Equivalent Circuits For High Frequency Transistors

R. Trew
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引用次数: 10

Abstract

topology is determined by physical arguments and two-port characterization techniques. Mathematical functions are determined by physical device modeling or curve fitting to experimental data. The functions can then be analyzed to define a topology. In this manner, for example, it can be shown that the input circuit of an FET can be represented as a series RC circuit and the output network can be represented as a parallel RC circuit. The element values and their relationship to device parameters can be determined by analytic device modeling of the physical structure and the mechanisms responsible for device operation. Once the circuit topology is known the element values can also be extracted from experimental data taken from actual devices over a specified frequency band. The equivalent circuit is generally valid only over the frequency band for which the circuit has been determined. Attempts to extrapolate the response of the circuit beyond the characterized frequency band can produce misleading results, especially for circuits that have been simplified for convenience by removing certain elements. If an equivalent circuit is to be used to predict the upper frequency potential of devices (e.g., to determine ft or fmax) the equivalent circuit must be topologically accurate and based upon device physics. Elements representing the physical processes responsible for device operation must be present. The high frequency operation of four candidate transistors for mm-wave applications is compared in this paper. Physically based equivalent circuits are determined and used to predict high frequency potential. The element values are determined by extraction from measured dc and s-parameter data. The circuits are analyzed to determine the elements that limit high frequency operation. The four transistors investigated are listed in Table I and consist of a Hughes GaAs MESFET, the MIT Lincoln Labs PBT, a TRW AlGaAs/GaAs HEMT, and an Alpha AlGaAs/InGaAs/GaAs pseudomorphic HEMT.
高频晶体管等效电路
拓扑结构由物理参数和双端口表征技术决定。数学函数由物理设备建模或对实验数据的曲线拟合确定。然后可以分析这些函数以定义拓扑。例如,通过这种方式可以表明,场效应管的输入电路可以表示为串联RC电路,输出网络可以表示为并联RC电路。元件值及其与器件参数的关系可以通过物理结构和器件运行机制的解析器件建模来确定。一旦电路拓扑结构已知,元件值也可以从特定频带上实际设备的实验数据中提取出来。等效电路一般只在电路已确定的频带内有效。试图推断电路在特征频带之外的响应可能会产生误导性的结果,特别是对于为了方便而通过去除某些元素而简化的电路。如果等效电路用于预测器件的高频电位(例如,确定ft或fmax),则等效电路必须在拓扑结构上准确并基于器件物理。表示负责设备操作的物理过程的元素必须存在。本文比较了四种候选毫米波晶体管的高频工作特性。确定了基于物理的等效电路,并将其用于预测高频电位。元素值是通过提取测量的直流和s参数数据来确定的。对电路进行分析,确定限制高频工作的因素。所研究的四个晶体管列在表1中,由休斯GaAs MESFET、麻省理工学院林肯实验室PBT、TRW AlGaAs/GaAs HEMT和Alpha AlGaAs/InGaAs/GaAs伪晶HEMT组成。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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