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Breakdown Conduction in Al‐SiO‐Al Capacitors

机译:Al-SiO-Al电容器的击穿传导

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摘要

Destructive breakdown has been studied in Al-SiO-Al capacitors using transmission electron microscopy and electron diffraction, while the capacitors were subjected to controlled electrical stresses. Extensive electrical measurements were made outside the electron microscope on other capacitors. The purpose is to describe destructive breakdown and to relate it to prebreakdown conduction, conditions of fabrication, and capacitor structure. It is found that breakdowns originate at inhomogeneities in the dielectric which appear in electron micrographs as irregularly shaped dark spots about 0.5 μ in diameter. The structure of these dark spots has not been determined. Breakdowns are not concentrated at pinholes, dust spots, or fissures. Breakdown is accompanied by the growth of crystalline silicon. Electrical measurements with a given capacitor reveal two well-defined polarity-sensitive threshold voltages, one for the onset of breakdown and one for the cessation of breakdown. Both are virtually independent of temperature from 80° to 380°K. The voltage threshold for the onset of breakdown varies approximately as w1/2, where w is the dielectric thickness, while the voltage threshold for the cessation of breakdown is found to be independent of dielectric thickness. The diameter of a typical breakdown is 10 to 100 μ. The conductivity of the breakdown site at the onset of breakdown changes by a factor of about 1010 in a time less than 0.1 μsec. Duration of a breakdown is usually about 1 μsec. A breakdown mechanism is proposed that is based upon an electrochemical solid reaction in the presence of the breakdown electric field: Si-O-Si+(breakdown electric field)→Si-Si++O+e, where the term Si-Si+ means the two silicon atoms are in crystalline form and one is singly ionized. A de-nscription of the breakdown process is given using this reaction.
机译:已经在Al-SiO-Al电容器中使用透射电子显微镜和电子衍射研究了破坏性击穿,同时使电容器受到受控的电应力。在电子显微镜以外的其他电容器上进行了广泛的电气测量。目的是描述破坏性击穿,并将其与击穿前导通,制造条件和电容器结构相关联。发现击穿起源于电介质中的不均匀性,其在电子显微照片中显示为直径约0.5μ的不规则形状的暗点。这些黑点的结构尚未确定。故障不集中在针孔,灰尘点或裂缝处。击穿伴随着晶体硅的生长。使用给定电容器进行的电气测量显示了两个定义明确的极性敏感阈值电压,一个用于击穿开始,一个用于停止击穿。两者实际上都与80°至380°K的温度无关。击穿开始的电压阈值大约变化为w1 / 2,其中w是电介质厚度,而发现击穿停止的电压阈值与电介质厚度无关。典型击穿的直径为10至100μ。击穿开始时击穿部位的电导率在不到0.1微秒的时间内变化约1010倍。击穿的持续时间通常约为1微秒。提出了一种在存在击穿电场的情况下基于电化学固体反应的击穿机理:Si-O-Si +(击穿电场)→Si-Si ++ O + e,其中术语Si-Si +表示两个硅原子为晶体形式,一个被单个离子化。使用该反应给出了分解过程的描述。

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  • 来源
    《Journal of Applied Physics》 |1967年第7期|共15页
  • 作者单位

    Auburn University, Auburn, Alabama;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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