低动态导通电阻千伏范围AlGaN/GaN hfet

N. Tipirneni, A. Koudymov, V. Adivarahan, J. Yang, G. Simin, M. Khan
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引用次数: 1

摘要

近年来,AlGaN/GaN异质结构场效应晶体管(hfet)被认为是功率转换和开关应用中有前途的新型构建模块。高压开关器件的关键挑战是同时实现高击穿电压的VBR和低导通电阻的RON。对于横向器件,RON最小化转化为实现具有最小栅极漏极间距LGD的给定VBR。在大多数报道的AlGaN/GaN HFET开关中,采用了场镀设计来实现高击穿电压[1,2]。在本文中,我们证明了在没有现场电镀的情况下,可以获得高于1 kV的高VBR值;我们首次证明了场极板在高压AlGaN/GaN开关中的重要作用是抑制由SiN钝化引起的过大的栅漏电流。这是首次报道动态RON低至4 mQ的AlGaN/GaN HFET。cm2在击穿电压VBR= 1000 V时。通常,高电压AlGaN/GaN hfet的VBR-LGD依赖性在大LGD值下饱和,限制了可实现的最大击穿电压低于400 - 800 V。最近,我们已经表明[3],在未钝化的HFET的VBR-LGD曲线中观察到的饱和是由于表面闪闪,而不是由于整体击穿。表面闪络的抑制导致VBRLGD线性依赖,最高可达LGD 20 ptm,击穿电压为1600V[3]。研究还表明,即使高VBR值仍然受到表面击穿而不是通道雪崩的限制。这些结果表明,在高压fEIFET设计中,通常使用的场极板并不需要达到高击穿电压。因此,需要修正场镀在提高高压大功率AlGaN-GaN HFET开关性能中的作用。在本文中,我们首次详细研究了场极板对用于大功率开关的hfet性能的影响。该器件是在蓝宝石衬底上制备的。晶圆片电阻在350q左右,阈值电压,VT =-6V。欧姆接触由Ti(200A)/Al(iooa)/Ti(500A)/Au(1500A)作为金属组合形成。这些材料在850°C的成形气体环境中退火1分钟。源极间距为2 ptm,栅极漏极间距为4 ~ 16 ptm。Au/Ni栅极形成后,对器件在空气环境和Flourinert®环境下的击穿电压进行了测试。正如预期的那样,VBR- lgd的依赖关系是线性的,产生了VBR
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Low Dynamic On-Resistance Kilovolt-Range AlGaN/GaN HFETs
In the recent years, AlGaN/GaN Heterostructure Field Effect Transistors (HFETs) have been recognized as promising novel building blocks for power conversion and switching applications. The key challenge in high-voltage switching devices is to achieving high breakdown voltage VBR and low on-resistance RON simultaneously. For lateral devices, the RON minimization translates into achieving a given VBR with a minimal gate drain spacing LGD. In most of the reported AlGaN/GaN HFET switches, the field-plated design was implemented to achieve high breakdown voltages [1, 2]. In this paper we demonstrate that high VBR values, above 1 kV, can be achieved without field-plating; we for the first time show that the essential role of the field-plate in high-voltage AlGaN/GaN switches is to suppress the excessive gate leakage currents arising from the SiN passivation. This is the first report of an AlGaN/GaN HFET with the dynamic RON as low as 4 mQ.cm2 at the breakdown voltage VBR= 1000 V. Commonly, the VBR-LGD dependencies for high-voltage AlGaN/GaN HFETs saturate at large LGD values limiting the achievable maximum breakdown voltages below 400 800 V. Recently, we have shown [3] that the saturation observed in the VBR-LGD curves for the unpassivated HFET is due to a surface flashover, not to a bulk breakdown. The suppression of the surface flashover leads to a linear VBRLGD dependence up to LGD 20 ptm resulting in the breakdown voltage of 1600V [3]. It was also shown that even that high VBR values were still limited by surface breakdown and not by the channel avalanche. These results imply that the field plate commonly used in the high-voltage fEIFET design is not required to achieve high breakdown voltage. Thus the role of field-plating in improving the performance of high-voltage high-power AlGaN-GaN HFET switches needs to be revised. In this paper, we present the first detailed study of the role of field plate on the performance of HFETs for high power switching. The fEIETs devices were fabricated over sapphire substrate. The wafer sheet resistance was around 350 Q, the threshold voltage, VT =-6V. The ohmic contacts were formed by Ti(200A)/Al(ioooA)/Ti(500A)/Au(1500A) as metal combination. These were annealed at 850 °C for 1 min. in a forming gas ambient. The source-gate spacing was 2 pim, gate drain spacing was varying from 4 to 16 ptm. After Au/Ni gate formation, the devices were tested for breakdown voltage in air ambience and in Flourinert® ambience. As expected the VBR-LGD dependence was linear yielding the VBR
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