一种确定放大器晶体管几何形状的新方法

Yingying Yang, Bin Li, Brian Johnson, Hal Banbrook
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引用次数: 0

摘要

该方法使用了一个新的概念“增益数${\左({GN} \右)}$”和“过渡频率${\左({f_{Tr}} \右)}$”(介于最大稳定增益${\左({MSG} \右)}$和最大可用增益$\左之间)。{\left({MAG} \right)} \right)$作为优值,为PA设计选择最合适的HBT器件${\left({f \_ dsn} \right)}$。关键是建立${GN}$和${f_Tr}$之间的关系,以及HBT的几何参数和相关的数学量:HBT的基座面积$\左的比率。{\left({A_B} \right)} \right)$到发射器区域$\left。{\left({A_E} \right)} \right)$和基极电阻$\left的乘积。{\left({R_B} \right)} \right)$和${A_E}$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Novel Method to Determine Transistor Geometry for PA Design
This method uses a new concept “Gain Number ${\left( {GN} \right)}$” and “Transition Frequency ${\left( {f_{Tr}} \right)}$” (between Maximum Stable Gain ${\left( {MSG} \right)}$ and Maximum Available Gain $\left. {\left( {MAG} \right)} \right)$ as figures-of-merit to select a most suitable HBT device for a PA design of a certain required frequency ${\left( {f \_ dsn} \right)}$. The key is to establish relationships between ${GN}$ and ${f_Tr}$, and the HBT's geometrical parameters and associated mathematical quantities: the ratio of an HBT's base pedestal area $\left. {\left( {A_B} \right)} \right)$ to emitter area $\left. {\left( {A_E} \right)} \right)$ and the product of base resistance $\left. {\left( {R_B} \right)} \right)$ and ${A_E}$.
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