Ga_(1-x)Al_xAs/GaAs异质结构二维电子气晶体管(TEGFET)

制备了耗尽型和增强型TEGFET,耗尽TEGFE单栅长1μm,其室温跨导g_m=90mS/mm;双栅栅长均为2μm。g_m=75mS/mm。双栅的结果优于本实验室相同结构与尺寸的离子注入型常规双栅MESFET与高掺杂沟道MIS结构肖特基势垒FET的实验结果。双栅耗尽型器件在77K下跨导增加到1.7倍。双栅增强型的TEGFET在室温0.6V栅偏压下,g_m=63mS/mm,在77K下增加到1.4倍。如器件中出现平行电导时,则器件性能退化,它不但使跨导降低,且随栅编压变化很大。文中讨论了这一现象。     

MBE生长的跨导为186mS/mm的AlGaN/GaN HEMT

用分子束外延 ( MBE)技术研制出了 Al Ga N/Ga N高电子迁移率晶体管 ( HEMT)材料 ,其室温迁移率为 10 35cm2 /V· s、二维电子气浓度为 1.0× 10 13 cm - 2 ;77K迁移率为 2 6 53cm2 /V· s、二维电子气浓度为 9.6× 10 12 cm- 2 。用此材料研制了栅长为 1μm、栅宽为 80μm、源 -漏间距为 4μm的 Al Ga N/Ga N HEMT,其室温最大非本征跨导为 186 m S/mm、最大漏极饱和电流密度为 92 5m A/mm、特征频率为 18.8GH z。另外 ,还研制了具有 2 0个栅指 (总栅宽为 2 0× 80μm =1.6 mm )的大尺寸器件 ,该器件的最大漏极饱和电流为 1.33A。     

输出功率密度为2.23W/mm的X波段AlGaN/GaN功率HEMT器件

MOCVD技术在蓝宝石衬底上制备出具有高迁移率GaN沟道层的AlGaN/GaN HEMT材料.高迁移率GaN外延层的室温迁移率达741cm2/(V·s),相应背景电子浓度为1.52×1016cm-3;非有意掺杂高阻GaN缓冲层的室温电阻率超过108Ω·cm,相应的方块电阻超过1012Ω/□.50mm HEMT外延片平均方块电阻为440.9Ω/□,方块电阻均匀性优于96％.用此材料研制出了0.2μm栅长的X波段HEMT功率器件,40μm栅宽的器件跨导达到250mS/mm,特征频率fT为77GHz;0.8mm栅宽的器件电流密度达到1.07A/mm,8GHz时连续波输出功率为1.78W,相应功率密度为2.23W/mm,线性功率增益为13.3dB.     

输出功率密度为2.23W/mm的X波段AlGaN/GaN功率HEMT器件

MOCVD技术在蓝宝石衬底上制备出具有高迁移率GaN沟道层的AlGaN/GaN HEMT材料.高迁移率GaN外延层的室温迁移率达741cm2/(V·s),相应背景电子浓度为1.52×1016cm-3;非有意掺杂高阻GaN缓冲层的室温电阻率超过108Ω·cm,相应的方块电阻超过1012Ω/□.50mm HEMT外延片平均方块电阻为440.9Ω/□,方块电阻均匀性优于96％.用此材料研制出了0.2μm栅长的X波段HEMT功率器件,40μm栅宽的器件跨导达到250mS/mm,特征频率fT为77GHz;0.8mm栅宽的器件电流密度达到1.07A/mm,8GHz时连续波输出功率为1.78W,相应功率密度为2.23W/mm,线性功率增益为13.3dB.     

分子束外延AlGaN/GaN异质结场效应晶体管材料

用自组装的氨源分子束外延 (NH3-MBE)系统和射频等离子体辅助分子束外延 (PA-MBE)系统在 C面蓝宝石衬底上外延了优质 Ga N以及 Al Ga N/Ga N二维电子气材料。Ga N膜 (1 .2 μm厚 )室温电子迁移率达3 0 0 cm2 /V· s,背景电子浓度低至 2× 1 0 1 7cm- 3。双晶 X射线衍射 (0 0 0 2 )摇摆曲线半高宽为 6arcmin。 Al Ga N/Ga N二维电子气材料最高的室温和 77K二维电子气电子迁移率分别为 73 0 cm2 /V·s和 1 2 0 0 cm2 /V· s,相应的电子面密度分别是 7.6× 1 0 1 2 cm- 2和 7.1× 1 0 1 2 cm- 2 ;用所外延的 Al Ga N/Ga N二维电子气材料制备出了性能良好的 Al Ga N/Ga N HFET(异质结场效应晶体管 ) ,室温跨导为 5 0 m S/mm(栅长 1 μm) ,截止频率达 1 3 GHz(栅长 0 .5μm)。该器件在 3 0 0°C出现明显的并联电导 ,这可能是材料中的深中心在高温被激活所致     

RF-MBE生长AlGaN/GaN极化感应二维电子气材料

用射频等离子体辅助分子束外延技术(RF-MBE)在C面蓝宝石衬底上外延了高质量的GaN膜以及AlGaN/GaN极化感应二维电子气材料.所外延的GaN膜室温背景电子浓度为2×1017cm-a,相应的电子迁移率为177cm2/(V·s);GaN(0002)X射线衍射摇摆曲线半高宽(FWHM)为6′;AlGaN/GaN极化感应二维电子气材料的室温电子迁移率为730cm2/(V·s),相应的电子气面密度为7.6×1012cm-2;用此二维电子气材料制作的异质结场效应晶体管(HFET)室温跨导达50mS/mm(栅长1μm),截止频率达13GHz(栅长0.5μm).     

