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Decay curve analyses in carrier lifetime measurements of p- and n-type 4H-SiC epilayers

机译:p型和n型4H-SiC外延层载流子寿命测量中的衰减曲线分析

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摘要

The impacts of the ambipolar diffusion constant and surface recombination in carrier lifetime measurements of p- and n-type 4H-SiC epilayers are investigated in detail by comparing a numerical simulation based on a diffusion equation and the measurement of microwave photoconductance decay (μ-PCD) curves measured from 4H-SiC epilayers. The simulation reveals that the shapes of decay curves of excess carrier concentration in epilayers, which defines the effective carrier lifetime, are different between p- and n-type 4H-SiC under a low-level injection condition, even when the bulk lifetime and the surface recombination velocity are fixed to the same values for p- and n-type epilayers. In experiments, the shapes of the microwave photoconductance decay curves measured from p- and n-type 4H-SiC epilayers show a similar tendency to the simulation results under a low-level injection condition. This is attributed to the difference in the dependence of the ambipolar diffusion constant on the excess carrier concentration for p- and n-type 4H-SiC. The comparison of μ-PCD decay curves obtained from 50-μm-thick epilayers with different surface passivation indicates that the surface recombination velocity on the epilayer passivated with deposited SiO_2 followed by NO annealing is about one order of magnitude lower than that of the epilayer passivated with the dry oxide.
机译:通过比较基于扩散方程的数值模拟和微波光导衰减(μ-PCD)的测量,详细研究了双极性扩散常数和表面重组对p型和n型4H-SiC外延层载流子寿命测量的影响。 )曲线是从4H-SiC外延层测得的。模拟表明,在低注入条件下,p型和n型4H-SiC在外延层中过量载流子浓度的衰减曲线形状(定义了有效载流子寿命)是不同的,即使在长寿命和对于p型和n型外延层,表面重组速度固定为相同的值。在实验中,从p型和n型4H-SiC外延层测量的微波光电导衰减曲线的形状在低注入条件下显示出与模拟结果相似的趋势。这归因于对于p型和n型4H-SiC,双极性扩散常数对过量载流子浓度的依赖性不同。从具有不同表面钝化层的50-μm厚外延层获得的μ-PCD衰减曲线的比较表明,经沉积SiO_2钝化并进行NO退火的外延层上的表面复合速度比钝化后的外延层低约1个数量级。与干氧化物。

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  • 来源
    《Japanese journal of applied physics》 |2014年第11期|111301.1-111301.5|共5页
  • 作者单位

    Department of Electronic Science and Engineering, Kyoto University, Kyoto 615-8510, Japan;

    Department of Electronic Science and Engineering, Kyoto University, Kyoto 615-8510, Japan;

    Department of Electronic Science and Engineering, Kyoto University, Kyoto 615-8510, Japan;

    Department of Electronic Science and Engineering, Kyoto University, Kyoto 615-8510, Japan;

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