Microwave wide bandgap GaN high electron mobility transistor development and its monolithic integrated circuits (Invited)

H. Chiu, Chih-Wei Yang, Hsiang-Chun Wang, F. Huang
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引用次数: 1

Abstract

Wide bandgap gallium nitride (GaN) high electron mobility transistor (HEMT) has been extensively studied [1]. The material properties of GaN compared to competing materials are presented in Table I. The superior material properties high breakdown voltage, which allows large drain voltages to be used, leading to high output impedance per watt of RF power, and lower loss matching circuits. High current density of 2-D electron gas (2-DEG) leads to large sheet charge [2] and transistor area can be reduced resulting in high watts per millimeter of gate periphery. High saturated velocity leads to high saturation current densities and watts per unit gate periphery. These result GaN based HEMT are suitable for high-power and high-frequency monolithic microwave integrated circuit (MMIC) applications [3-5]. Due to these excellent material characteristics, the output power and efficiency of GaN power amplifier between L-band and Ka-band was not only more superior to the conventional LDMOSFETs and GaAs power amplifier, but also the die area can be reduced. The GaN HEMT can be operated at 42 V of VDS and even higher, while also demostrated the similar fT and fmax with GaAs pHEMT. The high powers from GaN HEMT transistors at a wide frequency range have been reported form a single die up to several hundred watts [6-7]. However, these high power densities also present extreme power dissipation on the layouts and the semiconductor substrates. Nevertheless, the SiC substrates with a high thermal conductivity (> 330 W/mK) allows high power densities to be efficiently dissipated for practical drain efficiencies, preventing the extreme channel that would result due to self-heating with other substrate technologies.
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微波宽禁带氮化镓高电子迁移率晶体管的研制及其单片集成电路(特邀)
宽禁带氮化镓(GaN)高电子迁移率晶体管(HEMT)得到了广泛的研究[1]。与竞争材料相比,GaN的材料特性如表1所示。优越的材料特性高击穿电压,允许使用大漏极电压,导致每瓦射频功率的高输出阻抗,以及更低的损耗匹配电路。二维电子气体(2- deg)的高电流密度导致较大的片电荷[2],晶体管面积可以减少,从而产生每毫米栅极外围的高瓦数。高饱和速度导致高饱和电流密度和单位栅极外围瓦数。这些结果表明,GaN基HEMT适用于高功率和高频单片微波集成电路(MMIC)应用[3-5]。由于这些优异的材料特性,GaN功率放大器在l波段和ka波段之间的输出功率和效率不仅优于传统的ldmosfet和GaAs功率放大器,而且可以减小芯片面积。GaN HEMT可以在42 V甚至更高的VDS下工作,同时也显示出与GaAs pHEMT相似的fT和fmax。据报道,GaN HEMT晶体管在宽频率范围内的高功率可从单个芯片达到数百瓦[6-7]。然而,这些高功率密度也在布局和半导体衬底上呈现出极端的功耗。然而,具有高导热系数(> 330 W/mK)的SiC衬底可以有效地消散高功率密度,从而实现实际漏极效率,防止因其他衬底技术自热而导致的极端通道。
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