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1.
制作了蓝宝石衬底上生长的AlGaN/GaN高电子迁移率晶体管.0V栅压下,0.3μm栅长、100μm栅宽的器件的饱和漏电流密度为0.85A/mm,峰值跨导为225mS/mm;特征频率和最高振荡频率分别为45和100GHz;4GHz频率下输出功率密度和增益分别为1.8W/mm和9.5dB,8GHz频率下输出功率密度和增益分别为1.12W/mm和11.5dB.  相似文献   

2.
砷化镓PHEMT功率器件具有工作频率高,输出功率密度大,效率高,功率增益高等特点,我们研制的0.5μm栅长GaAsPHEMT小功率晶体管,栅宽1mm,直流跨导250ms/mm,栅漏反向击穿电压大于13V,在20GHz下最大可用增益为8dB,X波段输出功率为0.8W/mm,可应用于22GHz以下的窄带功率放大器和18GHz以下的宽带功率放大器。  相似文献   

3.
在6H-SiC衬底上,外延生长了AlGaN/GaN HEMT结构,设计并实现了高性能1mm AlGaN/GaN微波功率HEMT,外延材料利用金属有机物化学气相淀积技术生长.测试表明,该lmm栅宽器件栅长为0.8μm,输出电流密度达到1.16A/mm,跨导为241mS/mm,击穿电压>80V,特征频率达到20GHz,最大振荡频率为28GHz.5.4GHz连续波测试下功率增益为14.2dB,输出功率达4.1W,脉冲条件测试下功率增益为14.4dB,输出功率为5.2W,两端口阻抗特性显示了在微波应用中的良好潜力.  相似文献   

4.
在6H-SiC衬底上,外延生长了AlGaN/GaN HEMT结构,设计并实现了高性能1mm AlGaN/GaN微波功率HEMT,外延材料利用金属有机物化学气相淀积技术生长.测试表明,该lmm栅宽器件栅长为0.8μm,输出电流密度达到1.16A/mm,跨导为241mS/mm,击穿电压>80V,特征频率达到20GHz,最大振荡频率为28GHz.5.4GHz连续波测试下功率增益为14.2dB,输出功率达4.1W,脉冲条件测试下功率增益为14.4dB,输出功率为5.2W,两端口阻抗特性显示了在微波应用中的良好潜力.  相似文献   

5.
我们实验室研制的0.25μm栅长掺杂沟道PHEMT,在毫米波频率下已显示出优良的功率性能,44GHz下的输出功率密度和功率附加效率分别为0.93W/mm和41%,用这些器件已研制出两种Q波段混合功率放大器。二级放大器输出功率为108mW,相应功率增益为9.5dB,功率附加效率为26.5%;三级放大器输出功率达251mW,功率增益为13.6dB,功率附加效率为26.8%。当加上不同偏压时,三级放大器的峰值效率可达31.3%。这两种放大器的线性增益分别为12dB和20dB。这些结果清楚地表明这些器件能够用于毫米波发射器。  相似文献   

6.
报道了研制的AlGaN/GaN微波功率HEMT,该器件采用以蓝宝石为衬底的非掺杂AlGaN/GaN异质结构,器件工艺采用了Ti/Al/Ni/Au欧姆接触和Ni/Au肖特基势垒接触以及SiN介质进行器件的钝化.研制的200μm栅宽T型布局AlGaN/GaN HEMT在1.8GHz,Vds=30V时输出功率为28.93dBm,输出功率密度达到3.9W/mm,功率增益为15.59dB,功率附加效率(PAE)为48.3%.在6.2GHz,Vds=25V时该器件输出功率为27.06dBm,输出功率密度为2.5W/mm,功率增益为10.24dB,PAE为35.2%.  相似文献   

7.
使用自主研制的SiC衬底GaN HEMT外延材料,研制出高输出功率AlGaN/GaN HEMT,优化了器件研制工艺,比接触电阻率小于1.0×10-6Ω·cm2,电流崩塌参量小于10%,击穿电压大于80V.小栅宽器件工作电压达到40V,频率为8GHz时输出功率密度大于10W/mm.栅宽为2mm单胞器件,工作电压为28V,频率为8GHz时,输出功率为12.3W,功率增益为4.9dB,功率附加效率为35%.四胞内匹配总栅宽为8mm器件,工作电压为27V时,频率为8GHz时,输出功率为33.8W,功率增益为6.3dB,功率附加效率为41.77%,单胞器件和内匹配器件输出功率为目前国内该器件输出功率的最高结果.  相似文献   

