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Comment on “Direct measurement of minority carriers diffusion length using Kelvin probe force microscopy” †Appl. Phys. Lett. 75, 2435 „1999…‡

机译:关于“使用开尔文探针力显微镜直接测量少数载流子扩散长度”的评论。物理来吧75,2435„ 1999…‡

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摘要

A scanning Kelvin probe microscopy based method forndetermining minority carrier diffusion length was presentednin Ref. 1. The authors claim that diffusion length measurednby this method is independent of surface recombinationnvelocity.n1nWe point out that this claim is applicable only inncase of low surface recombination velocity and the effect ofnsurface recombination has to be taken into account in apply-ning this method to high surface recombination velocity cases.nIf surface recombination velocity is low, minority carrier dif-nfusion toward the surface is negligible compared to diffusionntoward the p–n junction in the Fig. 1 of Ref. 1 such thatndiffusion toward the surface has negligible effect on minorityncarrier density at the edge of surface space charge region andnthe surface potential profile shown in the Fig. 3 of Ref. 1 isna reliable representation of minority carrier density gradientnresulting from diffusion toward the p–n junction in the bulk.nminority carrier diffusion toward the surface can be compa-nrable to diffusion toward the p–n junction. Therefore minor-nity carrier distribution near the meeting point of a p–n junc-ntion and a high recombination velocity surface is governednby a two-dimensional diffusion equation. Numerical simula-ntions of two-dimensional diffusion equations near a p–nnjunction under illumination have shown significant role ofnsurface recombination on minority carrier distribution whichndeviates considerably from the distribution obtained from thensolution of a one-dimensional diffusion equation.n2nHence fornhigh surface recombination velocity cases the minority car-nrier distribution given by the Eq. u00024u0003 in Ref. 1 should benreplaced by the solution of a two-dimensional diffusionnequation subject to an independently determined surface re-ncombination velocity as one of the boundary conditions.
机译:参考文献中提出了一种基于扫描开尔文探针显微镜的确定少数载流子扩散长度的方法。 1.作者声称这种方法测得的扩散长度与表面重组速度无关。n1n我们指出,该主张仅在表面重组速度低的情况下适用,并且在将这种方法应用到表面时必须考虑表面重组的影响。 n如果表面重组速度低,与图1中向p–n结的扩散相比,少数载流子向表面的扩散可忽略不计。从图1可以看出,朝向表面的扩散对表面空间电荷区边缘的少数载流子密度的影响可忽略不计,而表面电势分布如图3所示。图1可靠地表示了从载流子中向p-n结的扩散引起的少数载流子密度梯度。向表面的少数载流子的扩散与向p-n结的扩散可以进行比较。因此,在一个二维结和一个高复合速度表面的相交点附近的少数载流子分布是由二维扩散方程控制的。在光照下靠近结点的二维扩散方程的数值模拟表明,n表面复合对少数载流子分布的重要作用,这大大地偏离了从一维扩散方程解得到的分布。由等式给出的汽车载货汽车分布。参考中的u00024u0003应将二维扩散方程的解替换为边界条件之一,该方程要经受独立确定的表面重组速度来代替1。

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  • 来源
    《Applied Physics Letters》 |2010年第21期|p.1-1|共1页
  • 作者单位

    University of Alaska–Fairbanks, Fairbanks, Alaska 99701, USA;

  • 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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