用于电子应用的GaN基器件

M.A. Khan, M. Shur
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引用次数: 2

摘要

甘有非常高的细分领域(测量值是1.3 MV /厘米(见Gaska et al。(1997)和预期值超过5 MV /厘米),高峰和饱和速度(vp≈2.7 x10 5 m / s, vs≈1.5 x10 m / s预测的蒙特卡罗模拟,看到Bhapkar和前(1997年),一个相对较高的电子迁移率(800厘米/ v在GaN掺杂在室温下10厘米,超过1500厘米/ v二维电子在GaN /沃甘接口,参见Shur et al.(1996))和可观的导热性(与Si相当,比砷化镓高三倍)。这些特性使得氮化镓和相关材料在高温、高功率和/或恶劣环境下的电子器件应用中非常有吸引力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
GaN based devices for electronic applications
GaN has a very high breakdown field (the measured value is 1.3 MV/cm (see Gaska et al. (1997) and the expected values are over 5 MV/cm), high peak and saturation velocity (vp ≈ 2.7x10 5 m/s, vs ≈ 1.5x10 m/s predicted by Monte Carlo simulations, see Bhapkar and Shur (1997)), a relatively high electron mobility (up to 800 cm/V-s at room temperature in GaN doped at 10 cm and over 1,500 cm/V-s for two-dimensional electrons at the GaN/AlGaN interface, see Shur et al. (1996)) and a respectable thermal conductivity (comparable to that of Si and three times higher than for GaAs). These properties make GaN and related materials very attractive for applications in electronic devices operating at high temperatures, high power, and/or in a harsh environment.
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