8.
使用自主研制的SiC衬底GaN HEMT外延材料,研制出高输出功率AlGaN/GaN HEMT,优化了器件研制工艺,比接触电阻率小于1.0×10-6Ω·cm2,电流崩塌参量小于10%,击穿电压大于80V.小栅宽器件工作电压达到40V,频率为8GHz时输出功率密度大于10W/mm.栅宽为2mm单胞器件,工作电压为28V,频率为8GHz时,输出功率为12.3W,功率增益为4.9dB,功率附加效率为35%.四胞内匹配总栅宽为8mm器件,工作电压为27V时,频率为8GHz时,输出功率为33.8W,功率增益为6.3dB,功率附加效率为41.77%,单胞器件和内匹配器件输出功率为目前国内该器件输出功率的最高结果.  相似文献   

9.
基于SiC衬底成功研制X波段0.25μm栅长带有Γ栅场板结构的AlGaN/GaN HEMT,对比T型栅结构器件,研究了Γ栅场板引入对器件直流、小信号及微波功率特性的影响。结果表明,Γ栅场板结构减小器件截止频率及振荡频率,但明显改善器件膝点电压和输出功率密度。针对场板长度分别为0.4、0.7、0.9、1.1μm,得出一定范围内增加场板长度,器件输出功率大幅度提高,并结合器件小信号模型提参结果分析原因。在频率8 GHz下,总栅宽1 mm,场板长度0.9μm的器件,连续波输出功率密度7.11 W/mm,功率附加效率(PAE)35.31%,相应线性增益10.25 dB。  相似文献   

10.
报道了W波段GaN三级放大电路的研制结果。采用电子束直写工艺在AlGaN/GaN HEMT外延结构上制备了栅长100nm的"T"型栅结构。器件直流测试最大电流密度为1.3A/mm,最大跨导为430mS/mm;小信号测试外推其fT和fmax分别为90GHz及210GHz。采用该器件设计了三级放大电路,在75~110GHz频段内最大小信号增益为21dB。该单片在90GHz处的最大输出功率可达1.117W,PAE为13%,功率增益为11dB,输出功率密度为2.33 W/mm。  相似文献   

11.
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.  相似文献   

12.
This Daper describes the first domestic Ku-band power AlGaN/GaN HEMT fabricated on a sapphire substrate.The device with a gate width of 0.5 mm and a gate length of 0.35 μm has exhibited an extrinsic current gain cutoff frequency of 20 GHz and an extrinsic maximum frequency of oscillation of 75 GHz.Under V_(DS)=30 V, CW operating conditions at 14 GHz,the device exhibits a linear gain of 10.4 dB and a 3-dB-gain-compressed output power of 1.4 W with a Dower added efficiency of 41%.Under pulse operating conditions,the linear gain is 12.8 dB and the 3-dB-compressed output power is 1.7 W The power density reaches 3.4 W/mm.  相似文献   

13.
State-of-the-art AlGaN/GaN high electron mobility structures were grown on semi-insulating 4H-SiC substrates by MOCVD and X-band microwave power high electron mobility transistors were fabricated and characterized.Hall mobility of 2291.1 cm2/(V·s) and two-dimensional electron gas density of 9.954 × 1012 cm-2 were achieved at 300 K.The HEMT devices with a 0.45-μm gate length exhibited maximum drain current density as high as 1039.6 mA/mm and peak extrinsic transconduct-ance of 229.7 mS/mm.The fT of 30.89 GHz and fmax of 38.71 GHz were measured on the device.Load-pull measurements were performed and analyzed under (-3.5,28) V,(-3.5,34) V and (-3.5,40) V gate/drain direct current bias in class-AB,respectively.The uncooled device showed high linear power gain of 17.04 dB and high power-added efficiency of 50.56% at 8 GHz when drain biased at (-3.5,28) V.In addition,when drain biased at (-3.5,40) V,the device exhibited a saturation output power dens-ity up to 6.21 W/mm at 8 GHz,with a power gain of 11.94 dB and a power-added efficiency of 39.56%.Furthermore,the low fmax/fT ratio and the variation of the power sweep of the device at 8 GHz with drain bias voltage were analyzed.  相似文献   

14.
AlGaN-GaN HEMTs on Si with power density performance of 1.9 W/mm at 10 GHz   总被引:1,自引:0,他引:1  
AlGaN-GaN high electron mobility transistors (HEMTs) on silicon substrate are fabricated. The device with a gate length of 0.3-/spl mu/m and a total gate periphery of 300 /spl mu/m, exhibits a maximum drain current density of 925 mA/mm at V/sub GS/=0 V and V/sub DS/=5 V with an extrinsic transconductance (g/sub m/) of about 250 mS/mm. At 10 GHz, an output power density of 1.9 W/mm associated to a power-added efficiency of 18% and a linear gain of 16 dB are achieved at a drain bias of 30 V. To our knowledge, these power results represent the highest output power density ever reported at this frequency on GaN HEMT grown on silicon substrates.  相似文献   

