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1.
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   

2.
使用自主研制的SiC衬底GaNHEMT外延材料,研制出高输出功率A1GaN/GaNHEMT,优化了器件研制工艺,比接触电阻率小于1.0×10^-6Ω·cm^2,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   

3.
自主研制的GaN HEMT,栅源泄漏电流从10-4 A量级减小到了10 -6 A量级,有效提高了栅漏击穿电压,改善了器件工作特性.采用MIS结构制作了2.5mm栅宽GaN HEMT,测试频率为8GHz,漏源电压为33V时,器件连续波输出功率为18.2W,功率增益为7.6dB,峰值功率附加效率为43.0%.2.5mm×4 GaN HEMT内配配器件,测试频率8GHz,连续波输出功率64.5W,功率增益7.2dB,功率附加效率39%.  相似文献   

4.
X波段GaN HEMT内匹配器件   总被引:1,自引:1,他引:0  
自主研制的GaN HEMT,栅源泄漏电流从1E-4A量级减小到了1E-6A量级,有效提高了栅漏击穿电压,改善了器件工作特性. 采用MIS结构制作了2.5mm栅宽GaN HEMT,测试频率为8GHz,漏源电压为33V时,器件连续波输出功率为18.2W,功率增益为7.6dB,峰值功率附加效率为43.0%. 2.5mm×4 GaN HEMT内匹配器件,测试频率8GHz,连续波输出功率64.5W,功率增益7.2dB,功率附加效率39%.  相似文献   

5.
基于GaN微波功率器件工艺制作了大栅宽GaN高电子迁移率晶体管(HEMT)管芯,通过负载牵引及建模技术提取了管芯的输入阻抗、输出阻抗.采用二项式多节阻抗匹配变换器实现了宽带功率分配器及合成器电路的制作,通过采用LC网络提升了管芯输入阻抗、输出阻抗,加入了稳定网络,实现了50 Ω阻抗匹配.采用高热导率金属陶瓷外壳,提高了器件散热能力.最终研制成功大功率GaN HEMT内匹配器件,器件采用四胞管芯功率合成技术,总栅宽为40 mm.测试结果表明,频率为4.5~4.8 GHz,脉宽300μs,占空比10%,工作电压VDSs为28 V,器件的输出功率大于120 W,功率附加效率大于50%,功率增益大于11 dB.  相似文献   

6.
利用MOCVD技术研制了国产SiC衬底的GaN HEMT外延材料,方块电阻小于260 Ω/□,迁移率最大值达到2 130 cm2V-1s-1,方块电阻和迁移率不均匀性小于3%,采用新的器件栅结构和高应力SiN钝化技术,降低了大栅宽器件栅泄漏电流,提高了工作电压.研制的总栅宽为25.3 mm的四胞内匹配器件X波段输出功率达到141.25 W,线性增益大于12 dB,PAE达到41.4%.  相似文献   

7.
报道了研制的SiC衬底AIGaN/GaN HEMT微带结构微波功率MMIC,芯片工艺采用凹槽栅场板结构提高AlGaN/GaNHEMTs的微波功率特性.S参数测试结果表明AlGaN/GaN HEMTs的频率特性随器件的工作电压变化显著.研制的该2级功率MMIC在9~11GHz带内30V工作,输出功率大于10W,功率增益大于12dB,带内峰值输出功率达到14.7W,功率增益为13.7dB,功率附加效率为23%,该芯片尺寸仅为2.0mm×1.1mm.与已发表的X波段AlGaN/GaN HEMT功率MMIC研制结果相比,本项工作在单位毫米栅宽输出功率和芯片单位面积输出功率方面具有优势.  相似文献   

