30-nm-gate AlGaN/GaN MIS-HFETs with 180 GHz fT

M. Higashiwaki, T. Matsui, T. Mimura
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引用次数: 13

Abstract

AlGaN/GaN heterostructure field-effect transistors (HFETs) are excellent candidates for high power and high frequency applications operating in the millimeter-wave frequency range. Therefore, it is important to clarify how fast GaN HFETs can operate, because this will be key information to judge the frequency limit of GaN HFET applications. We recently reported AlGaN/GaN HFETs with a current-gain cutoff frequency (fT) of 163 GHz, which is a record for GaN transistors [1]. The high fT was achieved with our novel approach using high-Al-composition and extremely thin AlGaN barriers, SiN gate-insulating and passivation layers deposited by catalytic chemical vapor deposition (Cat-CVD), and 60-nm-long T-gates, which makes it possible to maintain a high aspect ratio for sub-0.1 -pim gates and suppress the short-channel effect. To enhance high-frequency characteristics, for the present work, we further decreased the gate length (LG) and fabricated 30-nm-gate AlGaN/GaN HFETs. The decrease in LG successfully resulted in the enhancement offT, which reached a new record of 180 GHz. Figure 1 shows a schematic cross section of the SiN(2 nm)/Alo.4Gao.6N(8 nm)/AlN(1.3 nm)/GaN(1500 nm) MIS-HFET. The structure was grown on a sapphire substrate by plasma-assisted molecular-beam epitaxy (PAMBE), and all of the epitaxial layers were nominally undoped. The patterning processes except for the gate finger were done by photolithography with a contact aligner. Device isolation was performed by mesa dry etching with C12/BCl3/Ar mixture gas. Source and drain ohmic contacts were formed by rapid thermal annealing of Ti/Al/Ni/Au at 820°C. The specific contact resistance was 3 x 10-6 Qcm2. Cat-CVD at 300°C was used to deposit a 2-nm-thick SiN film on the device. The SiN film worked not only as a passivation film but also as a gate-insulating layer. 30-nm-long T-shaped gates were defined by electron-beam (EB) lithography with a triple-layer resist, and gate metal with Ti/Pt/Au was deposited and lifted off. Finally, contact pad metal for probing with Ti/Au was deposited and lifted off. The source-drain spacing was 2 pim, and the gate width was 50x2 pim. Four-point van der Pauw Hall patterns were fabricated on the same wafer during the device processing. After SiN deposition, a mobility of 827 cm2/Vs, an electron density (Ns) of 2.07x1013 cm-2, and a sheet resistance (Rsh) of 364 Q/square were obtained for the HFET structure from the Hall effect measurement. The large Ns and low Rsh in spite of the thin AlGaN barrier were attributed to the Cat-CVD SiN passivation [2]. Figure 2 shows DC current-voltage (I-V) curves for the 30-nm-gate HFETs. The devices had a good pinch-off characteristic. The maximum drain current density (IDs) reached 