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1.
研究了Zn~+离子注入p-GaP半导体所引起的缺陷。在电流密度为0.03μA/cm~2下,将注入Zn~+离子剂量为1×101~(14)离子/厘米~2的GaP样品腐蚀出蚀坑后用SEM观察,结果表明,在离子注入区域有缺陷形成。 相似文献
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在扫描电镜和H-800透射电子显微镜上,研究了Ti3Al-Nb(Ti-24Al-14Nb-3V-0.5Mo)(at.%)合金不同组织状态下的室温拉伸变形机制。利用双倾技术和双束条件下g.b=0不可见判据,分析了合金中具有D019结构的α2相和bcc结构的B2相在拉伸变形后的位错类型和滑移系。结果表明,初生α2相体积分数高时,α2相内部出现致密且平行的滑移带,a型位错在基面{0001}上形成大量亚晶界和六角位错网络,使初生α2晶粒产生形变,并且协调了晶界的变形。另外,还有a型刃位错及少量c型位错在柱面{1010}上滑移,初生α2相体积分数低时,基体B2相上形成宽而长的滑移带,a/2〈111〉刃型位错在{110}面上滑移是B2相的主要变形模式。 相似文献
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工艺因素对Ba_(6-3x)(Sm_(1-y)Nd_y)_(8+2x)Ti_(18)O_(54)陶瓷微波特性的影响 总被引:7,自引:2,他引:7
探讨了研磨时间,黏合剂浓度、用量,压力,保压时间,预烧温度,烧结温度,烧结时间等工艺因素对Ba6-3x(Sm1-yNdy)8+2xTi18O54陶瓷(x=0.6,y=0.2,0.3)微波性能的影响,试验结果表明,在其他工艺因素控制得当时,预烧温度和烧结温度对微波性能的影响最大。在预烧温度1050℃,烧结温度1200℃下,其微波特性参数εr=76.19,Q·f=10.2THz,(f=4.5GHz)。本系统陶瓷的烧结温度比一般文献低100℃左右,性能仍不错。进一步研究可为制备低温烧结微波陶瓷提供可能。 相似文献
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阳极铝箔交流腐蚀发孔对比容的影响 总被引:2,自引:0,他引:2
采用50Hz交流电腐蚀发孔和进一步腐蚀阳极铝箔,在腐蚀箔表面形成透明钝化型腐蚀膜且蚀孔孔径较大。在交流电腐蚀过程中不产生发黑、掉粉和减薄现象。另外,该工艺对盐酸浓度和硫酸添加剂浓度的适应范围很宽。 相似文献
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《微纳电子技术》1995,(5)
用一种简练的异质结双极晶体管(HBT)模型来模拟SiC基双极晶体管的高频和大功率特性。研究了一种外壳温度在27℃(300K)到600℃(873K)下的6H-SiC/3C-SiCHBT。将其高频大功率特性与AlGaAs/GaAsHBT作了比较。不出所料,欧姆接触电阻限制了SiCHBT的高频性能。现在看来,在SiC上只能可靠地产生1×10 ̄(-4)Ω-cm ̄2的接触电阻。所以f_T和f_(max)的最高实际值仅分别为4.4GHz和3.2GHz。但假定发射极、基极和集电极的接触电阻低到1×10 ̄(-6)Ω时,则6H/3CSiCHBT的f_T和f_(max)分别可达到31.1GHz和12.76Hz。 相似文献
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低压铝箔交流腐蚀研究 总被引:4,自引:2,他引:2
在30Hz频率下,通过铝箔在HCl+H2SO4+HNO3+H3PO4体系中的交流腐蚀,研究腐蚀液组成中腐蚀主体及缓蚀剂对铝箔腐蚀的作用,探讨腐蚀过程中电源频率、腐蚀液温度、电流密度及腐蚀时间对铝箔腐蚀的影响。腐蚀液组成的配比恰当,有利于比容的提高。在特定的频率下采用合适的腐蚀液温度、适宜的电流密度和腐蚀时间可以提高铝箔的静电容量。 相似文献
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本文针对广义e-bent函数进行了讨论,证明了此类函数仅包括bent函数,常数函数和形如f(x1,x2,…,xn)=α0+(x1+α1)(x2+α2)…的函数,其中αi∈{0,1},i=0,1,…,n。 相似文献
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电容器铝箔交流腐蚀扩面机理研究 总被引:5,自引:0,他引:5
实现铝电解电容器小型化的关键是铝电极箔电解腐蚀扩面过程的人为设计。为实现这一目标,本文就目前尚不清楚的交流腐蚀扩面机制进行了系统分析研究。首先研究了高纯铝箔在水溶液中的热力学和在盐酸溶液中的动力学行为,接着详细地研究了铝在交流电的负半周所发生的变化,以及这些变化对交流正半周铝的点蚀的萌生和生长的影响,并从理论上推导出控制交流负半周腐蚀膜形成的数学关系式。在此基础上,提出了铝在交流负半周发生的四种变化,以及交流腐蚀扩面机理。根据这一机理,提出了铝箔的交流腐蚀工艺优化原则,并用实验对这一原则进行了初步验证。本论文的主要内容如下: 相似文献
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Faster image template matching in the sum of the absolute value ofdifferences measure 总被引:11,自引:0,他引:11
Given an mxm image I and a smaller nxn image P, the computation of an (m-n+1)x(m-n+1) matrix C where C(i, j) is of the form C(i,j)=Sigma(k=0)(n-1)Sigma(k'=0) (n-1)f(I(i+k,j+k'), P(k,k')), 0=/相似文献
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Shih-Chia Chang 《Journal of Electronic Materials》1984,13(6):955-967
The conventional method used for aluminum (Al) and aluminum alloy (Al + Si, Al + Si + Cu) delineation in integrated circuits