基于蓝宝石衬底的高性能AlGaN/GaN二维电子气材料与HEMT器件

利用低压MOCVD技术在蓝宝石衬底上生长了高性能的AlGaN/GaN二维电子气(2DEG)材料,室温和77K温度下的电子迁移率分别为946和2578cm2/(V*s),室温和77K温度下2DEG面密度分别为1.3×1013和1.27×1013cm-2.并利用AlGaN/GaN二维电子气材料制造出了高性能的HEMT器件,栅长为1μm,源漏间距为4μm,最大电流密度为485mA/mm(VG=1V),最大非本征跨导为170mS/mm(VG=0V),截止频率和最高振荡频率分别为6.7和24GHz.     

RF-MBE生长的AlGaN/GaN高电子迁移率晶体管特性

用射频分子束外延技术研制出了室温迁移率为1035cm2/(V·s),二维电子气浓度为1.0×1013cm-2,77K迁移率为2653cm2/(V·s),二维电子气浓度为9.6×1012cm-2的AlGaN/GaN高电子迁移率晶体管材料.用此材料研制的器件(栅长为1μm,栅宽为80μm,源-漏间距为4μm)的室温非本征跨导为186mS/mm,最大漏极饱和电流密度为925mA/mm,特征频率为18.8GHz.     

低噪声高电子迁移率晶体管

采用直接描绘电子束刻蚀法制造了用于低噪声极高频(EHF)放大器的亚半微米栅长的高电子迁移率晶体管。调制掺杂的外延结构是用分子束外延法生长的,在10~(12)电子/cm~2的电子浓度时,室温下的霍耳迁移率为8000cm~2/V·sec,液氮温度下为77,600cm~2/V·sec。通过腐蚀通n~+GaAs接触层的凹楷的方法确定了窄达0.28μm的栅长。0.4μm栅长的耗尽型器件的直流跨导超过260mS/mm。对0.37μm栅长的器件,进行了噪声系数和相关增益的测量,在34GHz下,得到了2.7dB的噪声系数和5.9dB的相关增益。还制造了具有240mS/mm跨导的增强型器件,对0.35μm的栅长,在18GHz下,它们的噪声系数为1.5dB,相关增益为10.5dB。这些结果可以和已报导过的最好的0.25μm栅长的GaAsMESFET的噪声系数相匹敌。     

基于蓝宝石衬底的高性能AlGaN/GaN二维电子气材料与HEMT器件

利用低压MOCVD技术在蓝宝石衬底上生长了高性能的Al Ga N/Ga N二维电子气(2 DEG)材料,室温和77K温度下的电子迁移率分别为94 6和2 5 78cm2 /(V·s) ,室温和77K温度下2 DEG面密度分别为1.3×10 1 3和1.2 7×10 1 3cm- 2 .并利用Al Ga N/Ga N二维电子气材料制造出了高性能的HEMT器件,栅长为1μm,源漏间距为4 μm,最大电流密度为4 85 m A/mm(VG=1V) ,最大非本征跨导为170 m S/mm(VG=0 V) ,截止频率和最高振荡频率分别为6 .7和2 4 GHz     

Enhancement of electron velocity in modulation-doped (Al,Ga)As/GaAs FETs at cryogenic temperatures

High-performance normally-off modulation-doped (Al,Ga)As/GaAs field-effect transistors with a 1 ?m gate length were fabricated and characterised. The transconductance obtained was 225 mS/mm at 300 K and 400 mS/mm at 77 K, leading to intrinsic transconductances (zero source resistance) of 305 and 565 mS/mm at 300 and 77 K, respectively. Since the device performance in short-gate transistors is limited by the electron saturation velocity, the increasing transconductance observed as the device is cooled is due to an increase in the electron velocity from about 2×107 cm/s to 3×107 cm/s. These velocities are inferred from a model developed for modulation-doped transistors and are predicted by pulse measurements in similar structures.     

High-performance modulation-doped GaAs integrated circuits with planar structures

A planar process of using proton isolation for modulationdoped GaAs/GaAlAs integrated circuits is presented. Devices with very low contact resistance (~ 5 × 10?7 ? cm2) and very high transconductance (~ 210 ms/mm) have been achieved. DCFL ring oscillators with 10 ?m switching FETs have been operated at ? = 36.6 ps at room temperature and 27.3 ps at 77 K. The lowest speed-power product is 2.43 fJ per gate.     

