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The new approach in the determination of the dependency of sur-face charge density on semiconductor surface potential based voltage–capacity analysis of the depletion region of MIS-structures

机译:新方法在确定耗尽区半导体表面电位电压分析的依次依赖性的依赖性

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The analysis algorithm of quasistatic C-V-characteristics of MIS-structures in the range of the depletion of the semi-conductor surface of main carriers of the charge are developed. This algorithm provides the quantitative determination of a concentration of doping impurity, the fflat bands voltage and efficient values of a capacity and a thickness of a gate insula-tor. On this data, obtained within the framework of the single experiment on the Al-SiO_2-(100) n-Si MOS-structure, dependencies of ψ_s(V_g),Q_s[ψ_s(V_g)] and V_i(V_g) (where ψ_s and Q_s — a surface potential and a density of the surface charge in n-Si, V_g —a gate potential, V_i— a voltage drop on an oxide) are reduced. These dependencies without any a priori information about the state of the electronic gas under the strong accumulation or deep inversion are found. Experimental curves of ψ_s(V_g) and Q_s[ψ_s(V_g)] are possible considered as the criterion of the correct of the theory of the semiconductor space charge region, take into account electron gas degeneration and quantum confinement effects, as observed maximum layered densities of electrons and holes exceed I0~(13)cm~(-2). The dependency of V_i(V_g) necessary to use under investigations of the conductivity through gate insulators, particularly, in cases their small and ultrasmall of the thickness, when the leakage current is defined basically by the tunnel effect.
机译:开发了耗尽电荷主载体的半导体表面的耗尽范围的Quasistatic C-V-特征的分析算法。该算法提供了掺杂杂质浓度的定量测定,“FFLAT条带电压和高效值的容量和栅极insula-tor的厚度。该数据,在Al-SiO_2-(100)中的单个实验的框架内获得的n的Si MOS-结构,ψ_s的依赖(V_g),Q_s [ψ_s(V_g)]和V_I(V_g)(其中ψ_s Q_S - Q_S - 氧化物上的N-Si,V_G -A栅极电位V_i-A电压降的表面电位和表面电荷的密度)。没有找到关于在强累积或深度反演下的电子气体状态的任何先验信息的这些依赖关系。 (V_g)和Q_sψ_s的实验曲线[ψ_s(V_g)]是可能认为是正确的半导体空间电荷区的理论的标准,考虑到电子气变性和量子限制效应,所观察到的最大层叠密度电子和孔超过I0〜(13)cm〜(-2)。在通过栅极绝缘体的电导率调查中使用的v_i(v_g)的依赖性,特别是在它们的厚度的小和超容器的情况下,当基本上通过隧道效应定义时。

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