0.15 μm超短栅极长度GaN hemt的不同技术表征:基于二维物理仿真的TCAD陷阱识别

M. Bouslama, R. Sommet, J. Nallatamby
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引用次数: 1

摘要

在本文中,我们使用漏极滞后和栅极滞后测量比较了0.15-$\mu$m超短栅极长度GaN HEMT器件的不同技术(A和B)。在25circC和100circC的不同卡盘温度下,还进行了低频(LF) s参数测量。两种技术s参数测量前后的泄漏电流均小于100 $\mu$A/mm。此外,还进行了一项完整的研究,利用基于二维物理模拟的TCAD确定了a技术中存在的陷阱的确切位置。因此,模型参数已被调整,以适应直流模拟与测量的I-V特性在25circC。这样可以估计在25°c时装置中存在的陷阱(NT)的浓度。了解利用LF s参数测量提取的陷阱能级,在不同温度下进行基于TCAD物理的模拟,以提取低频Y22导纳参数。对于技术A, TCAD模拟表明,当温度升高时,陷阱浓度增加。模拟结果与实测结果吻合较好,并假设陷阱的位置在缓冲区内,活化能Ea=0.47eV,截面约为$6\ × 10^{-16}cm^{2}$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Characterization of Different Technologies of GaN HEMTs of 0,15 μm Ultra-Short Gate Length: Identification of Traps Using TCAD Based 2D Physics-based Simulation
In this paper, we compare to different technologies (A and B) of 0.15-$\mu$m ultra-short gate length GaN HEMT devices using drain lag and gate lag measurements. A low frequency (LF) S-parameters measurements was also performed for different chuck temperatures ranging from 25circC and 100circC. The leakage current which was measured before and after S-parameters measurements for both technologies was lower than 100 $\mu$A/mm. In addition, a complete study has been performed to determine the exact location of the traps existing in technology A using TCAD based 2D physics-based simulation. Thus, the model parameters have been tuned to fit the dc simulation with the measured I-V characteristics at 25circC. This allows to estimate the concentration of traps (NT) present in the device at 25 °c. Knowing the trap energy level extracted using LF S-parameters measurements, TCAD physics-based simulations are performed at various temperatures in order to extract the low frequency Y22 admittance parameter. For technology A, TCAD simulation demonstrate that the concentration of traps increases when the temperature increases. Simulation results are in good agreements with the measurements and assume that the location of traps was in the buffer region, with an activation energy Ea=0.47eV and cross section around $6\times 10^{-16}cm^{2}$.
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