is mainly by wet chemical etching. Because of its isotropic characteristic, wet chemical etching becomes inadequate for patterning
Al metal lines with linewidths narrower than about 4 Μm. In this work, Al and Al alloys (Al + 2% Si; Al + 1% Si + 1% Cu) were
reactively etched in SiCl4 plasma using patterned photoresist as the etch-mask. Resist patterns were generated either by conventional processing methods
or by tri-level resist techniques which included hard-baking (200°C, ≤ 30 min), and two consecutive reactive ion etchings
in CF4 and 02 plasmas. Masking resists prepared by the tri-level resist technique retained their integrity during exposure to a SiCl4 plasma, and significantly improved resolution and fidelity of pattern transfer from resist to underlying Al or Al alloy film.
The substrate surface of the reactively etched Al + Si + Cu sample was considerably rougher than that of the Al or Al + Si
sample due to the high concentration of Cu accumulated at the metal/substrate region during RIE process. 相似文献
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《Microwave Theory and Techniques》1986,34(4):436-441
A novel analog frequency divider which can generate a 1/4 frequency component is proposed. The frequency divider consists of a dual-gate FET and a two-stage capacitor-resistor coupled amplifier. This circuit configuration also enables achieving a small-size GaAs MMIC analog frequency divider. In this analog frequency divider, the input signal f/sub 0/ is mixed with signal component f/sub 0//x caused by noise or transients in a feedback loop. Then, a (1 -- 1/x)f/sub 0/ IF component is induced and is again mixed with the input signal. This process delivers the f/sub 0//x component regeneratively. Resultant continuous signal components f/sub 0//x and (1-1/x)f/sub 0/ have a harmonic relation when the system reaches a steady state. The f/sub 0//x component can be mainly obtained at an output port of the frequency divider. The operation band was simulated using a SPICE II computer program. The designed bandwidth and conversion gain for the 1/4 frequency divider are 8.5-10.6 GHz and -3 dB, respectively. Based on the simulation, a GaAs monolithic analog 1/4 frequency divider was made and tested. The developed 1/4 frequency divider provides a 8.5-10.2-GHz operation bandwidth and --5+-1-dB conversion gain. The designed and experimental values are in good agreement. The frequency division band can be shifted to higher frequency (10.65-11.2 GHz) by adopting the external matching circuit at the GaAs chip output port. The proposed analog frequency divider circuit can be applied not only for 1/4 frequency division, but also for 1/n frequency division (interger n > 2). 相似文献
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《Microwave Theory and Techniques》1987,35(12):1156-1160
