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首页> 外文期刊>International journal of numerical modelling >A pertinent approximation of the electrostatic potential in a quantized electron accumulation layer induced at a nonideal surface of a narrow-gap semiconductor
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A pertinent approximation of the electrostatic potential in a quantized electron accumulation layer induced at a nonideal surface of a narrow-gap semiconductor

机译:在窄间隙半导体非理想表面感应的量子化电子积累层中的静电势的近似值

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摘要

Quantitative analysis of the electron accumulation layer formed near nonideal (actual) semiconductor surface causes considerable difficulties. In the present article, for the accumulation layers induced in the subsurface region at the real narrow-gap semiconductor-insulator interface, an effective algorithmic approach providing a simplified self-consistent solution of the Poisson and Schrodinger equations is proposed and discussed. The physical model takes into account the conduction band nonparabolicity, electron gas degeneration, and other dominant features of solids in question; special attention is paid to the existence of semiconductor-dielectric intermediate layer. A novel approximation for the surface electrostatic potential in the form of a modified ?ratzer potential is proposed and substantiated. It allows us to obtain the electron wavefunctions and energy spectrum in the analytical form. It is shown that the modified ?ratzer potential is a good approximation function applicable at least to subsurface electron accumulation layers induced at the A(3)B(5) narrow-gap semiconductor boundary surface allowing for the existence of a semiconductor-insulator intermediate layer. For the n-InSb nonideal surface, as an example, spatial distribution of electron potential energy, discrete energy spectrum of electrons in the broad range of surface densities (up to 10(13)cm(-2)), and some other physical characteristics are calculated using the proposed algorithm.
机译:对在非理想(实际)半导体表面附近形成的电子积累层进行定量分析会产生很大的困难。在本文中,对于在真正的窄间隙半导体-绝缘体界面处在地下区域中引起的累积层,提出并讨论了一种有效的算法方法,该方法为Poisson和Schrodinger方程提供了简化的自洽解。物理模型考虑了导带的非抛物线性,电子气的退化以及所讨论固体的其他主要特征;特别注意半导体介电中间层的存在。提出并证实了一种新型的表面静电势的近似形式,其形式为修饰的弗雷泽电势。它使我们能够以分析形式获得电子波函数和能谱。结果表明,修饰的阱电压至少在A(3)B(5)窄间隙半导体界面处感应到的地下电子累积层具有良好的近似函数,从而可以存在半导体绝缘体中间层。例如,对于n-InSb非理想表面,电子势能的空间分布,在广泛的表面密度范围内(高达10(13)cm(-2))的电子离散能谱以及一些其他物理特性使用提出的算法计算。

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