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BGO as a hybrid scintillator / Cherenkov radiator for cost-effective time-of-flight PET

机译:BGO作为一种混合闪烁体/ Cherenkov散热器,用于具有成本效益的飞行时间宠物

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摘要

Due to detector developments in the last decade, the time-of-flight (TOF) method is now commonly used to improve the quality of positron emission tomography (PET) images. Clinical TOF-PET systems based on L(Y) SO: Ce crystals and silicon photomultipliers (SiPMs) with coincidence resolving times (CRT) between 325 ps and 400 ps FWHM have recently been developed. Before the introduction of L(Y) SO: Ce, BGO was used in many PET systems. In addition to a lower price, BGO offers a superior attenuation coefficient and a higher photoelectric fraction than L(Y) SO: Ce. However, BGO is generally considered an inferior TOF-PET scintillator. In recent years, TOF-PET detectors based on the Cherenkov effect have been proposed. However, the low Cherenkov photon yield in the order of similar to 10 photons per event complicates energy discrimination-a severe disadvantage in clinical PET. The optical characteristics of BGO, in particular its high transparency down to 310 nm and its high refractive index of similar to 2.15, are expected to make it a good Cherenkov radiator. Here, we study the feasibility of combining event timing based on Cherenkov emission with energy discrimination based on scintillation in BGO, as a potential approach towards a cost-effective TOF-PET detector. Rise time measurements were performed using a timecorrelated single photon counting (TCSPC) setup implemented on a digital photon counter (DPC) array, revealing a prompt luminescent component likely to be due to Cherenkov emission. Coincidence timing measurements were performed using BGO crystals with a cross-section of 3 mm x 3 mm and five different lengths between 3 mm and 20 mm, coupled to DPC arrays. NonGaussian coincidence spectra with a FWHM of 200 ps were obtained with the 27 mm3 BGO cubes, while FWHM values as good as 330 ps were achieved with the 20 mm long crystals. The FWHM value was found to improve with decreasing temperature, while the FWTM value showed the opposite trend.
机译:由于过去十年的探测器的发展,现在通常用于提高正电子发射断层扫描(PET)图像的质量的飞行时间(TOF)方法。基于L(Y)的临床TOF-PET系统:最近开发了325 ps和400ps fwhm之间的巧合分辨率(CRT)的CE晶体和硅光电倍增器(SIPMS)。在引入L(Y)之前:CE,BGO被用于许多PET系统。除了较低的价格外,BGO还提供优越的衰减系数和比L(Y)更高的光电级分,因此:CE。然而,BGO通常被认为是较低的TOF-PET闪烁体。近年来,已经提出了基于Cherenkov效应的TOF-PET探测器。然而,低Cherenkov光子的优点是每次事件的相似于10光子的顺序使能量辨别 - 临床宠物的严重缺点。 BGO的光学特性,特别是其低至310nm的高透明度及其高折射率与2.15相似,将成为一个好的Cherenkov散热器。这里,我们研究了基于Cherenkov发射与基于BGO的闪烁的能量辨别的Cherenkov发射相结合的活动时间,作为一种经济高效的TOF-PET检测器的潜在方法。使用在数字光子计数器(DPC)阵列上实现的时间围绕的单光子计数(TCSPC)设置来执行上升时间测量,揭示可能是由于Cherenkov发射的提示发光组件。使用BGO晶体进行巧合时测量测量,其横截面为3mm×3mm,五个不同长度在3mm和20mm之间,耦合到DPC阵列。用27mm3 BGO块获得FWHM的Nongaussian巧合光谱,27mm 3 BGO块获得了FWHM值与330 PS一样好,通过20mm长的晶体实现。发现FWHM值随温度降低而改善,而FWTM值表明相反的趋势。

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