18 GHz时功率密度为9.1 W/mm的现场镀AlGaN/GaN hemt

V. Kumar, G. Chen, S. Guo, B. Peres, I. Adesida
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The AlGaN HEMT structure used in the present study was grown on 6H-SiC substrates by metal organic chemical vapor deposition (MOCVD). The epilayer consists of an AlN buffer, 1.5 pm undoped GaN, and a 20 mm Al.30Ga70N barrier layer. Average sheet resistance across the as-grown wafer was 380 Q/sq as measured by Leighton. Device fabrication started with mesa isolation using C12/Ar plasma in an inductively-coupled-plasma reactive ion etch (ICP-RIE) system. Alloyed ohmic contacts of Ti/Al/Mo/Au were formed at 850°C with a low contact resistance of 0.15 ohm-mm. The source-drain spacing for these devices was 2.7 jim. Next, silicon nitride was deposited using PECVD system. Then 0.25 gm gatefootprints were patterned using e-beam lithography and etched through the silicon nitride film in a RIE system. The distance between the gate-footprint and source contact was 0.8 gm for all transistors. Finally, Ni/Au (300/2500 A) gamma-gates with different side-lobe lengths on the drain side were deposited by ebeam evaporation. Three side-lobe (field-plate) lengths were designed: 0.9, 1.2, and 1.5 jm. The devices had a total gate width of 100 jm. On-wafer DC measurements were performed using an HP4145B semiconductor parameter analyzer. Devices with different lengths of field plates had similar dc characteristics. Figure 1 shows a typical drain current-voltage (ID-VDS) characteristics for the device with a field plate length (LFP) of 1.5 jm. The gate was biased from -5 V to 2 V in a step of 1 V. The devices exhibited a maximum drain current density (ID,.) of 1.42 A/mm at a gate bias of 2 V and a drain bias of 9 V. The DC transfer characteristics for this device are shown in Fig. 2. The drain was biased at 7 V. A peak extrinsic transconductance (gm) of 437 mS/mm was measured at Vg, = -3.2 V. The high value of gm is attributed to the thin AlGaN barrier layer and the low contact resistance. On-wafer small signal RF measurements were carried out using a Cascade Microtech Probe and an HP851OC network analyzer. With the increase of field plate length from 0.9 to 1.5 pm, the cut-off frequency (fT) decreased from 50 to 41 GHz while the maximum frequency of oscillation (fm) degraded from 81 to 63 GHz. This is attributed to an increase in the gate-drain capacitance. Figure 3 shows the small signal RF performance of the device with the field plate length (LFp) of 1.5 lim. Large signal CW measurements at 18 GHz were performed using a Focus Microwave automatic load pull system. The data were taken on-wafer at room temperature without any thermal management. At a drain bias of 40 V, power densities of 5.4, 6.4 and 7.3 W/mm were measured for devices with LFP of 0.9, 1.2 and 1.5 jm, respectively. Large signal performance of the device with L+p of 1.5 jm at a drain bias of 55 V is shown in Fig. 4. The device has an output power of 29.57 dBm corresponding to 9.1 W/mm with an associated gain of 5.8 dB and PAE of 23.7 %. In summar, we have presented the CW power performance of 0.25 gm gate-length AlGaN/GaN HEMTs with field plates at 18 GHz. These results demonstrate the exceptional potential ofthese devices for high power applications beyond X band. [1] Y.