Contact mechanics modeling of piezo-actuated stick-slip microdrives

This paper draws a line from early attempts of modeling stick-slip microdrives to open questions from today’s research. As a basis, it contains a collection of substantial investigations on piezo-actuated stick-slip microdrives for nanomanipulation purposes. Friction models showing special characteristics and their mathematical representations are reviewed. It is found that the working properties of stick-slip drives strongly depend on friction characteristics of the contact points between the guiding elements, which is known for years. However, numerous publications in the field of friction and remaining problems — which cannot be explained by known friction models — indicate that there is a demand for even more friction-related research.Former attempts to model stick-slip drives are based on the so-called LuGre friction model, which is shortly presented. An empirical model called CEIM is also analyzed. It is an adaption of the elastoplastic model. The latter can cover not only the phenomenon “0-amplitude’ (described by the authors in recent publications), but also stick-slip based force generation scenarios. Nevertheless, interesting friction characteristics such as the generation of μN forces with stick-slip drives, which are already proven, cannot be covered by known friction models. It is pointed out which characteristics have to be considered.     

强激光加载下金属材料微喷回收诊断

金属材料在冲击载荷下的动态响应在许多民用工程、航空航天等领域都有重要的应用背景.而金属材料在冲击载荷下的微喷形成过程,包括微射流、碎裂以及微层裂的物理过程的研究中尚存在许多空白.介绍了国内首次在神光Ⅲ原型激光装置上开展的金属材料微喷回收实验,实现了激光加载下低密度泡沫材料对微喷颗粒的回收,对回收样品进行了X光CT分析,通过图像重建,获得了回收微喷颗粒的三维图像,以及颗粒不同形态分布、颗粒尺寸、颗粒质量等定量结果.     

微流控制备单分散微米级SiO2微球

采用软模板法制备出了聚二甲基硅氧烷微流控装置。利用该装置讨论了正硅酸乙酯和氨水的用量分别对反应体系凝胶化时间的影响,确定了制备SiO2微球的优化反应体系,即二甲基乙酰胺、正硅酸乙酯和氨水的体积比为8∶4∶1,实验所需的反应温度为60 ℃。实验发现:在微流体通道中,分散相的流速越大,粒径越大;连续相流速越大,粒径越小。因此,通过控制微流控装置中分散相和连续相的流速制备了粒径40~220 m的单分散SiO2微球,并对其形貌进行表征。光学显微镜和粒径分析均表明所制备的SiO2微球球形度高,单分散性好。     

MnxSny(x=2,3,4; y=18,24,30)团簇几何结构的密度泛函研究

采用密度泛函方法,研究了Mn_xSn_y(x=2,3,4; y=18,24,30)团簇的几何结构. 发现Mn_xSn_6x+6(x=2,3,4)倾向于形成 Mn 原子内掺入D_3d Sn团簇单笼结构,即Mn₂Sn₁₈, Mn₃Sn₂₄ 和Mn₄Sn₃₀.而Mn_xSn_6x+12(x=2,3)则倾向于形成由两个小笼连接 而成的双笼结构,即MnSn₁₂-MnSn₁₂ 和MnSn₁₂-Mn₂Sn₁₈.因此,可望通过控制掺杂Mn 原子的数量来组装成不同结构的Mn_xSn_y一维纳米线.     

非均匀加宽单模激光器的最佳透射率

给出四能级系统非均匀加宽单模激光器最佳透射率的表达式和分布曲线,并与均匀加宽单模激光器最佳透射率进行了比较.叙述了非均匀加宽单模激光器的特点.     

铁掺杂PMP泡沫制备工艺研究

 以聚-4-甲基-1-戊烯为泡沫骨架，二茂铁为掺杂材料，通过热诱导倒相技术制备出铁掺杂聚合物泡沫。掺杂泡沫的实际密度均高于理论密度，且沿轴向从上至下逐渐增大。在理论密度不变的情况下，掺杂泡沫实际密度随掺杂元素原子百分含量的升高而呈降低趋势。与PMP泡沫相比，掺杂泡沫的孔洞直径分布变宽且网络骨架尺寸有变大的趋势。     

A FURTHER STUDY OF QUASI RESONATING GROUP METHOD—— ANALYSIS OF p+6Li ELASTIC SCATTERING

In this paper,the elastic scattering of p+⁶Li is studied by 3QRGM,a three-cluster RGM omitting the antisymmetrization with the nucleon in the double magic cluster.The main conclusion from studying the systems of p+⁶Li and n+⁶Li is the following:The clustering and exchange effects lower the phase shifts conspicuously.hence they are very important in the lower energy region.     

基片光学特性对薄膜光强透过谱的影响

在考虑基片与空气界面反射率以及基片吸收不能忽略的情况下，对常见的基片上薄膜的光强透过率公式进行了修正，导出了该情况下的透过率公式．以非晶硅薄膜为研究对象，采用模拟计算说明基片光学特性对薄膜光强透过谱的影响．     

Three‐dimensional visible‐light capsule enclosing perfect supersized darkness via antiresolution

Supersized darkness in three dimensions surrounded by all light in free space is demonstrated theoretically and experimentally in the visible regime. The object staying in the darkness is similar to staying in an empty light capsule because light just bypasses it by resorting to destructive interference. A binary‐optical system is designed and fabricated based on achieving antiresolution (AR), by which electromagnetic energy flux avoids and bends smoothly around a nearly perfect darkness region. AR remains an unexplored topic hitherto, in contrast to the super‐resolution for realizing high spatial resolution. This novel scheme replies on smearing out the point spread function and thus poses less stringent limitations upon the object's size and position since the created dark (zero‐field) area reach 8 orders of magnitude larger than λ² in cross‐sectional size. It functions very well with arbitrarily polarized beams in three dimensions, which is also frequency scalable in the whole electromagnetic spectrum.