间接转换非晶硒探测器中聚对二甲苯和光导体厚度的优化。

Kaitlin Hellier, Hamid Mirzanezhad, Molly McGrath, Paul Pryor, Ivan Mollov, Shiva Abbaszadeh
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引用次数: 0

摘要

无定形硒(a- se)为低成本、大面积的雪崩光电探测器提供了一个用于间接转换探测器的机会。然而,其2.2 eV的带隙降低了长波长下的响应,特别是CsI:Tl闪烁体发出的550 nm绿光,限制了其应用。将碲加入到a-Se转换层中可以减小带隙并提高这些较长波长的灵敏度。先前的研究已经证明了这种有效性,并表明尽管Se-Te的载流子迁移率和寿命降低,但仍然可以实现高的转换效率。该小组提出在85 um像素间距的间接转换平板探测器中使用Se-Te层,实现对二甲苯孔阻挡层。这项工作的结果表明,需要优化这些层的厚度,以实现高灵敏度、合理的泄漏、低滞后和重影。在本研究中,我们评估了改变聚对二甲苯层厚度和光电探测器转换层对单像素Se-Te器件的影响。我们发现,虽然较厚的Se-Te和对二甲苯器件实现低暗电流、预期信号电平和低滞后,但较薄的样品在器件中遭受信号损失和残余电荷。改变对二甲苯的厚度会导致暗电流和剩余电荷的权衡,这对最终成像仪的性能都很重要。为了利用聚对二甲苯作为孔阻挡层,必须采用较厚的光电导体和聚对二甲苯层。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optimizing parylene and photoconductor thickness in indirect conversion amorphous selenium detectors.

Amorphous selenium (a-Se) provides an opportunity for a low cost, large area, avalanche photodetector for use in indirect conversion detectors. However, its bandgap of 2.2 eV reduces the response at long wavelengths, specifically the 550 nm green light emitted by CsI:Tl scintillators, limits its application. Incorporating tellurium into the a-Se conversion layer is known to reduce the bandgap and increase sensitivity at these longer wavelengths. Previous studies have demonstrated this effectiveness and have shown that high conversion efficiencies can be achieved despite the reduced carrier mobility and lifetime of Se-Te. This group has proposed utilizing a Se-Te layer in an indirect conversion flat panel detector with 85 um pixel pitch, implementing a parylene hole blocking layer. Results of that work demonstrated the need for optimization of the thickness of those layers to achieve high sensitivity, reasonable leakage, and low lag and ghosting. In this study, we evaluate the effects of varying the parylene layer thickness and the photodetector conversion layer for single pixel Se-Te devices. We find that, while thicker Se-Te and parylene devices achieve low dark current, anticipated signal levels, and low lag, thinner samples suffer from signal loss and residual charge in the device. Varying the thickness of parylene leads to tradeoffs in dark current and residual charge, each of which is important in the performance of the final imager. To make use of parylene as a hole blocking layer, thicker photoconductor and parylene layers must be employed.

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