基于混合优化算法的关节臂式测量机参数标定

为进一步提高关节臂式坐标测量机等高机动性精密测量设备的测量精度,使用D-H矩阵法建立其关节坐标转换数学模型并据此推导出参数误差模型.针对非线性多参数标定问题,通过变换分析消除了最小二乘法求解时矩阵中的冗余参数,降低了计算的复杂性.设定判定准则并实现最小二乘法和模拟退火算法的混合,提出了一种基于混合优化算法的参数标定方法,解决了LM算法的初值设定和SA算法的搜索效率逐步降低的问题.实验结果表明:关节臂式测量机参数经混合优化算法标定后,参数的误差范围有了显著的缩小,单点重复性误差的平均值减小了1.746 mm,长度误差的平均值减小了0.941 mm,测量误差得到了进一步的抑制.     

超高功率超短脉冲发展的现状及相关科学问题

超高功率超短脉冲激光系统在其聚焦焦点附近可以实现高达1022-24 W/cm2的峰值功率输出,为强场物理实验研究,以及实验室内模拟极端环境下的天体物理条件提供了直接的实现方案.自从国际上首次提出了建造EW激光的概念,即输出总功率达到1018 W的大型激光系统后,国际上很多国家都在设计和建造大规模的超高功率超短脉冲激光系统.本文简要介绍了国际上这种规模激光系统的发展状况,并结合国内超高功率高能超短脉冲激光的发展,对超高功率超短脉冲激光系统发展中相关技术问题进行阐述.     

激光快速成型TC4合金显微组织及力学性能

采用金相显微镜、扫描电镜、电子拉伸机等，研究了激光快速成型TC4合金沉积态在平行沉积方向和垂直沉积方向的组织和力学性能.结果表明:激光快速成型TC4合金沉积态宏观组织沿沉积方向生长的粗大β柱状晶呈明暗相间的条带状结构，具备典型的魏氏组织特征;垂直沉积方向的强度比平行沉积方向的强度高，但塑性低;合金断口为韧窝状断口，垂直沉积方向的断口韧窝尺寸比平行沉积方向的小.     

扫描探针检测交变力场

设计了一个可检测交变力场的扫描探针系统，针尖受到与样品间的交变电场力或磁场力的作用而振动，针尖振动由一超外差激光干涉仪检测。从而确定作用力的大小，该文分析了系统的灵敏度，测量了针尖与样品间的交变电场力随两者间距的变化曲线，对周期性分布的电场进行了一维扫描检测，并进行了金属薄膜厚度的测量。该文还利用磁性探针进行了交变磁场力的检测，系统的电磁力检测灵敏度为１０＾－１１Ｎ。     

检测陀螺仪转子安装精度的一种新方法

陀螺仪转子的安装精度对其运行的稳定性和精确性有很大的影响。由于要求的安装误差很好，因此，对其误差的测量要求准则。其测量误差应经安装误差小1／10以及上，一般的检测方法很难达到要求，为此介绍了一种新型的光电检测方法，该方法利用狭缝的光学傅立叶变换提取陀螺仪转子的误差信息，采用计算机进行信息处理，从而完成陀螺仪转子的自动检测和分类，该方法也可用于其他一些精密年的自动检测处理。     

光电转换体系太阳能聚集器

In standard P-V systems, the high cost and low quantum efficiency of silicon cells has held back widespread adoption of this technology for decades. To generate electrical power from solar energy in a cost effective way, most methods require the concentration of the sunlight in order to increase the efficiency of energy conversion. Most systems use parabolic mirrors to focus sunlight to either a line （trough systems） or a small volume （dishes）. One of the reasons solar power still remains little utilised, is the high cost of the collection systems. Light focussing devices using reflection usually take the form of a curved rein＇or. In contrast, this paper describes the new design of a device consisting of an array of small angled reflecting m/trot facets located in a planar form. The three dimensional angle of each facet in the array is a function of its position in the array, and is calculated to be such that for a parallel beam striking the array, each facet will reflect the light in such a way as to form a focal point region.     

自平衡式单臂双用扭矩定标器

本文指出了当前在科研和生产中采用的一般机械式扭矩加载器的某些缺点和错 误；提出一种自平衡式单臂双用纯扭矩加载装置，可以消除定标过程的附加干扰，保 证检测精度。该装置简单，合理、适用。     

双脉冲TEA CO_2激光器电路参数的选择

分析了电路参数及电路结构对双脉冲TEA CO_2激光器输出稳定性的影响,并提出合理选择电路参数与结构的原则。实验结果,证实了分析的正确性。     

双模三次激光模型的微扰解法及统计特性

采用微扰方法,得到了双模三次激光模型在不满足势条件下的相关结果.并对该模型的等时自相关和互相关系数进行了计算和讨论.     

Orthogonally linear polarized lasers(Ⅰ)--principle and devices

Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect,stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c/4L instead of c/2L.