mm-Wave N-polar GaN MISHEMT with a self-aligned recessed gate exhibiting record 4.2 W/mm at 94 GHz on Sapphire

B. Romanczyk, S. Wienecke, M. Guidry, Haoran Li, K. Hestroffer, E. Ahmadi, Xun Zheng, S. Keller, U. Mishra
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引用次数: 9

Abstract

GaN based high electron mobility transistors have emerged as a leading technology for mm-wave solid state power amplification at W-band. To date, reports on W-band GaN HEMTs and MMICs have primarily featured devices grown in the Ga-polar orientation [1, 2]. In this work, the advantages of the N-polar orientation are exploited to produce a MISHEMT exhibiting record high 4.2 W/mm peak output power (Pout) at 94 GHz. The key enabling advantage of N-polar GaN devices are their inverted polarization fields. These fields create a natural, charge-inducing back-barrier that decouples the tradeoff between aspect ratio and channel electron density. Further, the reversed field in an AlGaN cap above the GaN channel opposes gate leakage and improves breakdown voltage [3]. Additionally, to mitigate surface-state induced dispersion and enhance the conductivity of the access regions, a GaN cap layer is added in the access regions through which the gate is recessed [4]. The fabrication process reported in this paper extends that of [4, 5] to have the foot gate metal deposited in a self-aligned fashion to the GaN cap recess etch.
具有自对准嵌入式栅极的毫米波n极GaN MISHEMT在蓝宝石上在94 GHz下表现出创纪录的4.2 W/mm
基于氮化镓的高电子迁移率晶体管已成为w波段毫米波固态功率放大的领先技术。迄今为止,关于w波段GaN hemt和mmic的报道主要以ga极性方向生长的器件为特征[1,2]。在这项工作中,利用n极取向的优势,生产出在94 GHz下具有创纪录的4.2 W/mm峰值输出功率(Pout)的MISHEMT。n极GaN器件的关键使能优势是其反向极化场。这些场创造了一个自然的、电荷诱导的后障,使纵横比和通道电子密度之间的权衡去耦。此外,GaN沟道上方的AlGaN帽中的反向场防止栅极泄漏并提高击穿电压[3]。此外,为了减轻表面态引起的色散并增强通路区域的导电性,在栅极嵌入的通路区域中添加了GaN帽层。本文报道的制造工艺扩展了[4,5]的制造工艺,使脚栅金属以自对准的方式沉积到GaN帽凹槽蚀刻上。
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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