Study of Annihilation Photon Pair Coincidence Time Resolution Using Prompt Photon Emissions in New Perovskite Bulk Crystals

溶血酶- 半导体 材料科学 Crystal(编程语言) 光电倍增管 光子 闪烁体 光学 光电子学 闪烁 硅光电倍增管 切伦科夫辐射 半最大全宽 物理 探测器 计算机科学 程序设计语言
作者
Li Tao,Yihui He,Mercouri G. Kanatzidis,Craig S. Levin
出处
期刊:IEEE transactions on radiation and plasma medical sciences [Institute of Electrical and Electronics Engineers]
卷期号:6 (7): 804-810 被引量:5
标识
DOI:10.1109/trpms.2022.3149992
摘要

Semiconductor-based radiation detectors can typically achieve better energy and spatial resolution when compared to scintillator-based detectors. However, if used for positron emission tomography (PET), semiconductor-based detectors normally cannot achieve excellent coincidence time resolution (CTR), due to the relatively slow charge carrier collection time limited by the carrier drift velocity. If we can collect prompt photons emitted from certain semiconductor materials, there are possibilities that the CTR can be greatly improved, and time-of-flight (ToF) capability can be achieved. In this paper, we studied the prompt photon emission (mainly Cherenkov luminescence) property and fast timing capability of cesium lead chloride (CsPbCl3) and cesium lead bromide (CsPbBr3), which are two new perovskite semiconductor materials. We also compared their performance with thallium bromide (TlBr), another semiconductor material that has already been studied for timing using its Cherenkov emissions. We performed coincidence measurements using silicon photomultipliers (SiPMs), and the full-width-at-half-maximum (FWHM) CTR acquired between a semiconductor sample crystal and a reference lutetium-yttrium oxyorthosilicate (LYSO) crystal (both with dimensions of 3 × 3 × 3 mm3) is 248 ± 8 ps for CsPbCl3, 440 ± 31 ps for CsPbBr3, and 343 ± 16 ps for TlBr. Deconvolving the contribution to CTR from the reference LYSO crystal (around 100 ps) and then multiplying by the square root of 2, the estimated CTR between two of the same semiconductor crystals was calculated as 324 ± 10 ps for CsPbCl3, 606 ± 43 ps for CsPbBr3 and 464 ± 22 ps for TlBr. This ToF capable CTR performance combined with an easily scalable crystal growth process, low cost and toxicity, as well as good energy resolution lead us to the conclusion that new perovskite materials such as CsPbCl3 and CsPbBr3 could be excellent candidates as PET detector materials.
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