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In-beam PET imaging for on-line adaptive proton therapy: An initial phantom study

机译:在线自适应质子治疗的束流PET成像:初始幻像研究

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We developed and investigated a positron emission tomography (PET) system for use with on-line (both in-beam and intra-fraction) image-guided adaptive proton therapy applications. The PET has dual rotating depth-of-interaction measurable detector panels by using solid-state photomultiplier (SSPM) arrays and LYSO scintillators. It has a 44mm diameter trans-axial and 30mm axial field-of-view (FOV). A 38mm diameter polymethyl methacrylate phantom was placed inside the FOV. Both PET and phantom axes were aligned with a collimated 179.2 MeV beam. Each beam delivered ~50 spills (0.5s spill and 1.5s inter-spill time, 3.8 Gy at Bragg peak). Data from each beam were acquired with detectors at a given angle. Nine datasets for nine beams with detectors at nine different angles over 180 were acquired for full-tomographic imaging. Each dataset included data both during and 5min after irradiations. The positron activity-range was measured from the PET image reconstructed from all nine datasets and compared to the results from simulated images. A 22Na disc-source was also imaged after each beam to monitor the PET system's performance. PET performed well except for slight shifts of energy photo-peak positions (1%) after each beam, due mainly to the neutron exposure of SSPM that increased the dark-count noise. This minor effect was corrected offline with a shifting 350-650keV energy window for each dataset. The results show a fast converging of activity-ranges measured by the prototype PET with high sensitivity and uniform resolution. Sub-mm activity-ranges were achieved with minimal 6s acquisition time and three spill irradiations. These results indicate the feasibility of PET for intra-fraction beam-range verification. Further studies are needed to develop and apply a novel clinical PET system for on-line image-guided adaptive proton therapy.
机译:我们开发并研究了一种正电子发射断层扫描(PET)系统,该系统可用于在线(束内和部分内)图像引导的自适应质子治疗应用。通过使用固态光电倍增管(SSPM)阵列和LYSO闪烁体,PET具有双向旋转的相互作用深度可测量的探测器面板。它具有44毫米直径的跨轴和30毫米轴向视场(FOV)。将38mm直径的聚甲基丙烯酸甲酯幻影放置在FOV内部。 PET和幻像轴均与179.2 MeV准直光束对齐。每个发射的光束约有50次泄漏(0.5s泄漏和1.5s泄漏间时间,在Bragg峰处为3.8 Gy)。用检测器以给定角度获取每个光束的数据。采集了九个光束的九个数据集,这些光束在180个位置上具有九个不同角度的检测器,用于全断层成像。每个数据集都包括照射期间和照射后5分钟的数据。从所有九个数据集重建的PET图像中测量正电子活性范围,并将其与模拟图像的结果进行比较。在每束光束之后还对22Na光盘源进行了成像,以监视PET系统的性能。除了在每束光束后能量光峰位置发生轻微移动(<1%)外,PET表现良好,这主要是由于SSPM的中子暴露增加了暗计数噪声。通过为每个数据集移动350-650keV的能量窗口,可以离线校正此较小的影响。结果表明,原型PET测量的活性范围快速收敛,灵敏度高且分辨率均匀。亚毫米活动范围是在最少6s的采集时间和3次溢出照射下实现的。这些结果表明了PET在部分光束范围内验证的可行性。需要进一步的研究来开发和应用新型的临床PET系统,用于在线图像引导的自适应质子治疗。

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