首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 140 毫秒
1.
非掺杂AlGaN/GaN微波功率HEMT   总被引:9,自引:4,他引:5  
报道了研制的Al Ga N / Ga N微波功率HEMT,该器件采用以蓝宝石为衬底的非掺杂Al Ga N/ Ga N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Si N介质进行器件的钝化.研制的2 0 0μm栅宽T型布局Al Ga N / Ga N HEMT在1.8GHz,Vds=30 V时输出功率为2 8.93d Bm,输出功率密度达到3.9W/mm ,功率增益为15 .5 9d B,功率附加效率(PAE)为4 8.3% .在6 .2 GHz,Vds=2 5 V时该器件输出功率为2 7.0 6 d Bm ,输出功率密度为2 .5 W/ mm ,功率增益为10 .2 4 d B,PAE为35 .2 % .  相似文献   

2.
南京电子器件研究所于 2 0 0 0年进行了 Ga As功率 PHEMT的研究开发 ,完成了“WC2 0 0 3型高电子迁移率功率晶体管”项目的设定和 Ku波段 1 0 W功率 PHEMT的研制。WC2 0 0 3型器件在 9.4~ 9.9GHz带内 ,输出功率大于 2 .5W,功率增益大于 9.5d B,功率附加效率典型值为 40 % ,带内增益起伏小于± 0 .5d B,该器件的栅宽为 4.8mm。采用两个 9.6mm栅宽功率 PHEMT管芯合成研制的 Ku波段内匹配功率 PHEMT,在 1 0 .5~ 1 1 .3GHz带内 ,输出功率大于 9.8W,带内最大输出功率为 1 0 .9W,功率增益大于 9.9d B,功率附加效率典型值为 40 %…  相似文献   

3.
跨导为220 mS/mm的AlGaN/GaNHEMT   总被引:2,自引:1,他引:1  
介绍了 Al Ga N/ Ga N HEMT器件的研制及室温下器件特性的测试。漏源欧姆接触采用 Ti/ Al/ Pt/ Au,肖特基结金属为 Pt/ Au。器件栅长为 1 μm,获得最大跨导 2 2 0 m S/ mm,最大的漏源饱和电流密度 0 .72 A/ mm。由 S参数测量推出器件的截止频率和最高振荡频率分别为 1 2 GHz和 2 4GHz。  相似文献   

4.
Ka波段PHEMT功率放大器   总被引:1,自引:0,他引:1  
报道了 Ka波段的 PHEMT功率放大器的设计和研制。 PHEMT器件采用 0 .2 μm栅长的 Φ 76 mm Ga As工艺制作 ,并利用 CAD技术指导材料生长和器件制作。单级的 MIC放大器采用0 .3mm栅宽的 PHEMT,在 34GHz处 ,输出功率 10 0 m W,功率增益 4 d B。  相似文献   

5.
介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果. 制作了几种0.6μm栅长、100~1000μm不同栅宽的器件,对于栅宽分别为100, 300和500μm的器件,典型最大跨导为190~170mS/mm;截止频率比较相近,大约为24GHz;而最高振荡频率随栅宽增加而降低,分别为56, 46和40GHz. 测试了8GHz频率时,不同工作条件下1000μm栅宽器件的连续波微波功率特性:Vds=17V, Id=310mA, Pin=25.19dBm时,Po=30dBm (1W) ,Ga=4.81dB; Vds=18V, Id=290mA, Pin=27dBm时,Po=31.35dBm (1.37W) ,Ga=4.35dB.  相似文献   

6.
介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果.制作了几种0.6μm栅长、100~1000μm不同栅宽的器件,对于栅宽分别为100,300和500μm的器件,典型最大跨导为190~170mS/mm;截止频率比较相近,大约为24GHz;而最高振荡频率随栅宽增加而降低,分别为56,46和40GHz.测试了8GHz频率时,不同工作条件下1000μm栅宽器件的连续波微波功率特性:Vds=17V,Id=310mA,Pin=25.19dBm时,Po=30dBm(1W),Ga=4.81dB;Vds=18V,Id=290mA,Pin=27dBm时,Po=31.35dBm(1.37W),Ga=4.35dB.  相似文献   

