A unified current-voltage and charge-voltage model of quasi-ballistic III-nitride HEMTs for RF applications

Kexin Li, S. Rakheja
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引用次数: 1

Abstract

III-nitride high electron mobility transistors (HEMTs) are a strong candidate for high-power radio frequency (RF) applications due to their ability to support high breakdown fields, while maintaining a high electron mobility and a high density of the two-dimensional electron gas (2DEG). Analytic device models that are physically motivated and mathematically robust are preferred for circuit simulations. Most prior works have focused on compact models for 111-nitride HEMTs that operate in the drift-diffusive limit, while Ref. [1] presents a threshold-voltage-based compact model for quasi-ballistic gallium nitride (GaN) HEMTs using an empirical channel charge model. In this paper, we present a unified and self-consistent current-voltage (I-V) and capacitance-voltage (C-V) model of III-nitride HEMTs that is valid for quasi-ballistic transport. The terminal charges are used to calculate inter-nodal capacitances ensuring charge conservation in the device. Both I-V and C-V model are validated against numerical TCAD simulations and experimental data of short-channel GaN HEMTs. Effects of fringing charge resulting from bulk and surface traps are also incorporated in the model. Key equations of the dynamic model are presented in Table 1. Details of the static I-V model of III-nitride HEMTs are presented elsewhere by the authors [2], and equations are omitted for brevity.
准弹道iii -氮化hemt的统一电流电压和电荷电压模型
iii -氮化物高电子迁移率晶体管(hemt)是高功率射频(RF)应用的有力候选者,因为它们能够支持高击穿场,同时保持高电子迁移率和高密度的二维电子气体(2DEG)。解析器件模型是物理驱动和数学鲁棒的首选电路仿真。大多数先前的工作都集中在在漂移扩散极限下工作的111-氮化物hemt的紧凑模型上,而Ref.[1]使用经验通道电荷模型提出了基于阈值电压的准弹道氮化镓hemt的紧凑模型。本文提出了一种适用于准弹道输运的iii -氮化物hemt的统一且自一致的电流-电压(I-V)和电容-电压(C-V)模型。终端电荷用于计算节点间电容,以保证器件中的电荷守恒。I-V和C-V模型分别通过TCAD数值模拟和短通道GaN hemt的实验数据进行了验证。模型中还考虑了体积阱和表面阱产生的边缘电荷的影响。动态模型的关键方程如表1所示。iii -氮化物hemt静态I-V模型的细节由作者在其他地方提出[2],为简洁起见,省略了方程。
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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