{"title":"Real-time measurement of two-dimensional LET distributions of proton beams using scintillators.","authors":"Taiki Isomura, Satoshi Kamizawa, Kenta Takada, Yutaro Mori, Takeji Sakae","doi":"10.1088/1361-6560/ad8546","DOIUrl":null,"url":null,"abstract":"<p><p><i>Objective.</i>The linear energy transfer (LET) of proton therapy beams increases rapidly from the Bragg peak to the end of the beam. Although the LET can be determined using analytical or computational methods, a technique for efficiently measuring its spatial distribution has not yet been established. Thus, the purpose of this study is to develop a technique to measure the two-dimensional LET distribution in proton therapy in real time using a combination of multiple scintillators with different quenching.<i>Approach.</i>Inorganic and organic scintillator sheets were layered and irradiated with proton beams. Two-color signals of the CMOS sensor were obtained from the scintillation light and calibration curves were generated using LET. LET was calculated using Monte Carlo simulations asLETtandLETdweighted by fluence and dose, respectively. The accuracy of the calibration curve was evaluated by comparing the calculated and measured LET values for the 200 MeV monoenergetic and spread-out Bragg peak (SOBP) beams. LET distributions were obtained from the calibration curves.<i>Main results.</i>The deviation between the calculated and measured LET values was evaluated. For bothLETtandLETd, the deviation in the plateau region of the monoenergetic and SOBP beams tended to be larger than those in the peak region. The deviation was smaller forLETd. In the obtainedLETddistribution, the deviation between the calculated and measured values agreed within 3% in the peak region, while the deviation was larger in other regions.<i>Significance.</i>The LET distribution can be measured with a single irradiation using two scintillator sheets. This method may be effective for verifying LET in daily clinical practice and for quality control.</p>","PeriodicalId":20185,"journal":{"name":"Physics in medicine and biology","volume":" ","pages":""},"PeriodicalIF":3.3000,"publicationDate":"2024-10-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics in medicine and biology","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1088/1361-6560/ad8546","RegionNum":3,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, BIOMEDICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Objective.The linear energy transfer (LET) of proton therapy beams increases rapidly from the Bragg peak to the end of the beam. Although the LET can be determined using analytical or computational methods, a technique for efficiently measuring its spatial distribution has not yet been established. Thus, the purpose of this study is to develop a technique to measure the two-dimensional LET distribution in proton therapy in real time using a combination of multiple scintillators with different quenching.Approach.Inorganic and organic scintillator sheets were layered and irradiated with proton beams. Two-color signals of the CMOS sensor were obtained from the scintillation light and calibration curves were generated using LET. LET was calculated using Monte Carlo simulations asLETtandLETdweighted by fluence and dose, respectively. The accuracy of the calibration curve was evaluated by comparing the calculated and measured LET values for the 200 MeV monoenergetic and spread-out Bragg peak (SOBP) beams. LET distributions were obtained from the calibration curves.Main results.The deviation between the calculated and measured LET values was evaluated. For bothLETtandLETd, the deviation in the plateau region of the monoenergetic and SOBP beams tended to be larger than those in the peak region. The deviation was smaller forLETd. In the obtainedLETddistribution, the deviation between the calculated and measured values agreed within 3% in the peak region, while the deviation was larger in other regions.Significance.The LET distribution can be measured with a single irradiation using two scintillator sheets. This method may be effective for verifying LET in daily clinical practice and for quality control.
目的:
质子治疗光束的线性能量传递(LET)从布拉格峰到光束末端迅速增加。虽然 LET 可以通过分析或计算方法确定,但有效测量其空间分布的技术尚未建立。因此,本研究的目的是开发一种技术,利用多种不同淬火闪烁体的组合,实时测量质子治疗中的二维 LET 分布:方法:将无机和有机闪烁体薄片分层并用质子束照射。通过闪烁光获得 CMOS 传感器的双色信号,并利用 LET 生成校准曲线。LET 是通过蒙特卡洛模拟计算得出的,LETt 和 LETd 分别按通量和剂量加权。通过比较 200 MeV 单能量光束和扩散布拉格峰(SOBP)光束的计算值和测量值,评估了校准曲线的准确性。主要结果:
评估了计算和测量 LET 值之间的偏差。对于 LETt 和 LETd,单能光束和 SOBP 光束在高原区的偏差往往大于峰值区的偏差。LETd 的偏差较小。在得到的 LETd 分布中,峰值区域的计算值与测量值的偏差在 3% 以内,而其他区域的偏差较大:意义:使用两片闪烁片进行一次辐照即可测量出 LET 分布。意义:使用两片闪烁板,一次照射即可测量出 LET 分布,该方法可有效验证日常临床实践和质量控制中的 LET。
期刊介绍:
The development and application of theoretical, computational and experimental physics to medicine, physiology and biology. Topics covered are: therapy physics (including ionizing and non-ionizing radiation); biomedical imaging (e.g. x-ray, magnetic resonance, ultrasound, optical and nuclear imaging); image-guided interventions; image reconstruction and analysis (including kinetic modelling); artificial intelligence in biomedical physics and analysis; nanoparticles in imaging and therapy; radiobiology; radiation protection and patient dose monitoring; radiation dosimetry