Department of Physics, University of Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy. Istituto Nazionale di Fisica Nucleare, Sezione di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.
Phys Med Biol. 2014 Jan 6;59(1):43-60. doi: 10.1088/0031-9155/59/1/43. Epub 2013 Dec 10.
During particle therapy irradiation, positron emitters with half-lives ranging from 2 to 20 min are generated from nuclear processes. The half-lives are such that it is possible either to detect the positron signal in the treatment room using an in-beam positron emission tomography (PET) system, right after the irradiation, or to quickly transfer the patient to a close PET/CT scanner. Since the activity distribution is spatially correlated with the dose, it is possible to use PET imaging as an indirect method to assure the quality of the dose delivery. In this work, we present a new dedicated PET system able to operate in-beam. The PET apparatus consists in two 10 cm × 10 cm detector heads. Each detector is composed of four scintillating matrices of 23 × 23 LYSO crystals. The crystal size is 1.9 mm × 1.9 mm × 16 mm. Each scintillation matrix is read out independently with a modularized acquisition system. The distance between the two opposing detector heads was set to 20 cm. The system has very low dead time per detector area and a 3 ns coincidence window, which is capable to sustain high single count rates and to keep the random counts relatively low. This allows a new full-beam monitoring modality that includes data acquisition also while the beam is on. The PET system was tested during the irradiation at the CATANA (INFN, Catania, Italy) cyclotron-based proton therapy facility. Four acquisitions with different doses and dose rates were analysed. In all cases the random to total coincidences ratio was equal or less than 25%. For each measurement we estimated the accuracy and precision of the activity range on a set of voxel lines within an irradiated PMMA phantom. Results show that the inclusion of data acquired during the irradiation, referred to as beam-on data, improves both the precision and accuracy of the range measurement with respect to data acquired only after irradiation. Beam-on data alone are enough to give precisions better than 1 mm when at least 5 Gy are delivered.
在粒子治疗照射过程中,会从核过程中产生半衰期在 2 至 20 分钟之间的正电子发射体。半衰期如此之短,以至于可以在照射后立即使用射束内正电子发射断层扫描(PET)系统在治疗室内检测正电子信号,或者迅速将患者转移到近距离 PET/CT 扫描仪。由于活性分布与剂量在空间上相关,因此可以使用 PET 成像作为间接方法来确保剂量输送的质量。在这项工作中,我们提出了一种新的专用 PET 系统,能够在射束内运行。PET 仪器由两个 10cm×10cm 的探测器头组成。每个探测器由四个闪烁矩阵组成,每个闪烁矩阵由 23×23 的 LYSO 晶体组成。晶体尺寸为 1.9mm×1.9mm×16mm。每个闪烁矩阵都使用模块化采集系统独立读取。两个相对的探测器头之间的距离设置为 20cm。该系统每个探测器面积的死时间非常低,符合 3ns 的符合时间窗口,能够承受高单计数率并保持相对较低的随机计数。这允许使用一种新的全束监测模式,包括在束流开启时也进行数据采集。在意大利卡塔尼亚的 CATANA(INFN)回旋加速器质子治疗设施的照射过程中对 PET 系统进行了测试。分析了具有不同剂量和剂量率的四次采集。在所有情况下,随机符合与总符合的比率都等于或小于 25%。对于每次测量,我们在照射 PMMA 体模内的一组体素线上估计了活性范围的准确性和精度。结果表明,与仅在照射后采集的数据相比,包括照射期间采集的数据(称为束流开启数据)可以提高范围测量的精度和准确性。仅使用束流开启数据,当输送至少 5Gy 时,就足以获得精度优于 1mm 的结果。