弥合双极结晶体管噪声的微观和宏观理论之间的差距

G. Niu
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引用次数: 4

摘要

双极晶体管的主要噪声源是基极电阻热噪声或约翰逊噪声、基极电流散点噪声和集电极电流散点噪声。散粒噪声用2qI的谱密度来描述,其中I为直流基极I/sub B/或集电极I/sub C/电流。我们提出了晶体管集电极电流射噪声的详细微观处理,这通常是电子通过EB结势垒的宏观结果。该分析可以应用于异质结双极晶体管以及非均匀掺杂情况。确定了神奇的2qI/sub C/表达式背后的关键假设。其中之一是不包括大多数载流子速度波动引起的噪声,这在高注入时占主导地位。速度饱和和速度超调也会导致偏离2qI/sub C/。我们展示了增量部分内噪声源的详细建模,其向晶体管终端的传播,以及所有增量部分的集成,以评估总终端噪声。说明了标量格林函数和矢量格林函数的概念以及它们与肖克利阻抗场概念的等价性,重点是直观理解。这些概念对于执行有效的数值噪声模拟是必不可少的,最近已在商用TCAD工具中可用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Bridging the gap between microscopic and macroscopic theories of noise in bipolar junction transistors
The major noise sources in a bipolar transistor are the base resistance thermal noise, or Johnson noise, the base current shot noise and the collector current shot noise. The shot noise is described by a spectral density of 2qI, I being the DC base, I/sub B/, or collector, I/sub C/, current. We present a detailed microscopic treatment of the transistor collector current shot noise, which is typically given as a macroscopic result of electrons passing through the EB junction barrier. The analysis can be applied to heterojunction bipolar transistors as well as to non-uniform doping cases. The critical assumptions behind the magic 2qI/sub C/ expression are identified. One of them is that the noise due to majority carrier velocity fluctuations is not included, which dominates at high injection. Velocity saturation and velocity overshoot can also cause deviation from 2qI/sub C/. We show detailed modeling of the noise source within an incremental section, its propagation towards the transistor terminal, and the integration over all of the incremental sections for evaluation of the total terminal noise. The concept of scalar and vector Green's functions as well as their equivalence to Schockley's impedance field concept are illustrated with an emphasis on intuitive understanding. These concepts are essential to performing effective numerical noise simulation, which has recently become available in commercial TCAD tools.
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