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Photon counting performance of amorphous Selenium and its dependence on detector structure

机译:非晶态硒的光子计数性能及其与探测器结构的关系

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Photon counting detectors (PCD) have the potential to improve x-ray imaging, however they are still hindered by high production costs and performance limitations. By using amorphous Selenium (a-Se) the cost of PCDs can be significantly reduced compared to currently used crystalline semiconductors and enable large area deposition. To overcome the limitation of low carrier mobility and low charge conversion gain in a-Se, we are developing a novel direct conversion a-Se field-Shaping multi-Well Avalanche Detector (SWAD). SWADs multi-well, dual grid design creates separate non-avalanche interaction (bulk) and avalanche sensing (well) regions, achieving depth-independent avalanche gain. Unipolar time differential (UTD) charge sensing, combined with tunable avalanche gain in the well region allows for fast timing and comparable charge conversion gain to crystalline semiconductors. In the present work we developed a probability based numerical simulation to model the charge generation, transport and signal collection of three different a-Se detector configurations and systematically show the improvements in energy resolution attributed to UTD charge sensing and avalanche gain. Pulse height spectra (PHS) for each detector structure, exposed to a filtered ~(241)Am source, are simulated and compared against previously published PHS measurements of a conventional a-Se detector. We observed excellent agreement between our simulation of planar a-Se and the measured results. The energy resolution of each generated PHS was estimated by the full-width-at-half-maximum (FWHM) of the primary photo-peak. The energy resolution significantly improved from ~33 keV for the planar a-Se detector to ~7 keV for SWAD utilizing UTD charge sensing and avalanche gain.
机译:光子计数检测器(PCD)具有改善X射线成像的潜力,但是它们仍然受到高生产成本和性能限制的阻碍。与目前使用的晶体半导体相比,通过使用非晶硒(a-Se),可以显着降低PCD的成本并实现大面积沉积。为了克服a-Se中低载流子迁移率和低电荷转换增益的局限性,我们正在开发一种新颖的直接转换a-Se场成形多阱雪崩检测器(SWAD)。 SWAD的多井,双栅格设计创建了独立的非雪崩相互作用(体)和雪崩感测(井)区域,从而实现了与深度无关的雪崩增益。单极时差(UTD)电荷感测与阱区中的可调节雪崩增益相结合,可实现快速定时并具有与晶体半导体相当的电荷转换增益。在当前的工作中,我们开发了基于概率的数值模拟,以对三种不同的a-Se检测器配置的电荷产生,传输和信号收集进行建模,并系统地显示了归因于UTD电荷感测和雪崩增益的能量分辨率的提高。模拟每个暴露于过滤后的〜(241)Am源的探测器结构的脉冲高度谱(PHS),并将其与常规a-Se探测器先前发布的PHS测量值进行比较。我们观察到我们在平面a-Se的模拟与测量结果之间达成了极好的一致性。每个产生的PHS的能量分辨率是通过主光电峰的半峰全宽(FWHM)估算的。利用UTD电荷感测和雪崩增益,能量分辨率从平面a-Se检测器的〜33 keV显着提高到SWAD的〜7 keV。

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