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Complex conductivity in the presence of long range potential fluctuations. Application to the determination of the gap state density in undoped and boron doped a-Si : H films grown by CVD

机译:在长期潜在波动存在下复杂的电导率。在掺杂和硼掺杂A-Si:H由CVD生长的掺杂A-Si:H薄膜的应用

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摘要

In compensated crystalline and amorphous semiconductors long range potential fluctuations (PF), at the scale of the mean free path, largely affect the transport properties : they act on free carriers and they change the average degree of ionization of deep centers. The maximum magnitude of PF varies with the applied field, and the corresponding charge and discharge of deep centers in the bulk, at the frequency of the applied field, contribute to the complex conductivity of the sample. The expressions of the total complex conductivity due to lattice, free carriers and deep centers, and of the complex differential capacitance of a MIS diode, are derived in the general case of a compensated semiconductor with potential fluctuations (PF). These expressions differ significantly from those commonly used when ignoring the existence of PF. This ends up in a new method for the determination of the distribution of gap states which, contrary to other methods, allows to separate the contribution of the localized states from the contribution of band carriers. This method is applied to the interpretation of our data on a-Si: H films grown by CVD. The real and the imaginary parts of the conductivity can be fitted in wide ranges of temperatures and frequencies. The variations of the complex conductivity are completely explained by the action of PF on the transport of free carriers and on the ionization of deep centers. There is no evidence of hopping transport. The density of states shows a discrete series of peaks possibly superposed to a lower continuous density.
机译:在补偿结晶和无定形半导体的长范围电位波动(PF),在平均自由路径的规模中,在很大程度上影响运输特性:它们对游离载体作用,它们改变了深度的平均电离程度。 PF的最大幅度随所施加的场而变化,并且在施加的场的频率下,体积的深度的相应电荷和放电有助于样品的复杂电导率。由于晶格,自由载体和深中心以及MIS二极管的复杂差分电容而导致的总复杂电导率的表达在具有电位波动(PF)的补偿半导体的一般情况下导出。这些表达与忽略PF存在时常用的表达有显着差异。这最终以一种新的方法来确定差距状态的分布,这与其他方法相反,允许将局部状态与乐队载体的贡献分开的贡献。该方法适用于通过CVD生长的A-Si:H电影对我们的数据的解释。电导率的真实和虚部可以安装在宽范围的温度和频率范围内。通过PF对自由载体的运输和深居中的电离的作用,完全解释复杂电导率的变化。没有跳跃运输的证据。状态的密度显示了可能叠加到较低的连续密度的离散系列峰。

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