7.
介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果.制作了几种0.6μm栅长、100~1000μm不同栅宽的器件,对于栅宽分别为100,300和500μm的器件,典型最大跨导为190~170mS/mm;截止频率比较相近,大约为24GHz;而最高振荡频率随栅宽增加而降低,分别为56,46和40GHz.测试了8GHz频率时,不同工作条件下1000μm栅宽器件的连续波微波功率特性:Vds=17V,Id=310mA,Pin=25.19dBm时,Po=30dBm(1W),Ga=4.81dB;Vds=18V,Id=290mA,Pin=27dBm时,Po=31.35dBm(1.37W),Ga=4.35dB.  相似文献   

8.
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。  相似文献   

9.
研制成 Ga As/ In Ga As异质结功率 FET(HFET) ,该器件是在常规的高 -低 -高分布 Ga As MESFET的基础上 ,在有源层的尾部引入 i-In Ga As层。采用 HFET研制的两级 C波功率放大器 ,在 5 .0~ 5 .5 GHz带内 ,当Vds=5 .5 V时 ,输出功率大于 3 2 .3 1 d Bm(0 .1 77W/ mm ) ,功率增益大于 1 9.3 d B,功率附加效率 (PAE)大于3 8.7% ,PAE最大达到 49.4% ,该放大器在 Vds=9.0 V时 ,输出功率大于 3 6.65 d Bm(0 .48W/ mm) ,功率增益大于 2 1 .6d B,PAE典型值 3 5 %  相似文献   

10.
设计并制作了双异质结双平面掺杂的Al0 .2 4 Ga0 .76 As/ In0 .2 2 Ga0 .78As/ Al0 .2 4 Ga0 .76 As功率PHEMT器件,采用双选择腐蚀栅槽结构,有效提高了PHEMT器件的输出电流和击穿电压.对于1μm栅长的器件,最大输出电流为5 0 0 m A/ mm ,跨导为2 75 m S/ m m,阈值电压为- 1 .4 V,最大栅漏反向击穿电压达到了33V .研究结果表明,在栅源间距一定时,栅漏间距对于器件的输出电流、跨导和击穿电压有很大关系,是设计功率PHEMT的关键之一.  相似文献   

11.
高性能1mm AlGaN/GaN功率HEMTs研制   总被引:7,自引:4,他引:3  
报道了基于蓝宝石衬底的高性能1mm AlGaN/GaN HEMTs功率器件.为了提高微波功率器件性能,采用新的欧姆接触和新型空气桥方案.测试表明,器件电流密度为0.784A/mm,跨导197mS/mm,击穿电压大于40V,截止态漏电较小,1mm栅宽器件的单位截止频率达到20GHz,最大振荡频率为28GHz,功率增益为11dB,功率密度为1.2W/mm,PAE为32%,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   

12.
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   

13.
报道了利用南京电子器件研究所生长的蓝宝石衬底AlGaN/GaN异质结材料制作的HEMT,器件功率输出密度达4W/mm。通过材料结构及生长条件的优化,利用MOCVD技术获得了二维电子气(2DEG)面密度为0.97×1013cm-2、迁移率为1000cm2/Vs的AlGaN/GaN异质结构材料,用此材料完成了栅长1μm、栅宽200μm AlGaN/GaN HEMT器件的研制。小信号测试表明器件的fT为17GHz、最高振荡频率fmax为40GHz;负载牵引测试得到2GHz下器件的饱和输出功率密度为4.04W/mm。  相似文献   

14.
The DC and RF characteristics of Ga/sub 0.49/In/sub 0.51/P-In/sub 0.15/Ga/sub 0.85/As enhancement- mode pseudomorphic HEMTs (pHEMTs) are reported for the first time. The transistor has a gate length of 0.8 /spl mu/m and a gate width of 200 /spl mu/m. It is found that the device can be operated with gate voltage up to 1.6 V, which corresponds to a high drain-source current (I/sub DS/) of 340 mA/mm when the drain-source voltage (V/sub DS/) is 4.0 V. The measured maximum transconductance, current gain cut-off frequency, and maximum oscillation frequency are 255.2 mS/mm, 20.6 GHz, and 40 GHz, respectively. When this device is operated at 1.9 GHz under class-AB bias condition, a 14.7-dBm (148.6 mW/mm) saturated power with a power-added efficiency of 50% is achieved when the drain voltage is 3.5 V. The measured F/sub min/ is 0.74 dB under I/sub DS/=15 mA and V/sub DS/=2 V.  相似文献   

