 610 |
| 100 | 1 | _ | |a Ghesquiere-Dierickx, Laura |0 P:(DE-He78)84edc78dad0b83ad6c0633bd24a0b5b7 |b 0 |e First author |u dkfz |
| 245 | _ | _ | |a Detecting perturbations of a radiation field inside a head-sized phantom exposed to therapeutic carbon-ion beams through charged-fragment tracking. |
| 260 | _ | _ | |a College Park, Md. |c 2022 |b AAPM |
| 336 | 7 | _ | |a article |2 DRIVER |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1648038787_2990 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 500 | _ | _ | |a #EA:E040#LA:E040# / 2022 Mar;49(3):1776-1792 |
| 520 | _ | _ | |a Non-invasive methods to monitor carbon-ion beams in patients are desired to fully exploit the advantages of carbon-ion radiotherapy. Prompt secondary ions produced in nuclear fragmentations of carbon ions are of particular interest for monitoring purposes as they can escape the patient, and thus be detected and tracked to measure the radiation field in the irradiated object. This study aims to evaluate the performance of secondary-ion tracking to detect, visualize and localize an internal air cavity used to mimic inter-fractional changes in the patient anatomy at different depths along the beam axis.In this work, a homogeneous head phantom was irradiated with a realistic carbon-ion treatment plan with a typical prescribed fraction dose of 3 Gy (RBE). Secondary ions were detected by a mini-tracker with an active area of 2 cm2 , based on the Timepix3 semiconductor pixel detector technology. The mini-tracker was placed 120 mm behind the center of the target at an angle of 30 degrees with respect to the beam axis. To assess the performance of the developed method, a 2-mm-thick air cavity was inserted in the head phantom at several depths: in front of as well as at the entrance, in the middle and at the distal end of the target volume. Different reconstruction methods of secondary-ion emission profile were studied using the FLUKA Monte Carlo simulation package. The perturbations in the emission profiles caused by the air cavity were analyzed to detect the presence of the air cavity and localize its position.The perturbations in the radiation field mimicked by the 2-mm-thick cavity were found to be significant. A detection significance of at least three standard deviations in terms of spatial distribution of the measured tracks was found for all investigated cavity depths, while the highest significance (6 standard deviations) was obtained when the cavity was located upstream of the tumor. For a tracker with an eight-fold sensitive area, the detection significance rose to at least 9 standard deviations, and up to 17 standard deviations respectively. The cavity could be detected at all depths and its position measured within 6.5 mm ± 1.4 mm, which is sufficient for the targeted clinical performance of 10 mm.The presented systematic study concerning the detection and localization of small inter-fractional structure changes in a realistic clinical setting demonstrates that secondary ions carry a large amount of information on the internal structure of the irradiated object, and are thus attractive to be further studied for non-invasive monitoring of carbon-ion treatments. This article is protected by copyright. All rights reserved. |
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| 650 | _ | 7 | |a carbon-ion radiotherapy |2 Other |
| 650 | _ | 7 | |a inter-fractional changes |2 Other |
| 650 | _ | 7 | |a non-invasive ion-beam monitoring |2 Other |
| 650 | _ | 7 | |a nuclear fragmentation |2 Other |
| 650 | _ | 7 | |a secondary ions |2 Other |
| 650 | _ | 7 | |a secondary-ion tracking |2 Other |
| 650 | _ | 7 | |a semiconductor pixel detector Timepix3 |2 Other |
| 700 | 1 | _ | |a Félix-Bautista, Renato |0 P:(DE-HGF)0 |b 1 |
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| 700 | 1 | _ | |a Kelleter, Laurent |0 P:(DE-He78)e37dd0bc6f3e4d55b7967219607e7d4e |b 3 |u dkfz |
| 700 | 1 | _ | |a Reimold, Marvin |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Echner, Gernot |0 P:(DE-He78)5ce5a852e39ce8846d820376eb30697e |b 5 |u dkfz |
| 700 | 1 | _ | |a Soukup, Pavel |b 6 |
| 700 | 1 | _ | |a Jäkel, Oliver |0 P:(DE-He78)440a3f62ea9ea5c63375308976fc4c44 |b 7 |u dkfz |
| 700 | 1 | _ | |a Gehrke, Tim |0 P:(DE-He78)4af90cacc534bcab08c5a70badbb2d5e |b 8 |u dkfz |
| 700 | 1 | _ | |a Martisikova, Maria |0 P:(DE-He78)dfe82ba00edb8b1609794fbe37bd616f |b 9 |e Last author |u dkfz |
| 773 | _ | _ | |a 10.1002/mp.15480 |g p. mp.15480 |0 PERI:(DE-600)1466421-5 |n 3 |p 1776-1792 |t Medical physics |v 49 |y 2022 |x 0094-2405 |
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