Depletion Mode HEMT with Refractory Metal Silicide WSi Gate

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DC and RF performance of LP-MOCVD grownAl0.25Ga0.75As/InxGa1-xAs(x=0.15-0.28) P-HEMT's with Si-delta doped GaAs layer

Si-delta-doped Al_0.25Ga_0.75As/In_xGa_1-xAs (x=0.15-0.28) P-HEMT's, prepared by LP-MOCVD, are investigated. The large conduction band discontinuity leads to 2-DEG density as high as 2.1×10¹²/cm² with an electron mobility of 7300 cm²/V·s at 300 K. The P-HEMT's with 0.7×60 μm gate have a maximum extrinsic transconductance of 380 mS/mm, and a maximum current density of 300 mA/mm. The S-parameter measurements indicate that the current gain and power gain cutoff frequencies are 30 and 61 GHz, respectively, The RF noise characteristics exhibit a minimum noise figure of 1.2 dB with an associated gain of 10 dB at 10 GHz. Due to the efficient doping technique, the electron mobility and transconductance obtained are among the best reported for MOCVD grown P-HEMT's with the similar structure     

MOCVD生长的SiC衬底高迁移率GaN沟道层AlGaN/AlN/GaN HEMT结构

用MOCVD技术在高阻6H-SiC衬底上研制出了具有高迁移率GaN沟道层的AlGaN/AlN/GaN高电子迁移率晶体管(HEMT)结构材料,其室温和80K时二维电子气迁移率分别为1944和11588cm2/(V·s),相应二维电子气浓度为1.03×1013cm-2;三晶X射线衍射和原子力显微镜分析表明该材料具有良好的晶体质量和表面形貌,10μm×10μm样品的表面粗糙度为0.27nm.用此材料研制出了栅长为0.8μm,栅宽为1.2mm的HEMT器件,最大漏极饱和电流密度和非本征跨导分别为957mA/mm和267mS/mm.     

Multiple-channel GaAs/AlGaAs high electron mobility transistors

Multiple-channel high electron mobility transistors (HEMT's) have been designed and fabricated on GaAs/AlGaAs heterostructural material grown by molecular beam epitaxy (MBE). The sheet carrier density of the two-dimensional electron gas (2-DEG) measured at 77 K was linearly proportional to the number of high mobility electron channels, and reached 5.3 × 10¹²cm^-2for six-channel HEMT structures. Depletion-mode devices of the double-heterojunction HEMT were operated between negative pinchoff voltage and forward-biased gate voltage without any transconductance degradation. A peak extrinsic transconductance of 360 mS/mm at 300 K and 550 mS/mm at 77 K has been measured for a 1-µm gate-length double-heterojunction enhancement-mode device. An extremely high drain current of 800 mA/mm with a gate-to-drain avalanche breakdown voltage of 9 V was measured on six-channel devices.     

A high-performance δ-dopedGaAs/InxGa1-xAs pseudomorphic high electronmobility transistor utilizing a graded InxGa1-xAschannel

A δ-doped GaAs/InGaAs/GaAs pseudomorphic high electron mobility transistor (HEMT) utilizing a graded In composition InGaAs channel grown by low-pressure metalorganic chemical vapor deposition was demonstrated. This structure had an extrinsic transconductance as high as 175 (245) mS/mm and a saturation current density a high as 500 (690) mA/mm at 300 (77) K for a gate length of 2 μm. The maximum transconductance versus gate bias extended over a broad and flat region of more than 2 V at 300 K. A low gate leakage current (<10 μA at -7 V) at 300 K was obtained     

A high-current drivability i-AlGaAs/n-GaAs doped-channel MIS-Like FET (DMT)

A high-current drivability doped-channel MIS-like FET (DMT) has been proposed. The DMT takes advantage of high saturation current with large transconductance and high breakdown voltage, in regard to its operating principle. The fabricated 0.5-µm gate DMT showed 310-mS/mm (410-mS/mm) transconductance and 650-mA/mm (800-mA/mm) maximum saturation current at room temperature (at 77 K). Output current values are about three or four times those for conventional two-dimensional electron gas (2DEG) FET's. Estimated average electron velocity is rather high, 1.5 × 10⁷cm/s (2 × 10⁷cm/s) at room temperature (77 K). In addition,f_{max}is as high as 41 GHz. fTis 45 GHz, which is the best data ever reported in 0.5-µm gate FET's.     

SiGe pMOSFET's with gate oxide fabricated by microwave electroncyclotron resonance plasma processing

A new process, electron cyclotron resonance (ECR) microwave plasma oxidation, has been developed to produce a gate-quality oxide directly on SiGe alloys. One μm Al gate Si_0.86Ge_0.15 p-metal-oxide-semiconductor field-effect-transistors (pMOSFET's) with ECR-grown gate oxide have been fabricated. It is found that saturation transconductance increases from 48 mS/mm at 300 K to 60 mS/mm at 77 K. Low field hole mobilities of 167 cm²/V-s at 300 K and 530 cm ²/V-s at 77 K have been obtained