掺杂谱线改变对非晶硅辐射探测器的改进

J. Drewery, G. Cho, W. Hong, K.K. Lee, S. Kaplan, A. Mireshghi, V. Perez-mendez, J. Tao, D. Wildermuth
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引用次数: 0

摘要

厚(约50 μ m)非晶态Si p-i-n二极管作为最小电离粒子的直接辐射探测器的应用,由于需要施加大的偏置电压以完全耗尽检测本质层,这通常包含每厘米/sup 3/ 5-10*10/sup 14/电离悬空键,因此受到阻碍。大约需要1千伏的电压才能使50亩厚的探测器耗尽,并在p/i触点处形成一个大电场(500千伏/厘米)。这将导致不希望的泄漏电流和相关噪声。这些问题可以通过在本征层内添加薄掺杂层来缓解。通过在本征层内以等间隔插入薄的p型层,所需的耗尽电压可以降低至少1/(n+1),其中n是插入的层数。该原理适用于厚度约为12 μ m的器件。通过选择引入的p层的低掺杂浓度,可以使p型层内的电子损失保持在最小。在靠近主p/i和i/n界面的本征层中埋设掺杂层也可以减小触点处的电场
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Improvements to amorphous silicon radiation detectors by doping profile changes
Application of thick ( approximately 50 mu m) amorphous Si p-i-n diodes as direct radiation detectors for minimum ionizing particles is hampered by the need to apply large bias voltages in order fully to deplete the detecting intrinsic layer, which typically contains 5-10*10/sup 14/ ionizable dangling bonds per cm/sup 3/. A voltage of about 1 kV is required to deplete a 50- mu m-thick detector and a large field (500 kV/cm) builds up at the p/i contact. This leads to an undesirable leakage current and related noise. These problems can be mitigated by addition of thin doped layers within the intrinsic layers. By insertion of thin p-type layers at equal intervals within the intrinsic layer, the required depletion voltage can be reduced by a factor of at least 1/(n+1), where n is the number of layers inserted. This principle is demonstrated for devices approximately 12 mu m in thickness. Electron losses within the p-type layer can be kept to a minimum by choice of a low doping concentration for the introduced p-layers. The electric field at the contacts can also be reduced by doped layers buried in the intrinsic layer close to the main p/i and i/n interfaces.<>
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