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The kinetic behavior of mobile ions in the Al‐SiO2‐Si system

机译:Al-SiO2-Si体系中移动离子的动力学行为

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Thermally stimulated ionic current (TSIC) measurements have been used to study the kinetic behavior of mobile ions in Al‐SiO2‐Si structures formed by evaporation of Al electrodes onto thermally oxidized Si slices. It is shown that the ionic current under bias‐temperature stress is limited primarily by release of ions from traps at the interfaces, and that traps with a range of detrapping energies are involved. A model is proposed which accurately predicts the detrapping rate for an arbitrary temperature‐time profile. Its parameters are the initial distribution of ions among the trapping states, n0(E), and a quantity, β, characterizing the attempt‐to‐escape frequencies for the traps. n0(E) can be derived from analysis of a TSIC curve, given a value for β which can itself be determined by performing the detrapping in two stages. Escape frequencies are typically of the order 4×1011 s-1, in line with theoretical predictions. In the (111) samples studied, n0(E) at a detrapping field of 106 V cm-1 for Na+ ions at the Si‐SiO2 interface is found to have a sharp maximum at about 0.75 eV, with a tail extending upwards in energy to at least 1.5 eV. The same distribution is found irrespective of the conditions under which the ions were trapped. At the Al‐SiO2 interface, n0(E) is found to depend strongly on the maximum temperature at which the ions were trapped, higher temperatures causing the maximum in the distribution to be shifted to higher energies. This is explained in terms of thermal detrapping of ions initially captured in shallow traps followed by retrapping at the same interface in deeper traps. The total number of available trapping sites at the Si‐SiO2 interface is greater than 5×1012 cm-2. It is inf-nerred that the total density of traps at the Al‐SiO2 interface is much greater still.
机译:热激发离子电流(TSIC)测量已用于研究通过将Al电极蒸发到热氧化的Si切片上而形成的Al-SiO2-Si结构中移动离子的动力学行为。结果表明,偏置温度应力下的离子电流主要受到界面处陷阱的离子释放的限制,并且涉及具有一定范围内的陷阱能量的陷阱。提出了一个模型,该模型可以准确地预测任意温度-时间曲线下的去陷阱速率。其参数是离子在俘获状态之间的初始分布n0(E)和数量β,表征了陷阱的企图逃逸频率。 n0(E)可以从TSIC曲线的分析中得出,给定β值,其值可以通过分两个阶段进行脱陷来确定。逃逸频率通常约为4×1011 s-1,与理论预测一致。在研究的(111)个样品中,发现Si-SiO2界面上Na +离子在106 V cm-1的去俘获场处的n0(E)在0.75 eV处具有极大的最大值,尾部能量向上至少为1.5 eV。无论捕获离子的条件如何,都可以找到相同的分布。在Al-SiO2界面处,发现n0(E)很大程度上取决于离子被俘获的最高温度,较高的温度导致分布中的最大值转移到较高的能量上。这是通过对最初捕获在浅陷阱中的离子进行热解吸,然后在较深陷阱中的相同界面处重新捕获来进行解释的。 Si-SiO2界面处可用的捕获位点总数大于5×1012 cm-2。可以看出Al-SiO2界面处的陷阱的总密度仍然更大。

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    《Journal of Applied Physics 》 |1979年第2期| P.942-950| 共9页
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  • 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);
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