64×64全交叉互连函数的光学实现

光互连全交叉网络在巨型计算机和光子交换网络系统等领域具有十分重要的潜在应用。本文在自行设计研制成功棱镜光栅和６５×６５大列阵Ｄａｍｍａｎｎ光栅的基础上，运用自由空间光学互连技术实现了６４×６４全交叉网络的互连函数。采用互连矩阵对输出图样进行了计算，结果与实验吻合。     

全混洗交换Omega互连网络的光学实现

本文提出了一种由左、右全混洗和空间光开关列阵组成的等效Omega网络;成功地设计了一种实现全混洗互连的低损耗,等程的光学组合棱镜.由两块光学组合棱镜和空间光开关列阵组合成的光学系统实现了全混洗交换光学互连网络,该光学互连网络已在实验中得到了证实.     

未来计算系统中的光互连

论述了光互连网络对巨型计算机和智能计算机发展的重要作用，指出了光互连网络是解决目前电子计算机中通信“瓶颈”的关键，讨论了采用光互连的物理依据，强调了光互连网络的高效，快速和大容量特性。最后分析了我们正在研究的光学交叉开关互连网络的几个关键参数和初步实验结果。     

用多级衍射全息光栅实现2-D自由空间光学互连网络

用Mach-Zehnder干涉仪分两步记录制作了具有多级衍射的全息光栅.利用其多级衍射效应,实现了一点到多点的光学互连.再将两个1-D光栅正交密接实现2-D自由空间光学互连网络.结果表明该方法是可行的,且结构简单、操作容易.     

自由空间光学Comega多级互连网络特性研究

光学Ｃｏｍｅｇａ网络是一种新颖的易于光学实现的多级光互连网络。本文对该网络结构及特性进行了详细分析，和到了网络的互连函数，并给出了它与Ｓｔａｒａｎ，Ｃｒｏｓｓｏｖｅｒ，Ｏｍｅｇａ，Ｂａｎｙａｎ及基准等常见网络的拓扑等价证明。     

光互连Omega网络与全交叉网络拓扑等价的多样性

本文对互连网络拓朴等价的分析方法作了简单评述,并采用互连网络拓朴等价的图分析法分析了自由空间光学互连Omega网络与全交叉网络的拓朴等价及其多样性,拓展了Omega网络在通信交换、数字光计算以及并行多处理机系统的潜在应用。     

光学全息方法实现2＊2自由空间交叉光互连

采用光学全息的方法制备互连元件（布喇格衍射型体积相位光栅）。当光束垂直入射该光栅时,只有0级透射光和＋1级衍射光,可以较容易地得到直连、交叉光束,实现2＊2交叉互连。     

一种新型的光电混合多项式求值并行处理系统

本文提出了一种新型的并行求解多项式值的光电混合数字计算系统。系统中,我们采用了一种新的自由空间互连网络:逆全混洗互连,并用一特殊的组合棱镜和向列型液晶空间光调制器配合,在光学上实现了逆全混洗互连。     

实现交叉光互连的全息元件的研究

光学互连与电互连相比,具有并行处理、传输速度快、信息容量大、空间频带宽、串音小和能量损耗低等优点,因此在光计算和信息处理领域中成为越来越吸引人的课题[1~4].在光信息处理中,光互连在实行多种函数及变换过程中具有重要的地位[5].在数字光计算中,光互连可实行多种算法和构造,其中自由空间规则光互连如全混洗(perfect shuffle)光互连、交叉(crossover)光互连及蝶(butterfly)光互连已得到广泛研究和应用[6~8].     

高容量的单极二值互连神经网络联想存储模型

由于光学固有的数值精度低,难以表示负值等弱点,用光学方法实现神经网络时存在着许多困难。针对光学的弱点,本文提出并建立了具有单极二值互连的适应截值模型,这一模型避开了光学实现时难以表示负值和互连精度差等弱点,计算机模拟及光学实现结果表明,这种单极互连神经网络模型同其他的单极模型相比具有高的存储容量及较强的寻址能力。     

Closely packed micro optical fiber arrays in laser scanning system

Closely packed optical fiber arrays are used to increase the scanning speed in some laser scanning systems, but standard optical fibers are shown to be unsuitable for these systems. In this paper, a closely packing technique of micro optical fiber arrays is presented. The fabrication and properties of micro fibers, whose diameters range from several hundred nanometers to several microns, are introduced. These micro fibers are arranged side by side in V-shaped grooves, which are fabricated by photolithography and etching techniques on silicon substrate. Comparing to standard optical fiber arrays, such closely packed micro optical fiber arrays can eliminate the dark area among output light spots and can solve the problem of high accuracy demand of exposure location. This closely packing technique is also proved to be a feasible method in practical scanning systems.     