8.
研究了AlGaN/GaN HEMT器件Ti/Al/Ti/Au四层金属结构欧姆接触的形成过程.通过系统研究退火条件获得了较低的欧姆接触电阻,实现了10-7Ω·cm2的欧姆接触率,并在此基础上对AlGaN/GaN HEMT欧姆接触形成机理进行了深入讨论.通过器件工艺的优化,研制了高性能的AlGaN/GaN HEMT器件.栅宽40μm的器件跨导达到250mS/mm,fT达到70GHz;栅宽0.8mm的功率器件电流密度达到1.07A/mm(Vg=0.5V),Vds=30V时,8GHz工作频率下(在片测试)器件的输出功率为32.5dBm(1.6W),输出功率密度达到2.14W/mm,功率增益为12.7dB.  相似文献   

9.
基于蓝宝石衬底的Ku波段3.4W/mm功率AlGaN/GaN HEMT   总被引:2,自引:1,他引:1  
本文报道了国内第一个基于蓝宝石衬底的ku波段AlGaN/GaN HEMT。器件总栅宽0.5mm,栅长0.35um。漏压30V下器件的ft为20GHz,fmax为75GHz。在漏压30V、连续波测试条件下,器件在14GHz的线性增益为10.4dB,3dB增益压缩的输出功率为1.4W,附加效率41%。在脉冲测试条件下,线性增益12.8dB,3dB增益压缩的输出功率为1.7W,功率密度达到3.4W/mm。  相似文献   

10.
默江辉  蔡树军  冯震  王勇  张志国 《半导体技术》2007,32(6):478-480,489
制作了带有栅终端场板结构的GaN基HEMT,研究了击穿电压与场板长度的关系,提取了最佳场板长度为0.4,0.5,0.6μm时所对应的栅漏击穿电压最大,为120 V.研究了栅终端场板对器件小信号特性和大信号的影响,栅终端场板长度0.4μm时,器件特征频率及最大振荡频率减小量最小.在栅宽1 mm、频率8 GHz、无场板器件最大工作电压28 V时,连续波输出功率3.2 W,功率增益4.0 dB,功率附加效率17.0%;栅终端场板器件最大工作电压38 V时,连续波输出功率5.1 W,功率增益4.1 dB,功率附加效率21.0%.  相似文献   

11.
High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET > PDMAT > TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.  相似文献   

12.
In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal (200) (2d = 0.4027 nm) is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line(w), the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line(x), the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines(y), the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line(z) in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line(q) in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution(λ/△ 2) is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.  相似文献   

13.
This paper reviews our recent development of the use of the large-scale pseudopotential method to calculate the electronic structure of semiconductor nanocrystals, such as quantum dots and wires, which often contain tens of thousands of atoms. The calculated size-dependent exciton energies and absorption spectra of quantum dots and wires are in good agreement with experiments. We show that the electronic structure of a nanocrystal can be tuned not only by its size,but also by its shape. Finally,we show that defect properties in quantum dots can be significantly different from those in bulk semiconductors.  相似文献   

14.
An improving utilization and efficiency of critical equipments in semiconductor wafer fabrication facilities are concerned. Semiconductor manufacturing FAB is one of the most complicated and cost sensitive environments. A good dispatching tool will make big difference in equipment utilization and FAB output as a whole. The equipment in this paper is In-Line DUV Scanner. There are many factors impacting utilization and output on this equipment group. In HMP environment one of the issues is changing of reticule in this area and idle counts due to load unbalance between equipments. Here we'll introduce a rule-based RTD system which aiming at decreasing the number of recipe change and idle counts among a group of scanner equipment in a high-mixed-products FAB.  相似文献   

15.
This paper presents a brief overview of the Applied Centura(R)DPS(R)system,configured with silicon etch DPS Ⅱ chamber, with emphasis on discussing tuning capability for CD uniformity control. It also presents the studies of etch process chemistry and film integration impact for an overall successful gate patterning development. Discussions will focus on resolutions to key issues, such as CD uniformity, line-edge roughness, and multilayer film etching integration.  相似文献   

