用反向调制照明法分析光栅成像效应

提出了用反向调制照法明分析光栅成像效应的观点，研究了光栅系统的反向衍射干涉效应，成功地揭示了泰伯效应与劳效应的内在联系，并在白光双光栅衍射干涉的“消色效应”的基础上获得了白光扩展光源照明下白光光栅成像效应和具有实用意义的四光栅干涉系统。     

两层阵列二的补码复数并行算法及其光学实现

提出了直接的二的补码阵列算法，基于混合二的补码表达方式，加法，减法和阵列乘法都能全并行地实现。直接算法克服了传统算法中存在的困难，即原理上对操作数的编码位数无限制，更有效地利用了空间带宽积，卷积后的序更直接加权求和即为两数的乘积，复数运算由包含四个区域的两层阵列完成，并进行了光学实验。     

激光相干阵列探测中的二元全息光栅

从外差阵列探测出发，围绕木振光束整形问题，就计算全息位相光栅在激光相干雷达系统中的应用进行了理论及实施方面的研究，得出较好的结果。     

针孔阵列扫描成像系统研究

采用多针孔线阵配 X光条纹相机 ,由多个针孔的一维条纹图像的数据 ,利用图像处理技术重建出二维图像。由此获得一项高时间分辨的二维空间成像技术 (MIXS) ,此技术利用现有的设备获得比 X光分幅相机高得多的时间分辨的二维图像。     

红外凝视传感器定量仿真及模型验证

针对新一代红外凝视成像传感器,依据红外辐射能量传递和转换的物理过程,完成了对传感器各组成单元的物理效应建模.不同于以往成像模型的定性仿真,该模型实现了对系统各模块成像特性的定量描述,综合考虑了传感器的信号传递特性、空间传递特性、空间采样特性和时空噪音特性,构建了较为完善的高仿真度红外成像仿真模型.为验证仿真模型的有效性,搭建了有效性实验验证平台,获取了真实热像仪的性能曲线和输出图像.通过计算和比较仿真模型和真实热像仪性能曲线和输出图像相似程度,定量化评价了模型的仿真度,验证了仿真模型的有效性.     

Sixteen-element Ge-on-SOI PIN photo-detector arrays for parallel optical interconnects

We describe the structure and testing of one-dimensional array parallel-optics photo-detectors with 16 photodiodes of which each diode operates up to 8 Gb/s. The single element is vertical and top illuminated 30μm-diameter silicon on insulator （Ge-on-SOI） PIN photodetector. High-quality Ge absorption layer is epitaxially grown on SO1 substrate by the ultra-high vacuum chemical vapor deposition （UHV-CVD）. The photodiode exhibits a good responsivity of 0.20 A/W at a wavelength of 1550 nm. The dark current is as low as 0.36/aA at a reverse bias of 1 V, and the corresponding current density is about 51 mA/cm2. The detector with a diameter of 30 t.trn is measured at an incident light of 1.55 μm and 0.5 mW, and the 3-dB bandwidth is 7.39 GHz without bias and 13.9 GHz at a reverse bias of 3 V. The 16 devices show a good consistency.     

Novel wavelength-accurate InP-based arrayed waveguide grating

A 13-channel, InP-based arrayed waveguide grating （AWG） is designed and fabricated in which the on-chip loss of the central channel is about -5 dB and the crosstalk is less than -23 dB in the center of the spectrum response. However, the central wavelength and channel spacing are deviated from the design values. To improve their accuracy, an optimized design is adopted to compensate the process error. As a result, the central wavelength 1549.9 nm and channel spacing 1.59 nm are obtained in the experiment, while their design values are 1549.32 nm and 1.6 nm, respectively. The route capability and thermo-optic characteristic of the AWG are also discussed in detail.