Threshold voltage of m.o.s. transistors doped nonuniformly near the surface

H. Feltl
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Abstract

Due to impurity redistribution and ion implantation, m.o.s. transistors are usually doped nonuniformly beneath the gate. From an analytical solution of Poisson's equation a modified expression for the threshold voltage has been derived. The change in the impurity concentration is taken into account, on the one side, in the usual manner by its contribution to the surface charge and, on the other side, on the basis of its contribution to the surface potential instead of the rather arbitrary approximation by an ‘effective’ impurity concentration. The modified formula gives a better description of the measured threshold voltages at least for an extended region, if not for the entire range of the applied substrate bias voltage. As theoretically predicted, the substrate bias coefficient corresponds to the bulk impurity concentration. A comparison with experimental results shows exceptionally close agreement if the depletion layer fully, or largely, covers the region of altered impurity concentration. If this region extends substantially beyond the depletion layer, deviations are observed. This result has been confirmed from impurity profiles determined for the purpose of verification.
近表面非均匀掺杂mos晶体管的阈值电压
由于杂质重分布和离子注入,mos晶体管通常在栅极下不均匀掺杂。从泊松方程的解析解出发,导出了阈值电压的修正表达式。考虑杂质浓度的变化,一方面,以通常的方式,通过它对表面电荷的贡献,另一方面,根据它对表面电位的贡献,而不是相当武断的“有效”杂质浓度的近似。修正的公式给出了至少对于一个扩展区域的测量阈值电压的更好描述,如果不是对于所施加的衬底偏置电压的整个范围的话。正如理论预测的那样,衬底偏置系数对应于体杂质浓度。与实验结果的比较表明,如果耗尽层完全或大部分覆盖杂质浓度变化的区域,则与实验结果非常接近。如果这个区域大大超出枯竭层,就会观察到偏差。这一结果已从为验证目的而测定的杂质谱中得到证实。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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