-F. Wu et al., \"30 W/mm GaN HEMTs by Field Plate Optimization\", Electron Dev. Lett., vol. 25, p. 117 (2004) [2] R. Thompson et al., \"Performance of the AlGaN HEMT structure With a Gate Extension\" IEEE Trans. Electron Dev., vol. 51, p. 292 (2004)","PeriodicalId":306160,"journal":{"name":"63rd Device Research Conference Digest, 2005. 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Though GaN HEMTs using field plate have demonstrated power densities as high as 32W/mm at 4 GHz, however to date, there have been only few reports on field-plated devices up to X band [1,2]. In this paper, we present record power performance of AlGaN/GaN HEMTs on 6H-SiC substrates at 18 GHz. A CW output power density of 9.1 W/mm with a gain of 5.8 dB and power added efficiency of 23.7 % were achieved. The AlGaN HEMT structure used in the present study was grown on 6H-SiC substrates by metal organic chemical vapor deposition (MOCVD). The epilayer consists of an AlN buffer, 1.5 pm undoped GaN, and a 20 mm Al.30Ga70N barrier layer. Average sheet resistance across the as-grown wafer was 380 Q/sq as measured by Leighton. Device fabrication started with mesa isolation using C12/Ar plasma in an inductively-coupled-plasma reactive ion etch (ICP-RIE) system. Alloyed ohmic contacts of Ti/Al/Mo/Au were formed at 850°C with a low contact resistance of 0.15 ohm-mm. The source-drain spacing for these devices was 2.7 jim. Next, silicon nitride was deposited using PECVD system. Then 0.25 gm gatefootprints were patterned using e-beam lithography and etched through the silicon nitride film in a RIE system. The distance between the gate-footprint and source contact was 0.8 gm for all transistors. Finally, Ni/Au (300/2500 A) gamma-gates with different side-lobe lengths on the drain side were deposited by ebeam evaporation. Three side-lobe (field-plate) lengths were designed: 0.9, 1.2, and 1.5 jm. The devices had a total gate width of 100 jm. On-wafer DC measurements were performed using an HP4145B semiconductor parameter analyzer. Devices with different lengths of field plates had similar dc characteristics. Figure 1 shows a typical drain current-voltage (ID-VDS) characteristics for the device with a field plate length (LFP) of 1.5 jm. The gate was biased from -5 V to 2 V in a step of 1 V. The devices exhibited a maximum drain current density (ID,.) of 1.42 A/mm at a gate bias of 2 V and a drain bias of 9 V. The DC transfer characteristics for this device are shown in Fig. 2. The drain was biased at 7 V. A peak extrinsic transconductance (gm) of 437 mS/mm was measured at Vg, = -3.2 V. The high value of gm is attributed to the thin AlGaN barrier layer and the low contact resistance. On-wafer small signal RF measurements were carried out using a Cascade Microtech Probe and an HP851OC network analyzer. With the increase of field plate length from 0.9 to 1.5 pm, the cut-off frequency (fT) decreased from 50 to 41 GHz while the maximum frequency of oscillation (fm) degraded from 81 to 63 GHz. This is attributed to an increase in the gate-drain capacitance. Figure 3 shows the small signal RF performance of the device with the field plate length (LFp) of 1.5 lim. Large signal CW measurements at 18 GHz were performed using a Focus Microwave automatic load pull system. The data were taken on-wafer at room temperature without any thermal management. At a drain bias of 40 V, power densities of 5.4, 6.4 and 7.3 W/mm were