Approaches for Measuring Fast Modulation of Optical Properties Induced by 511keV Photon Interactions

Diana Jeong, Li Tao, Zander Adams, Yushin Kim, C. Levin
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Abstract

With a goal to achieve less than 10 picosecond (ps) coincidence time resolution for advancing time-of-flight positron emission tomography (TOF-PET), we seek to leverage the effects of transient free carriers generated from 511 keV interactions in a material. Most ultrafast optics methods rely on many excitation particles with a priori information on their arrival times. However, in PET it is critical to find a way to sensitively detect single, randomly emitted 511 keV annihilation photons from the ionization it produces. We investigate two ways to increase the signal: employing probe laser wavelength in the mid-IR and confining the probe beam to match the size of ionization tracks created by the 511 keV photons. We observed a continued decrease of 2% in transmission of the mid-IR probe beam (8μm) in a 10 X 10 X 1 mm3 Cadmium Telluride crystal with 511 keV annihilation irradiation over 300 seconds. The trend was reversed when the radiation source is removed, and reached the previous baseline transmission in 800 seconds. For confining the interaction volume to match the probe beam diameter, we revised a previously investigated interferometry approach to use a focused beam and did not apply a bias voltage across the detector crystal. With a 405nm laser diode as an excitation source, a shift of 43% in transmitted signal voltage was observed, and with Am-241 alpha source irradiation, a 1% shift was measured. With the improved sensitivity, these findings provide insights into possible methods of detecting single 511 keV events.
511keV光子相互作用诱导的光学特性快速调制测量方法
为了实现小于10皮秒(ps)的符合时间分辨率,以推进飞行时间正电子发射断层扫描(TOF-PET),我们试图利用材料中511 keV相互作用产生的瞬态自由载流子的影响。大多数超快光学方法依赖于许多具有其到达时间先验信息的激发粒子。然而,在PET中,找到一种方法来灵敏地探测它产生的电离中随机发射的511 keV湮灭光子是至关重要的。我们研究了两种增加信号的方法:采用中红外探测激光波长和限制探测光束以匹配511 keV光子产生的电离轨迹的大小。我们观察到在511 keV湮灭辐照300秒后,中红外探测光束(8μm)在10 X 10 X 1 mm3碲化镉晶体中的透射率持续下降2%。当辐射源被移除后,这一趋势发生了逆转,在800秒内达到了之前的基线传输。为了限制相互作用体积以匹配探测光束直径,我们修改了先前研究的干涉测量方法,使用聚焦光束,并且不在探测器晶体上施加偏置电压。以405nm激光二极管作为激发源,观察到传输信号电压偏移43%,在Am-241 α源照射下,测量到传输信号电压偏移1%。随着灵敏度的提高,这些发现为检测单个511 keV事件的可能方法提供了见解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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