1.49 A/mm for a gate bias of +1 V. Figure 3 shows the transfer characteristics for a drain bias of 2 V. The peak extrinsic transconductance (gm) was 402 mS/mm. Figure 4 shows the gate leakage current characteristics. The two-terminal reverse breakdown voltage, which was defined by a gate-drain leakage current density of 1 mA/mm, was about -18 V. Figures 5 and 6 show the current gain (H21), maximum stable gain (MSG), and unilateral gain (Ug) as a function of frequency. ThefT extracted from an extrapolation of H21 with -20 dB/decade was 180 GHz. The maximum oscillation frequency (fmax) for MSG and Ug were 185 and 189 GHz, which were obtained by extrapolations ofMSG with -20 dB/decade at 50 GHz and of Ug from 20 to 50 GHz with -20 dB/decade, respectively. The pad parasitic capacitances were de-embedded with the conventional Y-parameter subtraction method. To our knowledge, thef1 is a new record for GaN transistors. In conclusion, we fabricated 30-nm-long T-gate Al04Gao6N(8 nm)/GaN MIS-HFETs with a Cat-CVD SiN gate-insulating and passivation layer. The devices exhibited excellent DC and RF device characteristics; especially an excellentfT of 180 GHz. This work was partially supported by "The research and development project for expansion of radio spectrum resources" of the Ministry of Internal Affairs and Commnunications, Japan.
180ghz fet的30nm栅极AlGaN/GaN mishfet
AlGaN/GaN异质结构场效应晶体管(hfet)是毫米波频率范围内大功率高频应用的优秀候选者。因此,弄清GaN HFET的工作速度有多快是很重要的,因为这将是判断GaN HFET应用的频率限制的关键信息。我们最近报道了电流增益截止频率(fT)为163 GHz的AlGaN/GaN hfet,这是GaN晶体管的记录[1]。我们的新方法使用高铝成分和极薄的AlGaN势垒,催化化学气相沉积(Cat-CVD)沉积的SiN栅极绝缘和钝化层,以及60纳米长的t栅极来实现高fT,这使得保持低于0.1 -pim栅极的高宽高比并抑制短通道效应成为可能。为了提高高频特性,我们进一步减小栅极长度(LG),制备了30纳米栅极AlGaN/GaN hfet。LG的减少成功地导致了t的增强,达到了180 GHz的新记录。图1显示了SiN(2nm)/ alo4 gao的截面示意图。6N(8nm)/AlN(1.3 nm)/GaN(1500nm) miss - hfet。该结构通过等离子体辅助分子束外延(PAMBE)在蓝宝石衬底上生长,所有外延层名义上都未掺杂。除门指外的图案化过程是用接触对准器光刻完成的。用C12/BCl3/Ar混合气体进行台面干蚀刻,隔离器件。在820℃下对Ti/Al/Ni/Au材料进行快速热处理,形成源极和漏极欧姆触点。比接触电阻为3 × 10-6 Qcm2。在300°C下使用Cat-CVD在器件上沉积2nm厚的SiN薄膜。该薄膜不仅可以作为钝化膜,还可以作为栅极绝缘层。采用电子束(EB)光刻技术,用三层抗蚀剂定义了30nm长的t形栅极,并沉积和剥离了Ti/Pt/Au栅极金属。最后,沉积并取出用于Ti/Au探测的触点垫金属。源漏间距为2 pim,栅极宽度为50x2 pim。在器件加工过程中,在同一晶圆上制备了四点范德保霍尔图案。通过霍尔效应测量,得到了沉积后的HFET结构的迁移率为827 cm2/Vs,电子密度(Ns)为2.07x1013 cm-2,片电阻(Rsh)为364 Q/平方。尽管有较薄的AlGaN屏障,但仍有较大的Ns和较低的Rsh,这归因于Cat-CVD的SiN钝化[2]。图2显示了30nm栅极hfet的直流电流-电压(I-V)曲线。该器件具有良好的掐断特性。当栅极偏置为+ 1v时,最大漏极电流密度(IDs)达到1.49 A/mm。图3显示了漏极偏置为2 V时的传输特性。外源跨导峰值(gm)为402 mS/mm。图4显示了栅漏电流特性。双端反向击穿电压约为-18 V,由栅极漏极漏电流密度为1 mA/mm定义。图5和图6显示了电流增益(H21)、最大稳定增益(MSG)和单侧增益(Ug)作为频率的函数。从-20 dB/ 10的H21外推中提取的盗窃是180 GHz。MSG和Ug的最大振荡频率(fmax)分别为185 GHz和189 GHz,分别由MSG在50 GHz和Ug在20 ~ 50 GHz外推-20 dB/ 10年得到。采用传统的y参数减法对焊盘寄生电容进行了解嵌。据我们所知,这是氮化镓晶体管的新纪录。综上所述,我们制备了带有Cat-CVD SiN栅极绝缘和钝化层的30 nm长t栅al04高6n (8 nm)/GaN的mishfet。器件表现出优异的直流和射频器件特性;尤其是180千兆赫的高频率。这项工作得到了日本总务省“无线电频谱资源扩展研究与开发项目”的部分支持。
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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