具有电容耦合触点的氮化场效应晶体管

G. Simin, Z. Yang, A. Koudymov, V. Adivarahan, J. Yang, M. Khan
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引用次数: 0

摘要

我们展示了使用电容耦合电极(C3HFET)设计的新型宽带隙AlGaN/GaN异质结构场效应晶体管。C3HFET的源极、栅极和漏极与2d通道具有电容耦合。肖特基和绝缘栅极(C3MOSHFET)器件的实现已经实现。该器件不需要退火欧姆触点,可以使用栅极无对准技术制造。c3hfet和c3moshfet除了在制造技术上有明显的优势外,还具有较低的有效射频接触电阻(低于0.5 Qmm),当用作射频控制器件时,如功率调制器、开关、衰减器等,能够处理更高的射频功率。据我们所知,这是这种类型的宽带隙高功率射频器件的第一份报告。迄今为止,几乎所有的III-N高频电子器件都是基于AlGaN-GaN异质界面上具有高温退火源-漏欧姆触点的二维电子气(2DEG)通道。退火温度(通常超过850℃)会降低AlGaN-GaN异质结,产生捕获中心,并可能显著降低器件的可靠性。存在一类广泛的射频控制装置,其操作不需要直流偏置。这些是射频开关,衰减器,调制器,功率限制器等。对于这种器件类型,我们探索了一种新的设计方法,在AlGaN/GaN界面上使用金属电极和高密度2DEG之间的电容耦合。新型C3HFET由三个金属电极组成,即源极、栅极和漏极,沉积在AlGaNGaN结构的顶部。在SiC衬底1.5 pim厚的未掺杂GaN缓冲层上,MOCVD生长出25 nm厚的A1025Ga075N阻挡层。C3MOSHFET在金属电极下有一个额外的10nm厚的SiO2层。在器件制造中不使用退火。源极和漏极长度,L= 5 ptm;栅极长度LG=1 ptm。源漏间距为LDs=5jm。器件总宽度W= 2 × 125 ptm。采用hp851 OC网络分析仪测量了c3器件的高频特性。在1 GHz左右的触点截止频率以上,插入损耗与具有退火触点的常规HFET或MOSHFET相同或更低。s参数提取的有效接触电阻小于0.5 Q-mm。新型C3晶体管的功率处理能力在10 GHz下进行了表征。射频控制装置中最显著的大信号失真表现为由于通道电位调制而导致的亚阈值电流的增加;通常,亚阈值电流的增加对最大工作射频功率施加了最关键的限制。因此,对于GaAs器件,典型的最大工作(开关)射频功率不超过1W,对于基于AlGaN/GaN的hfet器件,其功率约为20w。我们发现,对于新型AlGaN/GaN C3 HFET和c3moshfet,最大射频功率比具有欧姆触点的HFET和MOSHFET器件高10倍左右。使用绝缘栅c3moshfet实现了最高的最大功率。我们的估计表明,对于1毫米宽的c3moshfet,最大射频功率高达100 W。据我们所知,这是场效应晶体管所达到的最高射频功率密度。进一步的实验和仿真表明,这些创纪录的高开关功率是由于大振幅射频输入信号在电容耦合触点下2DEG密度的自调制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
III-Nitride Field-Effect Transistors with Capacitively-Coupled Contacts
We demonstrate novel wide bandgap AlGaN/GaN heterostructure field-effect transistor design using capacitively-coupled electrodes (C3HFET). The source, gate and drain of C3HFET have capacitive coupling with the 2D-channel. Both Schottky and insulated gate (C3MOSHFET) device implementations have been realized. The devices do not require annealed ohmic contacts and can be fabricated using gate alignment-free technology. Besides obvious advantages in the fabrication technology, the C3HFETs and C3MOSHFETs have low effective RF contact resistance (below 0.5 Qmm) and are capable of handling much higher RF powers when used as RF control devices, such as power modulators, switches, attenuators etc. To the best of our knowledge this is first report of this type of wide bandgap high-power RF devices. To date nearly all the III-N high frequency electronic devices are based on 2D electron gas (2DEG) channel at the AlGaN-GaN heterointerface with high-temperature annealed source-drain ohmic contacts. The annealing temperatures (typically over 850 C) degrade AlGaN-GaN heterojunction, generate trapping centers, and may significantly reduce the device reliability. There exists a broad class of RF control devices, which operation does not require the DC bias. These are RF switches, attenuators, modulators, power limiters etc. For this device types we explore a new design approach using capacitive coupling between the metal electrodes and the high-density 2DEG at the AlGaN/GaN interface. Novel C3HFET consists of three metal electrodes, source, gate and drain, deposited on top of AlGaNGaN structure. The 25 nm thick A1025Ga075N barrier layer was grown by MOCVD over 1.5 pim thick undoped GaN buffer layer on SiC substrate. The C3MOSHFET has an additional 10 nm thick SiO2 layer under the metal electrodes. No annealing was used in device fabrication. The length of the source and drain electrodes, L= 5 ptm; the gate length LG=1 ptm. The source-drain spacing is LDs=5jm. Total device width W= 2 x 125 ptm. High-frequency characteristics of C3devices were measured using HP 851 OC network analyzer. Above the contact cut-off frequency of around 1 GHz, the insertion loss is the same or lower than that of a regular HFET or MOSHFET with annealed contacts. The effective contact resistance extracted from the S-parameters was below 0.5 Q-mm. The power-handling capability of novel C3 transistors was characterized at 10 GHz. The most significant large-signal distortions in RF control devices manifest themselves as an increase in the subthreshold currents due to channel potential modulation; normally, this increase in the sub-threshold current impose the most critical limitation on the maximum operating RF powers. As a result, the typical maximum operating (switching) RF powers do not exceed 1W for GaAs devices and around 20 W for the AlGaN/GaN based HFETs. We have found that for the novel AlGaN/GaN C3 HFETs and C3MOSHFETs the maximum RF powers were around 10 times higher than those of HFET and MOSHFET devices with ohmic contacts. The highest maximum powers were achieved with the insulated gate C3MOSHFETs. Our estimations show that for 1 mm wide C3MOSHFETs the maximum RF powers are as high as 100 W. To the best of our knowledge these are the highest RF power densities ever achieved with the field-effect transistors. Further experiments and simulations showed that these record high switching powers are due to the self-modulation if the 2DEG density under the capacitively-coupled contacts by the large-amplitude RF input signals.
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