15.
An experimental study in which the quantum well width (W) is varied from 45 to 200 Å is discussed. Optimum device performance was observed at a well width of 120 Å. The 0.2-μm×130-μm devices with 120-Å quantum-well width typically exhibit a maximum channel current density of 550 mA/mm, peak transconductance of 550 mS/mm, and peak current gain cutoff frequency ( fT) of 122 GHz. These results have been further improved in subsequent fabrications employing a trilevel-resist mushroom-gate process. The 0.2-μm×50-μm devices with mushroom gate exhibit a peak transconductance of 640 mS/mm, peak f T of 100 GHz, and best power gains cutoff frequency in excess of 200 GHz. These results are among the best ever reported for GaAs-based FETs and are attributed to the high two-dimensional electron gas (2DEG) sheet density, good low-field mobility, low ohmic contact, and the optimized mushroom gate process  相似文献   

16.
A low-voltage single power supply enhancement-mode InGaP-AlGaAs-InGaAs pseudomorphic high-electron mobility transistor (PHEMT) is reported for the first time. The fabricated 0.5/spl times/160 /spl mu/m/sup 2/ device shows low knee voltage of 0.3 V, drain-source current (I/sub DS/) of 375 mA/mm and maximum transconductance of 550 mS/mm when drain-source voltage (V/sub DS/) was 2.5 V. High-frequency performance was also achieved; the cut-off frequency(F/sub t/) is 60 GHz and maximum oscillation frequency(F/sub max/) is 128 GHz. The noise figure of the 160-/spl mu/m gate width device at 17 GHz was measured to be 1.02 dB with 10.12 dB associated gain. The E-mode InGaP-AlGaAs-InGaAs PHEMT exhibits a high output power density of 453 mW/mm with a high linear gain of 30.5 dB at 2.4 GHz. The E-mode PHEMT can also achieve a high maximum power added efficiency (PAE) of 70%, when tuned for maximum PAE.  相似文献   

17.
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   

18.
High-performance E-mode AlGaN/GaN HEMTs   总被引:1,自引:0,他引:1  
Enhancement-mode AlGaN/GaN high electron-mobility transistors have been fabricated with a gate length of 160 nm. The use of gate recess combined with a fluorine-based surface treatment under the gate produced devices with a threshold voltage of +0.1 V. The combination of very high transconductance (> 400 mS/mm) and low gate leakage allows unprecedented output current levels in excess of 1.2 A/mm. The small signal performance of these enhancement-mode devices shows a record current cutoff frequency (f/sub T/) of 85 GHz and a power gain cutoff frequency (f/sub max/) of 150 GHz.  相似文献   

19.
We report on AlGaN/GaN metal oxide semiconductor heterostructure field effect transistor (HFET) over SiC substrates with peripheries from 0.15 to 6 mm. These multigate devices with source interconnections were fabricated using a novel oxide-bridging approach. The saturation current was as high as 5.1 A for a 6 mm wide device with a gate leakage of 1 μA/cm2 for 1.5 μm gate length in a 5 μm source-drain opening. The cutoff frequency of around 8 GHz was practically independent of the device periphery. Large-signal output rf-power as high as 2.88 W/mm was measured at 2 GHz. Both the saturation current and the rf-power scaled nearly linearly with the gate width  相似文献   

20.
DC and RF characteristics of 0.15 °m GaAs power metamorphic high electron mobility transistors (MHEMT) have been investigated. The 0.15 °m ° 100 °m MHEMT device shows a drain saturation current of 480 mA/mm, an extrinsic transconductance of 830 mS/mm, and a threshold voltage of ‐0.65 V. Uniformities of the threshold voltage and the maximum extrinsic transconductance across a 4‐inch wafer were 8.3% and 5.1%, respectively. The obtained cut‐off frequency and maximum frequency of oscillation are 141 GHz and 243 GHz, respectively. The 8 ° 50 °m MHEMT device shows 33.2% power‐added efficiency, an 18.1 dB power gain, and a 28.2 mW output power. A very low minimum noise figure of 0.79 dB and an associated gain of 10.56 dB at 26 GHz are obtained for the power MHEMT with an indium content of 53% in the InGaAs channel. This excellent noise characteristic is attributed to the drastic reduction of gate resistance by the T‐shaped gate with a wide head and improved device performance. This power MHEMT technology can be used toward 77 GHz band applications.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号