A precise design is presented for a bandpass filter constructed by placing TE/sub 01delta/ dielectric ring resonators coaxially in a TE/sub 01/ cutoff circular waveguide. On the basis of a rigorous analysis by the mode- matching technique, the interresonator coupling coefficients are determined accurately from the calculation of two resonant frequencies f/sub sh/ and f/sub op/ when the structurally symmetric plane is short- and open-circuited. For the TE/sub 01delta/ ring resonator,the resonant frequency f/sub 0/, the temperature coefficient tau/sub f/, the unloaded Q(Q/sub u/), and the other resonances are also calculated accurately in a similar way. From the calculations, the optimum dimensions are determined to obtain the maximum Q/sub u/, as F/sub r/ = f/sub r/ /f/sub 0/ is kept constant, where f/sub r/ is the next higher resonant frequency the ring resonator using low-loss ceramics (epsilon/sub r/ = 24.3, tan delta = 5 x 10/sup -5/) has Q/sub u/ = 16800 at 12 GHz and tau/sub f/ = 0.1+-0.5 ppm/° C, while the rod one has Q/sub u/ = 14700. A four-stage Chebyshev filter having ripple of 0.04 dB and equiripple bandwidth of 27.3 MHz at f/sub 0/ =11.958 GHz is fabricated using these resonator; the measured frequency responses agree well with theory. The insertion loss is 0.9 dB, which corresponds to Q/sub u/ = 9800. 相似文献
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Al/sub 0.4/Ga/sub 0.6/N/GaN heterostructure field-effect transistors (HFETs) with an AlGaN barrier thickness of 8 nm and a gate length (L/sub G/) of 0.06-0.2 /spl mu/m were fabricated on a sapphire substrate. We employed two novel techniques, which were thin, high-Al-composition AlGaN barrier layers and SiN gate-insulating, passivation layers formed by catalytic chemical vapor deposition, to enhance high-frequency device characteristics by suppressing the short channel effect. The HFETs with L/sub G/=0.06-0.2 /spl mu/m had a maximum drain current density of 1.17-1.24 A/mm at a gate bias of +1.0 V and a peak extrinsic transconductance of 305-417 mS/mm. The current-gain cutoff frequency (f/sub T/) was 163 GHz, which is the highest value to have been reported for GaN HFETs. The maximum oscillation frequency (f/sub max/) was also high, and its value derived from the maximum stable gain or unilateral gain was 192 or 163 GHz, respectively. 相似文献
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采用传统固相反应工艺,按质量分数合成BaO-Al2O3-SiO2-5%(xLi2O-yB2O3)(x=0. 2~0. 6,y=0. 8~0. 4)陶瓷。研究xL-yB烧结助剂对BAS系微波介质陶瓷的结构和介电性能的影响。通过Clausius-Mossotti公式计算讨论了BAS理论与实验介电常数的差异。研究结果表明:xL-yB烧结助剂中Li+进入钡长石Ba2+位,并产生了O2-空位,促进BAS六方相向单斜相转变。添加适当比例的xL-yB烧结助剂后,BAS陶瓷的烧结温度从1400℃降低到925℃,同时BAS陶瓷样品密度、品质因数(Q×f)值以及谐振频率温度系数(τf)得到改善。当烧结助剂为0. 5L-0. 5B,烧结温度为925℃时,可获得综合性能相对较好的BAS陶瓷,其介电性能:εr=6. 74,Q×f=26670 GHz,τf=-21. 09×10-6℃-1。 相似文献