{"title":"用于碳离子疗法实验范围验证的二次粒子强度","authors":"Chuan Huang , Zhiguo Xu , Zulong Zhao , Yongzhi Yin , Xiulin Zhang , Xiyu Qiu , Peng Ma , Haibo Peng","doi":"10.1016/j.nimb.2024.165464","DOIUrl":null,"url":null,"abstract":"<div><p>Range uncertainty that reduces the dosimetric advantage of carbon ion therapy is a major problem limiting its treatment precision. To address this issue, high-precision monitoring of the in-beam range is essential. This paper proposes a method for range verification using a secondary particle intensity (SPI) system consisting of a cerium bromide (CeBr<sub>3</sub>) scintillation detector and an integrated ionization chamber (IC). This method uses the secondary particle intensity produced by the primary particles per monitor unit (MU) observed by the SPI system to convert the carbon ion range. Secondary particles, including gamma rays, neutrons, and charged particles, can be detected in the CeBr<sub>3</sub> detector as long as their signal exceeds the threshold, and no discrimination by particle type is required. The Heavy Ion Medical Machine (HIMM) terminal, situated in Lanzhou, China, provided the <sup>12</sup>C<sup>6+</sup> beam with energies ranging from 160.86 to 211.44 MeV/u. The experiment demonstrated that the carbon ion range accuracy of the <sup>12</sup>C<sup>6+</sup> beam in a polymethyl methacrylate (PMMA) target can reach 0.92 ± 0.67 mm under a 10 ms measurement period. The secondary particle energy spectrum was recorded during both the in-beam and off-beam phases, clearly recognizing the 511 keV annihilation photopeak with a full width at half maximum (FWHM) of 31.37 keV. The photopeak of annihilation confirmed the accumulation of activated products. During the 15 min continuous irradiation process, the effect of activated product accumulation on the range verification is about 1.15 mm. This paper illustrates the feasibility of SPI method for fast measurement of carbon ion range, which could potentially reduce the effects of range uncertainty in carbon ion therapy.</p></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"555 ","pages":"Article 165464"},"PeriodicalIF":1.4000,"publicationDate":"2024-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0168583X24002349/pdfft?md5=8d85b4dc146e59dc8881457d9d36ae68&pid=1-s2.0-S0168583X24002349-main.pdf","citationCount":"0","resultStr":"{\"title\":\"Secondary particle intensity for experimental range verification in carbon ion therapy\",\"authors\":\"Chuan Huang , Zhiguo Xu , Zulong Zhao , Yongzhi Yin , Xiulin Zhang , Xiyu Qiu , Peng Ma , Haibo Peng\",\"doi\":\"10.1016/j.nimb.2024.165464\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Range uncertainty that reduces the dosimetric advantage of carbon ion therapy is a major problem limiting its treatment precision. To address this issue, high-precision monitoring of the in-beam range is essential. This paper proposes a method for range verification using a secondary particle intensity (SPI) system consisting of a cerium bromide (CeBr<sub>3</sub>) scintillation detector and an integrated ionization chamber (IC). This method uses the secondary particle intensity produced by the primary particles per monitor unit (MU) observed by the SPI system to convert the carbon ion range. Secondary particles, including gamma rays, neutrons, and charged particles, can be detected in the CeBr<sub>3</sub> detector as long as their signal exceeds the threshold, and no discrimination by particle type is required. The Heavy Ion Medical Machine (HIMM) terminal, situated in Lanzhou, China, provided the <sup>12</sup>C<sup>6+</sup> beam with energies ranging from 160.86 to 211.44 MeV/u. The experiment demonstrated that the carbon ion range accuracy of the <sup>12</sup>C<sup>6+</sup> beam in a polymethyl methacrylate (PMMA) target can reach 0.92 ± 0.67 mm under a 10 ms measurement period. The secondary particle energy spectrum was recorded during both the in-beam and off-beam phases, clearly recognizing the 511 keV annihilation photopeak with a full width at half maximum (FWHM) of 31.37 keV. The photopeak of annihilation confirmed the accumulation of activated products. During the 15 min continuous irradiation process, the effect of activated product accumulation on the range verification is about 1.15 mm. This paper illustrates the feasibility of SPI method for fast measurement of carbon ion range, which could potentially reduce the effects of range uncertainty in carbon ion therapy.</p></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"555 \",\"pages\":\"Article 165464\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2024-07-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S0168583X24002349/pdfft?md5=8d85b4dc146e59dc8881457d9d36ae68&pid=1-s2.0-S0168583X24002349-main.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168583X24002349\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168583X24002349","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
Secondary particle intensity for experimental range verification in carbon ion therapy
Range uncertainty that reduces the dosimetric advantage of carbon ion therapy is a major problem limiting its treatment precision. To address this issue, high-precision monitoring of the in-beam range is essential. This paper proposes a method for range verification using a secondary particle intensity (SPI) system consisting of a cerium bromide (CeBr3) scintillation detector and an integrated ionization chamber (IC). This method uses the secondary particle intensity produced by the primary particles per monitor unit (MU) observed by the SPI system to convert the carbon ion range. Secondary particles, including gamma rays, neutrons, and charged particles, can be detected in the CeBr3 detector as long as their signal exceeds the threshold, and no discrimination by particle type is required. The Heavy Ion Medical Machine (HIMM) terminal, situated in Lanzhou, China, provided the 12C6+ beam with energies ranging from 160.86 to 211.44 MeV/u. The experiment demonstrated that the carbon ion range accuracy of the 12C6+ beam in a polymethyl methacrylate (PMMA) target can reach 0.92 ± 0.67 mm under a 10 ms measurement period. The secondary particle energy spectrum was recorded during both the in-beam and off-beam phases, clearly recognizing the 511 keV annihilation photopeak with a full width at half maximum (FWHM) of 31.37 keV. The photopeak of annihilation confirmed the accumulation of activated products. During the 15 min continuous irradiation process, the effect of activated product accumulation on the range verification is about 1.15 mm. This paper illustrates the feasibility of SPI method for fast measurement of carbon ion range, which could potentially reduce the effects of range uncertainty in carbon ion therapy.
期刊介绍:
Section B of Nuclear Instruments and Methods in Physics Research covers all aspects of the interaction of energetic beams with atoms, molecules and aggregate forms of matter. This includes ion beam analysis and ion beam modification of materials as well as basic data of importance for these studies. Topics of general interest include: atomic collisions in solids, particle channelling, all aspects of collision cascades, the modification of materials by energetic beams, ion implantation, irradiation - induced changes in materials, the physics and chemistry of beam interactions and the analysis of materials by all forms of energetic radiation. Modification by ion, laser and electron beams for the study of electronic materials, metals, ceramics, insulators, polymers and other important and new materials systems are included. Related studies, such as the application of ion beam analysis to biological, archaeological and geological samples as well as applications to solve problems in planetary science are also welcome. Energetic beams of interest include atomic and molecular ions, neutrons, positrons and muons, plasmas directed at surfaces, electron and photon beams, including laser treated surfaces and studies of solids by photon radiation from rotating anodes, synchrotrons, etc. In addition, the interaction between various forms of radiation and radiation-induced deposition processes are relevant.