15.
Microwave frequency capabilities of AlGaN/GaN high electron mobility transistors (HEMTs) on high resistive silicon (111) substrate for power applications are demonstrated in this letter. A maximum dc current density of 1 A/mm and an extrinsic current gain cutoff frequency (F/sub T/) of 50 GHz are achieved for a 0.25 /spl mu/m gate length device. Pulsed and large signal measurements show the good quality of the epilayer and the device processing. The trapping phenomena are minimized and consequently an output power density of 5.1 W/mm is reached at 18 GHz on a 2/spl times/50/spl times/0.25 /spl mu/m/sup 2/ HEMT with a power gain of 9.1dB.  相似文献   

16.
This paper describes the small-signal characterization through delay-time analysis and high-power operation of the Ka-band of AlGaN/GaN heterojunction field-effect transistors (FETs). An FET with a gatewidth of 100 /spl mu/m and a gate length of 0.09 /spl mu/m has exhibited a current gain cutoff frequency (f/sub T/) of 81 GHz, a maximum frequency of oscillation (fmax) of 187 GHz, and a maximum stable gain of 10.5 dB at 30 GHz (8.3 dB at 60 GHz). Delay-time analysis has demonstrated channel electron velocities of 1.50/spl times/10/sup 7/ to 1.75/spl times/10/sup 7/ cm/s in a gate-length range of 0.09-0.25 /spl mu/m. State-of-the-art performance-saturated power of 5.8 W with a linear gain of 9.2 dB and a power-added efficiency of 43.2%-has been achieved at 30 GHz using a single chip having a gatewidth of 1.0 mm and a gate length of 0.25 /spl mu/m.  相似文献   

17.
The RF and dc characteristics of microwave power double-heterojunction HEMt's (DH-HEMT's) with low doping density have been studied. Small-signal RF measurements indicated that the cutoff frequency and the maximum frequency of oscillation in DH-HEMT's with 0.8-1 µm gate length and 1.2 mm gate periphery are typically 11- 16 GHz and 36-41 GHz, respectively. However, the cutoff frequency in DH-HEMT's degrades strongly with increasing drain bias voltage. This may be caused by both effects of increasing effective transit length of electrons and decreasing average electron velocity, due to Gunn domain formation. In large-signal microwave measurement, the DH-HEMT (2.4 mm gate periphery) delivered a maximum output power of 1.05 W with 2.8 dB gain and 0.58 W with 1.6 dB gain at 20 and 30 GHz, respectively. These are the highest output powers yet reported for HEMT devices. For the dc characteristics, the onset of two-terminal gate breakdown voltage is found to correlate with the drain current Idssand recessed length, and three-terminal source-drain breakdown characteristics near pinchoff are limited by the gate-drain breakdown. A simple model on gate breakdown voltage in HEMT is also presented.  相似文献   

18.
The microwave characteristics at 18 and 20 GHz of submicron-gate indium phosphide (InP) metal-insulator-semiconductor field-effect transistors (MISFETs) for high output power density applications are presented. InP power MISFETs were fabricated with 0.7 μm gate lengths, 0.2 mm gate widths, and drain-source spacings of 2, 3 and 5 μm. The output power density was investigated as a function of drain-source spacing. The best output power density and gain were obtained for drain-source spacings of 3 μm. At 18 GHz output power densities of 1.59 W/mm with a gain of 3.47 dB and a power-added efficiency of 20.0% were obtained for a drain-source spacing of 3 μm. At 20 GHz output power densities of 1.20 W/mm with a gain of 3.17 dB and a power-added efficiency of 13.6% were obtained for a drain-source spacing of 3 μm  相似文献   

19.
5G 通信中3. 4~3. 6 GHz 是主要使用频段。GaN 射频器件由于高频、低功耗、高线性度等优势,满足5G 通信应用需求。文中在高阻硅基GaN 外延片上研制了AlGaN/GaN 高电子迁移率晶体管(High Electron Mobility Transistor, HEMT),并分析了金属鄄绝缘层鄄半导体(Metal-Insulator-Semiconductor,MIS)栅对器件直流和射频特性的影响。研究发现:相比于肖特基栅结构,MIS 栅结构器件栅极泄漏电流减少2~5 个数量级,漏极驱动电流能力和跨导提高10%以上;频率为3. 5 GHz 时,增益从1. 5 dB 提升到4. 0 dB,最大资用增益从5. 2 dB 提升到11. 0 dB,电流增益截止频率为8. 3 GHz,最高振荡频率为10. 0 GHz。  相似文献   

20.
正AlGaN/GaN HEMTs with 0.2μm V-gate recesses were developed.The 0.2μm recess lengths were shrunk from the 0.6μm designed gate footprint length after isotropic SiN deposition and anisotropic recessed gate dry etching.The AlGaN/GaN HEMTs with 0.2μm V-gate recesses on sapphire substrates exhibited a current gain cutoff frequency f_t of 35 GHz and a maximum frequency of oscillation f_(max) of 60 GHz.At 10 GHz frequency and 20 V drain bias,the V-gate recess devices exhibited an output power density of 4.44 W/mm with the associated power added efficiency as high as 49%.  相似文献   

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