16.
We have fabricated the white organic light-emitting devices (WOLEDs) based on 4,4' -bis(2,2 -diphenyl vinyl)-1,1' - biphenyl (DPVBi) and phosphorescence sensitized 5,6,11,12,-tetraphenylnaphthacene (rubrene). The device structure is ITO/2T-NATA (20 nm)/NPBX (20 nm)/CBP: x%Ir(ppy)3:0.5% rubrene (8 nm)/NPBX (5 nm)/DPVBi (30 nm)/Alq(30 nm)/LiF(0.5 nm)/A1. In the devices, DPVBi acts as a blue light-emitting layer, the rubrene is sensitized by a phosphorescent material, fac tris (2-phenylpyridine) iridium [Ir(ppy)3], acts as a yellow light-emitting layer, and N,N' -bis- (1-naphthyl)- N,N' -diphenyl -1, 1' -biphenyl-4,4' -diamine (NPBX) acts as a hole transporting and exciton blocker layer, respectively. When the concentration of Ir (PPY)3 is 6wt%, the maximum luminance is 24960 cd/m^2 at an applied voltage of 15 V, and the maximum luminous efficiency is 5.17 cd/A at an applied voltage of 8 V.  相似文献   

17.
To meet the need of automatic image features extraction with high precision in visual inspection, a complete approach to automatic identification and sub-pixel center location for similar-ellipse feature is proposed. In the method, the feature area is identified automatically based on the edge attribute, and the sub-pixel center location is accomplished with the leastsquare algorithm. It shows that the method is valid, practical, and has high precision by experiment. Meanwhile this method can meet the need of instrumentation of visual inspection because of easy realization and without man-machine interaction.  相似文献   

18.
The epi material growth of GaAsSb based DHBTs with InAlAs emitters are investigated using a 4 × 100mm multi-wafer production Riber 49 MBE reactor fully equipped with real-time in-situ sensors including an absorption band edge spectroscope and an optical-based flux monitor. The state-of-the-art hole mobilities are obtained from 100nm thick carbon-doped GaAsSb. A Sb composition variation of less than ± 0.1 atomic percent across a 4 × 100mm platen configuration has been achieved. The large area InAlAs/GaAsSb/InP DHBT device demonstrates excellent DC characteristics,such as BVCEO>6V and a DC current gain of 45 at 1kA/cm2 for an emitter size of 50μm × 50μm. The devices have a 40nm thick GaAsSb base with p-doping of 4. 5 × 1019cm-3 . Devices with an emitter size of 4μm × 30μm have a current gain variation less than 2% across the fully processed 100mm wafer. ft and fmax are over 50GHz,with a power efficiency of 50% ,which are comparable to standard power GaAs HBT results. These results demonstrate the potential application of GaAsSb/InP DHBT for power amplifiers and the feasibility of multi-wafer MBE for mass production of GaAsSb-based HBTs.  相似文献   

19.
本论文提出一种在多天线MIMO信道相关性建模中小角度扩展近似理论算法,并应用于分析MIMO系统性能。分析中分别对三种不同角能量分布情况下的空间相关性研发快速近似计算法,并同时提出双模(Bi-Modal)角能量分布情况下的近似运算。通过分析这些新方法的近似效率,可以得到计算简单、复杂度低、而且符合实际的MIMO相关信道矩阵,对系统级的快速高效计算法的研究和系统级的评估以及误差分析具有重要的意义。  相似文献   

20.
By using the expansion of the aperture function into a finte sum of complex Gaussian functions, the corresponding analytical expressions of Hermite-cosh-Gaussian beams passing through annular apertured paraxially and symmetrically optical systems written in terms of ABCD matrix were derived, and they could reduce to the cases with squared aperture. In a similar way, the corresponding analytical expressions of cosh-Gaussian beams through annular apertured ABCD matrix were also given. The method could save more calculation time than that by using the diffraction integral formula directly.  相似文献   

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