用光学记录速度干涉仪测量自由面速度

 建立了一套光学记录速度干涉仪系统(ORVIS),用于测量强激光产生的冲击波状态方程中的自由面速度。该光学记录速度干涉仪系统的时间分辨率为179 ps,可以测量自由面速度随时间变化的整个过程。在天光KrF高功率准分子激光装置上进行激光打靶实验,激光波长248.4 nm,脉冲宽度25 ns,最大输出能量158 J。在激光功率密度为6.24×10¹¹W·cm^-2的条件下,测得厚20 μm铁膜的自由面速度可达3.86 km/s;在激光功率密度为7.28×10¹¹W·cm^-2条件下,100 μm铝膜（靶前有100 μm的CH膜作为烧蚀层）的自由面速度可以达到2.87 km/s。     

压缩映射定理的相关结论

文中主要探讨了压缩映射定理的相关结论,并给出了这些结论的证明.     

液体弹珠及其研究进展

润湿性是固体表面的重要性质之一,主要由表面的化学组成和微观几何结构共同决定。不粘连表面是指具有特殊的表面形貌及性能,使得诸如尘土、水、冰以及污染物较难黏附的特殊表面。液体弹珠是被高疏水性颗粒包裹形成的不润湿的液滴,可以稳定地静置于固体及液体表面。本文介绍了液体弹珠的结构和制备方法,综述了液体弹珠的静态力学性能及其在磁场电场下的响应性能,探讨了这种新型不粘连体系用于移动和控制微量液滴的独特优势,展望了其发展趋势以及应用前景。     

干摩擦引起自激振动现象研究

对干摩擦引起自激振动现象进行分析,得到了其解析表达式,对振动过程进行了详细的分析,画出了振动曲线和相图,说明这就是弦弓乐器发出优美声乐的物理原因.     

Partial evolution based local adiabatic quantum search

Recently, Zhang and Lu provided a quantum search algorithm based on partial adiabatic evolution, which beats the time bound of local adiabatic search when the number of marked items in the unsorted database is larger than one. Later, they found that the above two adiabatic search algorithms had the same time complexity when there is only one marked item in the database. In the present paper, following the idea of Roland and Cerf [Roland J and Cerf N J 2002 Phys. Rev. A 65 042308], if within the small symmetric evolution interval defined by Zhang et al., a local adiabatic evolution is performed instead of the original “global” one, this “new” algorithm exhibits slightly better performance, although they are progressively equivalent with M increasing. In addition, the proof of the optimality for this partial evolution based local adiabatic search when M=1 is also presented. Two other special cases of the adiabatic algorithm obtained by appropriately tuning the evolution interval of partial adiabatic evolution based quantum search, which are found to have the same phenomenon above, are also discussed.     

Al掺杂ZnO纳米粉体的EPR谱研究

采用溶胶凝胶方法制备了Al掺ZnO纳米粉体.并用X射线衍射仪(XRD)和电子顺磁共振(EPR)对样品进行表征.结果表明:Al以替位形式掺入ZnO,未改变原有结构,掺杂Al离子浓度为2;时,其结晶性最好.Al掺杂ZnO粉末在g=1.96和2.00处具有明显信号峰.g=1.96位置的信号是制备过程中产生的Zn-H键的信号位置,该信号与ZnO导电特性有密切关系;g=2.00是晶体中锌空位对应的信号.g=1.96处信号峰强度与煅烧时间的长短无关;煅烧时间越长越有利于晶体结构的完善,减少空穴的产生;Al的掺入不仅替代了部分Zn的位置,也填补了部分的锌空位;温度变化起到了和Al离子同样的功效,Al离子的掺入增强了温度变化对ZnO的影响.     

不同宽厚比H形截面钢梁抗冲击性能

基于经实验校核的非线性有限元模型,对受横向冲击作用的H形钢梁进行了有限元分析。设计不同宽厚比组配的H形钢梁,分析H形钢梁跨中受横向冲击的动态响应和应力发展过程,并研究宽厚比对H形钢梁抗冲击性能的影响,重点讨论了腹板厚度、翼缘厚度对冲击力平台值和峰值以及耗能的影响。分析结果表明,两端铰接H形钢梁在跨中受冲击载荷作用下的变形模式主要为弯曲变形。相同冲击能量下,冲击力平台值主要受翼缘厚度的影响,冲击力峰值主要受腹板厚度的影响。翼缘厚度对钢梁抗冲击性能的影响要大于腹板厚度。本研究可为不同宽厚比H形钢梁的抗冲击设计提供依据和参考。

     

Study of the double rectangular waveguide grating slow-wave structure

A slow-wave structure (SWS) with two opposite gratings inside a rectangular waveguide is presented and analysed. As an all-metal slow-wave circuit, this structure is especially suited for use in millimetre-wave travelling wave tubes (TWTs) due to its advantages of large size, high manufacturing precision and good heat dissipation. The first part of this paper concerns the wave properties of this structure in vacuum. The influence of the geometrical dimensions on dispersion characteristics and coupling impedance is investigated. The theoretical results show that this structure has a very strong dispersion and the coupling impedance for the fundamental wave is several tens of ohms, but the coupling impedance for --1 space harmonic wave is much lower than that for the fundamental wave, so the risk of backward wave oscillation is reduced. Besides these, the CST microwave studio is also used to simulate the dispersion property of the SWS. The simulation results from CST and the theoretical results agree well with each other, which supports the theory. In the second part, a small-signal analysis of a double rectangular waveguide grating TWT is presented. The typical small-signal gain per period is about 0.45 dB, and the 3-dB small-signal gain bandwidth is only 4\%.     

采用双层靶提高激光薄膜相互作用中加速质子的产额

 在激光等离子体相互作用实验中测量到的加速质子,来源于薄膜靶表面的碳氢沾染物。为了提供稳定充足的质子源,设计一种新的复合靶,在2.5 μm塑料溅射200 nm 金薄层形成双层靶,并在中等强度激光功率密度下开展研究,采用磁谱仪和CR-39探测器测量得到其能谱,结果表明：双层靶结构能够有效地增加质子的产额,并可能改善加速质子束的单能性。     

外加气流法制备微相结构有序的PS-b-PEO嵌段共聚物薄膜

采用原子转移自由基聚合(ATRP)的方法合成了聚苯乙烯-聚环氧乙烷(PS-b-PEO)嵌段共聚物,并利用核磁共振波谱(1H-NMR)、傅里叶变换红外光谱(FTIR)以及凝胶渗透色谱法(GPC)对聚合物进行了表征.利用外加气流法制备了具有不同形貌的嵌段共聚物薄膜,并讨论聚合物分子组成、气流温度、气流速度以及不同基底对薄膜表面形貌以及内部结构的影响.当嵌段共聚物中聚苯乙烯嵌段的质量分数为83%~85%,气流温度为30~50℃,气流速度3~5 m/s时,有利于形成表面垂直柱状微相分离结构.当硅基底的接触角小于90°时,在合适的外加气流场作用下可以形成薄膜的表层和底层垂直有序而薄膜内部无序的非对称结构.