微透镜阵列线性光学扫描器

本文介绍了一种新型的线性扫描光学系统，它由一对处于望远型结构的微透镜阵列和一个普通的会聚透镜组成。微透镜阵列采用二元光学技术进行设计和制作。该装置具有扫描灵敏度高（～１０００）、扫描范围大（±１００ｍｍ）、结构紧凑、价格低廉等优点。     

Fiber waveguide arrays as model system for discrete optics

Optical waveguide arrays consisting of a two-dimensional arrangement of weakly coupled waveguides represent the basis of the new research field of discrete optics. For studying the nonlinear pulse dynamics, fiber waveguide arrays offer specific advantages such as a high optical damage threshold and an accessible range of anomalous dispersion. Coherent coupling of such waveguides for reasonable propagation lengths requires, however, a high structural quality of the waveguides and their superstructure, which is beyond conventional fiber technology. Design, fabrication and characterization of such a fiber waveguide array are described. The linear propagation properties in such a system are modeled and compared with experimental measurements. The high structural homogeneity and good optical quality of the arrays as well as the limits of the nearest-neighbor approximation are demonstrated.     

连续波DF激光器高腔压运转的数值研究

 对以C₂H₄作燃料、以He作稀释剂的燃烧驱动连续波DF化学激光器进行了模拟计算，着重研究了激光器在高腔压条件下的性能。通过比较两种具有不同喷管家结构的DF化学激光器的高腔压运转下的平均腔压、激射强度、输出耦合功率和化学效率，指出高腔压运转对喷管结构的要求。     

Supersonic CW HF chemical lasers with an extended active medium

Spatial-energy, spectral, and optical characteristics of kilowatt supersonic cw HF chemical lasers of self-contained type with three-jet nozzle arrays using nozzle-nozzle-injector and nozzle-nozzle-nozzle configurations were experimentally studied. It was shown that such nozzle arrays enable one to form an active medium as long as 12.5 cm with a high optical quality. In a laser with a wide-aperture stable cavity, a laser beam with a nearly square cross section 11 × 10 cm in size was formed.     

High-intensity near-field generation for silicon nanoparticle arrays with oblique irradiation for large-area high-throughput nanopatterning

We present near-field distributions around an isolated 800-nm silica or silicon nanoparticle, and nanoparticle arrays of 800-nm silica or silicon nanoparticles, on a silicon substrate by the finite-difference time-domain method when 800-nm light is irradiated obliquely to the substrate. Nanopatterning mediated with the nanoparticle system is promising for large-area, high-throughput patterning by using an enhanced localized near-field ablation by the nanoscattered light lens effect. The irradiation area cannot be extended for silica nanoparticles, because the optical field enhancement factor is low. Gold nanoparticles can generate highly enhanced near fields, although at present there are no useful ways to arrange the gold nanoparticles on the substrate at a high throughput. Silicon nanoparticles with high dielectric permittivity have optical characteristics of both silica and gold nanoparticles. The particle arrangement on the Si substrate is technically easy using a wet pulling process. From the calculation, high optical field intensity is acquired with oblique s-polarized irradiation to the substrate under silicon nanoparticle arrays, and the intensity is almost the same as that under gold nanoparticle arrays under the same condition. With this method, high-throughput nanopatterning for a large area would be achievable.     

稀疏光学相控阵设计方法研究

为克服光学相控阵单元间隔必须小于工作波长二分之一的限制,构建了一种稀疏光学相控阵模型。分析了一维稀疏光学相控阵在近场和远场条件下的扫描原理,并提出了一种设计方法。对其相关参数进行仿真的结果表明：稀疏光学相控阵所用的单元数目较少,单元间隔远大于工作波长,扫描范围较大,波束宽度较窄,且在整个扫描空间内没有栅瓣。因此,稀疏光学相控阵单元间隔不受工作波长的限制,同时具有较好的扫描性能。     

Ordered tellurium nanowire arrays and their optical properties

High-density tellurium (Te) nanowire arrays were prepared in the nanochannels of an anodic aluminum membrane (AAM) template using the electrochemical deposition method. The as-synthesized Te nanowires, typically 60 nm in diameter and up to 40 μm in length, possess a hexagonal single crystalline structure following [001] growth direction. The optical polarization properties of Te nanowire arrays embedded in AAM were investigated using an optic parameter oscillator in the wavelength range from 0.7 to 1 μm. The high optical polarization of the Te nanowire arrays embedded in the AAM assembly system was observed. PACS 81.05.Cy; 78.67.-n; 82.80.Fk.     

3D nanoimprinted Fabry–Pérot filter arrays and methodologies for optical characterization

Fabry–Pérot (FP) filter arrays fabricated by high-resolution three dimensional (3D) NanoImprint technology are presented. A fabrication process to implement 3D templates with very high vertical resolution is developed. Filter arrays with 64 different cavity heights have been fabricated requiring only one single imprint step. Different optical methods are involved in this paper to characterize geometric and spectral properties. In order to investigate the transfer accuracy of the surface quality from the NanoImprint template to the filter, we use white light interferometry (WLI) measurements. Surface roughness and structure height accuracy of <1 nm for both values demonstrate the conservation of these critical parameters during the 3D NanoImprint process. Additionally, an optical characterization methodology for spectral transmission and reflection measurements of the filter arrays is introduced and applied. A compact microscope spectrometer setup which allows efficient handling, high resolution and short inspection time is verified by comparing measurement results to that of an optical bench setup used as a reference. First, this paper focuses on the foundation of the FP filter arrays, second on the technological fabrication, third on validation calibration of the setup and forth on the characterization of the filter arrays. The measurements envisage the spectral position of filter transmission lines, the full width at half maximum (FWHM) and the total spectral bandwidth of the array, i.e. the stopbands of the included Distributed Bragg Reflectors (DBRs).