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首页> 外文期刊>Journal of Applied Physics >Modeling of high-frequency capacitance-voltage characteristics to quantify trap distributions near SiO_2/SiC interfaces
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Modeling of high-frequency capacitance-voltage characteristics to quantify trap distributions near SiO_2/SiC interfaces

机译:建模高频电容电压特性以量化SiO_2 / SiC界面附近的陷阱分布

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摘要

A procedure to calculate capacitance-voltage (C-V) characteristics from numerical solutions of the Poisson equation for metal-oxide-semiconductor (MOS) capacitors with traps located both at the oxide/semiconductor interface and in the semiconductor is presented. This method is tested for the simple case of a uniform distribution of a single acceptor or donor level in the semiconductor, for which an approximate analytical solution was derived by analogy with the results obtained for a Schottky diode within the depletion approximation. This method is then applied to model the high-frequency C-V curves of n-type 4H- and 6H-SiC MOS capacitors, which show a kink at depletion bias voltages that broadens with decreasing temperature below 150K. This feature of the high-frequency capacitance occurs at the same temperature and voltage range as a signal detected by constant capacitance deep-level-transient spectroscopy (CCDLTS) measurements and attributed to SiC traps. When only interface traps are considered, the trap energy distribution that is required to reproduce the kink in the C-V curves is not consistent with the trap energy distribution determined from CCDLTS measurements. Numerical simulations show that traps in the SiC epi-layer near the SiO_2/SiC interface as well as interface traps with energies close to the SiC conduction band are necessary to explain both the CCDLTS measurement results and the temperature dependence of C-V curves.
机译:提出了一种从泊松方程的数值解计算电容-电压(C-V)特性的过程,该泊松方程是在氧化物/半导体界面和半导体中均具有陷阱的金属氧化物半导体(MOS)电容器。测试了此方法的简单情况,即单个受主或施主能级在半导体中的分布均匀,为此,可以通过类似于在耗尽近似范围内获得的肖特基二极管的结果,得出近似的分析溶液。然后将该方法应用于对n型4H和6H-SiC MOS电容器的高频C-V曲线进行建模,这些曲线在耗尽偏置电压下会出现纽结,随着温度降低到150K以下,纽结会变宽。高频电容的这一特征出现在与恒定电容深电平瞬态光谱法(CCDLTS)测量所检测到的信号相同的温度和电压范围内,并归因于SiC陷阱。当仅考虑界面陷阱时,再现C-V曲线中的扭结所需的陷阱能量分布与根据CCDLTS测量确定的陷阱能量分布不一致。数值模拟表明,SiO_2 / SiC界面附近的SiC外延层中的陷阱以及能量接近SiC导带的界面陷阱对于解释CCDLTS测量结果和C-V曲线的温度依赖性都是必需的。

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  • 来源
    《Journal of Applied Physics 》 |2012年第9期| p.094509.1-094509.13| 共13页
  • 作者

    A. F. Basile; P. M. Mooney;

  • 作者单位

    Department of Physics, Simon Fraser University, Burnaby, British Columbia V5A 1S6, Canada;

    Department of Physics, Simon Fraser University, Burnaby, British Columbia V5A 1S6, Canada;

  • 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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