measured for devices with LFP of 0.9, 1.2 and 1.5 jm, respectively. Large signal performance of the device with L+p of 1.5 jm at a drain bias of 55 V is shown in Fig. 4. The device has an output power of 29.57 dBm corresponding to 9.1 W/mm with an associated gain of 5.8 dB and PAE of 23.7 %. In summar, we have presented the CW power performance of 0.25 gm gate-length AlGaN/GaN HEMTs with field plates at 18 GHz. These results demonstrate the exceptional potential ofthese devices for high power applications beyond X band. [1] Y.-F. Wu et al., \\\"30 W/mm GaN HEMTs by Field Plate Optimization\\\", Electron Dev. Lett., vol. 25, p. 117 (2004) [2] R. Thompson et al., \\\"Performance of the AlGaN HEMT structure With a Gate Extension\\\" IEEE Trans. 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引用次数: 3

摘要

AlGaN/GaN高电子迁移率晶体管(hemt)由于其优越的材料特性,是室温和高温下高功率和高频应用的优秀候选者。由于材料生长和加工技术的改进,微波功率密度已被证明比相应的gaas基器件高5到10倍。尽管使用场极板的GaN hemt已经证明在4ghz时功率密度高达32W/mm,但迄今为止,关于高达X波段的场极板器件的报道很少[1,2]。在本文中,我们提出了在18 GHz的6H-SiC衬底上的AlGaN/GaN hemt的创纪录功率性能。连续波输出功率密度为9.1 W/mm,增益为5.8 dB,功率增加效率为23.7%。本研究采用金属有机化学气相沉积(MOCVD)在6H-SiC衬底上生长AlGaN HEMT结构。涂层由AlN缓冲层、1.5 pm未掺杂的GaN和20 mm Al.30Ga70N阻挡层组成。Leighton测量的生长晶圆上的平均薄片电阻为380 Q/sq。在电感耦合等离子体反应离子蚀刻(ICP-RIE)系统中,使用C12/Ar等离子体进行台面隔离,开始器件制造。在850℃下形成Ti/Al/Mo/Au合金欧姆接触,接触电阻低至0.15 ω -mm。这些器件的源漏间距为2.7 jim。然后,利用PECVD系统沉积氮化硅。然后用电子束光刻技术刻制0.25 gm栅极足迹,并在RIE系统中通过氮化硅薄膜蚀刻。对于所有晶体管,栅极足迹和源触点之间的距离为0.8 gm。最后通过电子束蒸发在漏侧沉积不同旁瓣长度的Ni/Au (300/2500 A) γ门。设计了三个旁瓣(场板)长度:0.9、1.2和1.5 jm。这些器件的总栅极宽度为100 jm。晶圆上直流测量使用HP4145B半导体参数分析仪进行。不同场强板长度的器件具有相似的直流特性。图1显示了该器件在场极板长度(LFP)为1.5 jm时的典型漏极电流-电压(ID-VDS)特性。栅极在1 V的阶跃中从-5 V偏置到2 V。在栅极偏置2 V和漏极偏置9 V时,器件的最大漏极电流密度(ID,.)为1.42 a /mm。该器件的直流传输特性如图2所示。漏极偏置在7伏。在Vg = -3.2 V时,测量到的峰值外部跨导(gm)为437 mS/mm。高的gm值归因于较薄的AlGaN阻挡层和较低的接触电阻。晶圆上小信号射频测量使用级联微探针和HP851OC网络分析仪进行。随着场板长度从0.9 pm增加到1.5 pm,截止频率从50 GHz降低到41 GHz,最大振荡频率从81 GHz降低到63 GHz。这归因于栅极-漏极电容的增加。图3显示了场板长度(LFp)为1.5 lim时器件的小信号射频性能。采用Focus Microwave自动负载牵引系统进行了18 GHz的大信号连续波测量。这些数据是在没有任何热管理的情况下,在室温下进行的。在漏极偏置为40 V时,LFP分别为0.9、1.2和1.5 jm的器件的功率密度分别为5.4、6.4和7.3 W/mm。图4显示了该器件在漏极偏置为55 V时,L+p为1.5 jm时的大信号性能。该器件的输出功率为29.57 dBm,对应9.1 W/mm,相关增益为5.8 dB, PAE为23.7%。综上所述,我们已经展示了在18 GHz下具有场板的0.25 gm门长AlGaN/GaN hemt的连续波功率性能。这些结果证明了这些器件在X波段以外的高功率应用中的卓越潜力。[1] Y.-F。Wu et al.,“30 W/mm GaN HEMTs的场极板优化”,《电子开发》。[2]陈志强,“基于栅极扩展的AlGaN HEMT结构性能研究”,电子工程学报,vol. 25, p. 117(2004)。电子发展,vol. 51, p. 292 (2004)
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Field-plated AlGaN/GaN HEMTs with power density of 9.1 W/mm at 18 GHz
AlGaN/GaN high electron mobility transistors (HEMTs) are excellent candidates for high power and high frequency applications at room and elevated temperatures due to their superior material properties. As a result of improved material growth and processing technologies, microwave power densities have been demonstrated that are five to ten times greater than that of corresponding GaAs-based devices. Though GaN HEMTs using field plate have demonstrated power densities as high as 32W/mm at 4 GHz, however to date, there have been only few reports on field-plated devices up to X band [1,2]. In this paper, we present record power performance of AlGaN/GaN HEMTs on 6H-SiC substrates at 18 GHz. A CW output power density of 9.1 W/mm with a gain of 5.8 dB and power added efficiency of 23.7 % were achieved. The AlGaN HEMT structure used in the present study was grown on 6H-SiC substrates by metal