切连科夫辐射因为能提高正电子发射断层扫描专用探测器的时间分辨率而受到关注。由于切伦科夫光子在 1 ps 的量级内迅速发射,因此与基于闪烁体的探测器相比,该探测器的时序性能将得到增强。以前,人们采用不发射闪烁体光子的单体切伦科夫辐射体来抑制辐射体中的反射。然而,重建 γ 射线的相互作用位置是具有挑战性的,因为 γ 射线与辐射体相互作用时发射的切伦科夫光子数量最多只有 30 个。作为光电检测器,使用了具有单独读出功能的高密度光电检测器阵列,以提取切伦科夫光子的所有时间和空间信息。
单体切伦科夫辐射体
→最大限度地提高切伦科夫辐射的时序性能
单独读出
→从几个切伦科夫光子获得所有时间和空间信息
我们进行了蒙特卡洛模拟 [刊文 1]。根据模拟,我们发现对光电检测器的要求是高密度和良好的单光子时间分辨率 (SPTR)。例如,SPTR 必须优于 σ = 40 ps,才能获得 100 ps 半峰全宽 (FWHM) 的符合时间分辨率 (CTR)。
此外,我们还研究了深度学习在提高所提出的探测器的位置分辨率方面的潜在能力 [刊文 2]。
使用 MCP-PMT (R3809) 高速光电检测器测量 CTR 的实验。MCP-PMT 的 SPTR 为 25 ps FWHM。
使用光学胶水将一个氟化铅切伦科夫辐射体贴到 MCP-PMT 的窗口面板上。
结果是,成功获得高于 50 ps FWHM 的 CTR,此结果与模拟结果一致 [刊文 3]。
上述切伦科夫探测器存在光学边界。光学边界会降低探测器的时序性能。我们开发了一种集成切伦科夫辐射体的 MCP-PMT (CRI-MCP-PMT),以消除探测器的光学边界。将普通 MCP-PMT 的窗口面板更换为切伦科夫辐射体,并使用原子层沉积技术在辐射体和光阴极面之间插入氧化铝层。
使用一对 CRI-MCP-PMT 测量 CTR,获得的 CTR 为 41.9 ps FWHM [刊文 4]。此外,通过优化分析参数(例如定时拾取阈值电平和脉冲面积),将 CTR 提高至 30.1 ps FWHM。
通过从头开始回顾所有材料并应用 ALD 技术,我们成功创建了 ALD-MCP,可在不使用含铅材料的情况下确保低噪声和高信号倍增(增益率)。消除铅是向前迈出的一大步,因为在欧盟 (EU) 发布的 RoHS 指令中,铅作为有害物质而被限制使用。
一项符合实验表明,与普通 MCP-PMT 相比,集成 ALD-MCP 的 PMT 可将 CTR 从 41.9 提高到 35.4 ps FWHM [参考资料 6]。
我们利用上述探测器对以及独特的光探测和信号处理技术,成功地在世界上率先实现了无需图像重建的高精度正电子发射成像 [参考资料 7]。应用这些成功的研究结果有望实现一种完全创新的新型辐射医疗成像系统,该系统能够从简单、紧凑的设置中进行快速诊断,同时具有与当前使用的辐射成像系统(如正电子发射断层扫描 (PET))相同或更高的精度。这将有助于提高检测病变组织或器官(如癌症)的检查效率,同时减少辐射照射剂量,减轻患者和医务人员的负担。我们将进一步提高探测器性能,使这一新概念更加实用。
1. R. Ota et al., Med. Phys. 45 (2018) pp. 1999-2008
2. F. Hashimoto et al.,Biomed. Phys. Eng. Express 5 (2019) 035001
3. R. Ota et al., Nucl. Inst. Meth. A 923 (2019) pp. 1-4
4. R. Ota et al.,Phys Med. Biol. 64 (2019) 07LT01
5. R. Ota et al., Phys. Med. biol. 65 (2020) 10NT03
6. R. Ota et al.,Phys Med. Biol. 66 (2021) 064006
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