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Uncooled InAsSb photoconductors were fabricated. The photoconductors were based on InAs0.05Sb0.95 and InAs0.09Sb0.91 thick epilayers grown on InAs substrates by melt epitaxy (ME). Ge immersion lenses were set on the photoconductors. The cutoff wavelength of InAs0.09Sb0.91 detectors is obviously extended to 11.5 mm, and that of InAs0.05Sb0.95 detectors is 8.3 mm. At room temperature, the peak detectivity of Dλp at wavelength of 6.8 mm and modulation frequency of 1 200 Hz is 1.08×109 cm.Hz1/2.W-1 for InAs0.09Sb0.91 photoconductors, the detectivity D at wavelength of 9 mm is 7.56×108 cm.Hz1/2.W-1, and that at 11 mm is 3.92×108 cm.Hz1/2.W-1. The detectivity of InAs0.09Sb0.91 detectors at the wavelengths longer than 9 mm is about one order of magnitude higher than that of InAs0.05Sb0.95 detectors, which rises from the increase of arsenic (As) composition in InAs0.09Sb0.91 materials. 相似文献
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本文对日立公司新一代彩色显像管用电子枪的结构及性能进行了剖析和系统讨论。其超大椭圆孔的主透镜使有效直径比上一代电子枪提高了25%,电子束形成区实现最优化设计,不同电流下聚焦的稳定性提高,同时进入主透镜的电子束发散角在水平和垂直方向不同,实现与主透镜的最佳配合,充分发挥了主透镜中共同透镜为椭圆孔透镜的特点。聚焦对比实验也显示出日立公司新一代电子枪聚焦的优异性能。 相似文献
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利用表面等离子激元的新颖特性,设计了二维间隙表面等离子波导.以这种结构为基础通过变形和组合形成90°直角弯曲波导、T型光功率分配器和光开光,采用时域有限差分法研究了它们的传输特性.结果表明:不同于介质光波导的弯曲损耗来自于辐射泄漏,90°直角弯曲间隙表面等离子波导的能量损耗主要来自于金属中的欧姆热损耗.在间隙达到40 ... 相似文献
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采用基于密度泛函理论框架下的第一性原理平面波超软赝势方法,在相同环境条件下建立了浓度不同的由Ga原子取代Zn原子的Zn1-xGaxO模型.对低温高掺杂Ga原子的Zn1-xGaxO半导体的能带结构、态密度和吸收光谱进行了计算.结果表明:Ga原子浓度越大,进入导带的相对电子数越多,但是电子迁移率反而减小.通过对掺杂和未掺杂ZnO的电导率以及最小间隙带宽度分别进行了比较
关键词:
ZnO高掺杂Ga
电导率
红移
第一性原理 相似文献
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采用时域有限差分法研究三平行光子晶体直波导的传输特性及模场分布,结合耦合模理论计算光子晶体波导的耦合系数.计算结果表明,在高频段(0.33~0.42)(ωa/27πc)的范围内两耦合波导与主波导表现出相互的能量交换,实现光耦合,耦合系数随入射波频率增加而减小;而在低频段(0.31~0.33)(ωa/2πc)的范围内,两耦合波导与主波导的传输谱图同步变化,耦合波导的传输光强均约为入射光强的四分之一.最后,提出一种采用固定波导耦合长度同时实现超微结构光均分器及1/4功分器的方案,当耦合长度取L_c=(2n+1)π/2 K时,两耦合波导可将高频段相应入射波实现均分,同时将低频段中的任意入射波实现1/4功分.Abstract: The propagating characteristics and mode profiles of three parallel photonic crystal waveguides are studied by using finite-difference time-domain method, and the coupling coefficient between the parallel photonic crystal waveguides is obtained with coupled-mode theory. Numerical results demonstrate that for a high frequency range of (0.33~0.42)(ωa/ 2πc), they exchange energy with each other and the optical coupling is realized, the coupling coefficient decreased with the increase of input frequency; while at a low frequency range of (0.31 ~0.33) (ωa/2πc), the mode profiles of the coupling waveguides and main waveguide are changed synchronously, and the coupling waveguides propagating intensity occupies a quarter of the incident intensity. Finally, a solution realizing the ultracompact optical power equalizer and 1/4 optical beam splitter is proposed using a certain coupling length, when the coupling length is L_c= (2n+1)π/2 K, the corresponding incident wave with high frequency can be equalized, meanwhile the wave power with arbitrary frequency at low frequency can be quartered within the two coupling waveguides. 相似文献
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为克服传统时域有限差分法(FDTD)不能计算色散材料的困难,给出了一种基于Drude模型的色散FDTD算法,并推导出具体的差分公式。将该方法用于模拟金属透镜的聚焦功能,结果与已有理论吻合。本文方法完全适用于分析电导率与频率有关的各种色散材料所构建的光波导。 相似文献