用修正的热释电流模型分析肖特基二极管随温度变化的电流-电压特性

A. Turut
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引用次数: 0

摘要

我们通过数值模拟研究了不均匀肖特基二极管(SD)上的电流随温度变化的行为。我们使用了修正的热释电 (TE) 电流表达式,其势垒高度呈高斯分布。这种改进的热释电模型假定在肖特基接触和半导体界面上存在一系列低势垒贴片。首先,我们讨论了在 300、200 和 100 K 的不均匀 SD 中,贴片电流化合物相对于 TE 化合物的行为,这是标准偏差和圆形贴片数量 N 的函数。在 N1=1.81×106 或 N2=1.81×108 时,σ1=4.35×10-5cm2/3V1/3 和 σ2=7.35×10-5cm2/3V1/3 的 I-V-T 曲线中,两种 N 值下的 σ2 在 75 K 的 I-V 曲线中都观察到了交集行为;然而,由于 σ1<σ2 的原因,两种 N 值下的σ1 都没有观察到相同的行为。也就是说,σ2 在 75 K 时的电流超过了更高温度下的电流。这种行为是由于有效 BH 随温度值的降低而减小。在与偏压无关的 I-V-T 曲线中,σ1 没有观察到这种相交现象,而在 75 K 和 100 K 的 I-V 曲线中,σ2 却观察到了这种相交现象。因此,得出的结论是,在将 SD 的实验 I-V 曲线拟合到理论 I-V 曲线时,必须使用与偏压相关的 I-V 方程来避免这种相交行为。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Analysis of temperature-dependent current–voltage characteristics of Schottky diodes by the modified thermionic emission current model
We have investigated the behavior of current flow across an inhomogeneous Schottky diode (SD) as a function of temperature by numerical simulation. We have used the modified thermionic emission (TE) current expression with a Gaussian distribution of potential barrier heights. This modified TE model assumes the presence of a series of low-barrier patches at the Schottky contact and semiconductor interface. First, we have discussed the behavior of the patch current compound relative to the TE compound in the inhomogeneous SD at 300, 200, and 100 K, as a function of standard deviation and the number of circular patches N. Then, we have investigated the behavior of temperature- and bias-dependent and bias-independent current vs voltage (I–V–T) characteristics in the 75–300 K range. In bias-dependent I–V–T curves obtained for σ1=4.35×10−5cm2/3V1/3 and σ2=7.35×10−5cm2/3V1/3 at N1=1.81×106 or N2=1.81×108, an intersection behavior has been observed in the I–V curve at 75 K for σ2 at both N values; however, the same behavior has been not observed for σ1 at both N values due to σ1<σ2. That is, the current for σ2 at 75 K has exceeded the current at higher temperatures. This behavior has been ascribed to the effective BH to decrease with decreasing temperature value. In the I–V–T curves independent of bias, such an intersection has not been observed for σ1 while it has been observed for σ2 in the I–V curves at both 75 and 100 K. Thus, it has been concluded that the bias-dependeσnt I–V equations must be used to avoid this intersection behavior while fitting the experimental I–V curve of an SD to the theoretical I–V curve.
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