organic chemical vapor deposition (MOCVD). The epilayer consists of an AlN buffer, 1.5 pm undoped GaN, and a 20 mm Al.30Ga70N barrier layer. Average sheet resistance across the as-grown wafer was 380 Q/sq as measured by Leighton. Device fabrication started with mesa isolation using C12/Ar plasma in an inductively-coupled-plasma reactive ion etch (ICP-RIE) system. Alloyed ohmic contacts of Ti/Al/Mo/Au were formed at 850°C with a low contact resistance of 0.15 ohm-mm. The source-drain spacing for these devices was 2.7 jim. Next, silicon nitride was deposited using PECVD system. Then 0.25 gm gatefootprints were patterned using e-beam lithography and etched through the silicon nitride film in a RIE system. The distance between the gate-footprint and source contact was 0.8 gm for all transistors. Finally, Ni/Au (300/2500 A) gamma-gates with different side-lobe lengths on the drain side were deposited by ebeam evaporation. Three side-lobe (field-plate) lengths were designed: 0.9, 1.2, and 1.5 jm. The devices had a total gate width of 100 jm. On-wafer DC measurements were performed using an HP4145B semiconductor parameter analyzer. Devices with different lengths of field plates had similar dc characteristics. Figure 1 shows a typical drain current-voltage (ID-VDS) characteristics for the device with a field plate length (LFP) of 1.5 jm. The gate was biased from -5 V to 2 V in a step of 1 V. The devices exhibited a maximum drain current density (ID,.) of 1.42 A/mm at a gate bias of 2 V and a drain bias of 9 V. The DC transfer characteristics for this device are shown in Fig. 2. The drain was biased at 7 V. A peak extrinsic transconductance (gm) of 437 mS/mm was measured at Vg, = -3.2 V. The high value of gm is attributed to the thin AlGaN barrier layer and the low contact resistance. On-wafer small signal RF measurements were carried out using a Cascade Microtech Probe and an HP851OC network analyzer. With the increase of field plate length from 0.9 to 1.5 pm, the cut-off frequency (fT) decreased from 50 to 41 GHz while the maximum frequency of oscillation (fm) degraded from 81 to 63 GHz. This is attributed to an increase in the gate-drain capacitance. Figure 3 shows the small signal RF performance of the device with the field plate length (LFp) of 1.5 lim. Large signal CW measurements at 18 GHz were performed using a Focus Microwave automatic load pull system. The data were taken on-wafer at room temperature without any thermal management. At a drain bias of 40 V, power densities of 5.4, 6.4 and 7.3 W/mm were measured for devices with LFP of 0.9, 1.2 and 1.5 jm, respectively. Large signal performance of the device with L+p of 1.5 jm at a drain bias of 55 V is shown in Fig. 4. The device has an output power of 29.57 dBm corresponding to 9.1 W/mm with an associated gain of 5.8 dB and PAE of 23.7 %. In summar, we have presented the CW power performance of 0.25 gm gate-length AlGaN/GaN HEMTs with field plates at 18 GHz. These results demonstrate the exceptional potential ofthese devices for high power applications beyond X band. [1] Y.-F. Wu et al., "30 W/mm GaN HEMTs by Field Plate Optimization", Electron Dev. Lett., vol. 25, p. 117 (2004) [2] R. Thompson et al., "Performance of the AlGaN HEMT structure With a Gate Extension" IEEE Trans. Electron Dev., vol. 51, p. 292 (2004)
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