Roncali Emilie, Kwon Sun Il, Jan Sebastien, Berg Eric, Cherry Simon R
Department of Biomedical Engineering, University of California, Davis, One Shields Avenue, Davis, CA 95616, United States of America.
IMIV, CEA, Inserm, CNRS, Univ. Paris-Sud, Université Paris Saclay, CEA-SHFJ, 91 400, Orsay, France.
Biomed Phys Eng Express. 2019 Apr;5(3). doi: 10.1088/2057-1976/ab0f93. Epub 2019 Apr 17.
We are investigating the use of promptly emitted Cerenkov photons to improve scintillation detector timing resolution for time-of-flight (TOF) positron emission tomography (PET). Bismuth germanate (BGO) scintillator was used in most commercial PET scanners until the emergence of lutetium oxyorthosilicate, which allowed for TOF PET by triggering on the fast and bright scintillation signal. Yet BGO is also a candidate to generate fast timing triggers based on Cerenkov light produced in the first few picoseconds following a gamma interaction. Triggering on the Cerenkov light produces excellent timing resolution in BGO but is complicated by the very low number of photons produced. A better understanding of the transport and collection of Cerenkov photons is needed to optimize their use for effective triggering of the detectors.
We simultaneously generated and tracked Cerenkov and scintillation photons with a new model of light transport that we have released in GATE V8.0. This crystal reflectance model was used to study photon detection and timing properties, building realistic waveforms as measured with silicon photomultipliers.
We compared the behavior and effect of detecting Cerenkov and scintillation photons at several levels, including detection time stamps, travel time, and coincidence resolving time in 3 × 3 × 20 mm BGO crystals. Simulations showed excellent agreement with experimental results and indicated that Cerenkov photons constitute the majority of the signal rising edge. They are therefore critical to provide early triggering and improved the coincidence timing resolution by 50%.
To our knowledge, this is the first complete simulation of the generation, transport, and detection of the combination of Cerenkov and scintillation photons for TOF detectors. This simulation framework will allow for quantitative study of the factors influencing timing resolution, including the photodetector characteristics, and ultimately aid the development of BGO and other Cerenkov-based detectors for TOF PET.
我们正在研究利用即时发射的切伦科夫光子来提高用于飞行时间(TOF)正电子发射断层扫描(PET)的闪烁探测器的时间分辨率。在硅酸镥出现之前,锗酸铋(BGO)闪烁体被用于大多数商用PET扫描仪,硅酸镥通过基于快速且明亮的闪烁信号触发实现了TOF PET。然而,BGO也是基于伽马相互作用后最初几皮秒内产生的切伦科夫光生成快速定时触发信号的候选材料。基于切伦科夫光触发在BGO中能产生出色的时间分辨率,但由于产生的光子数量极少而变得复杂。为了优化其用于探测器有效触发的用途,需要更好地理解切伦科夫光子的传输和收集。
我们使用在GATE V8.0中发布的新型光传输模型同时生成并跟踪切伦科夫光子和闪烁光子。该晶体反射率模型用于研究光子探测和定时特性,构建如用硅光电倍增管测量的实际波形。
我们在多个层面比较了探测切伦科夫光子和闪烁光子的行为及效果,包括探测时间戳、传播时间以及在3×3×20 mm BGO晶体中的符合分辨时间。模拟结果与实验结果高度吻合,表明切伦科夫光子构成了信号上升沿的大部分。因此,它们对于提供早期触发至关重要,并将符合定时分辨率提高了50%。
据我们所知,这是首次对用于TOF探测器的切伦科夫光子和闪烁光子组合的产生、传输和探测进行的完整模拟。该模拟框架将允许对影响时间分辨率的因素进行定量研究,包括光电探测器特性,并最终有助于开发用于TOF PET的BGO和其他基于切伦科夫的探测器。