有机液芯光纤拉曼谱测量的研究

我们选用CCl4和CS2混合溶液作为芯液制作了有机液芯光纤,采用后向泵浦的方式测量了光纤的拉曼光谱.实验中发现,随着溶质浓度和光纤长度的变化,拉曼谱强度也随之变化,并存在溶质最佳浓度和最佳光纤长度,这与理论分析值相符,并发现随着溶质浓度的降低,拉曼光谱线宽变窄.     

二波混频高功率单频窄线宽光纤激光器

设计并制造了一种基于二波混频的高功率单频窄线宽光纤激光器.激光器采用长线形腔结构,以Er3+/Yb3+双包层光纤作为增益介质,利用输出信号光分束反馈注入,与腔内振荡激光混频干涉,形成分布的增益光栅与折射率光栅共同作用选模,获得稳定的1550.63 nm单频高功率激光输出.在975 nm多模激光二极管(LD)抽运下,激光...     

多光束激光远场干涉实验研究

设计了多组多孔径光阑,将激光扩束后通过自制的多孔径光阑,获得多光束相干激光光源.基于多光束干涉理论,通过改变不同的光阑,得到多组点状阵列分布的远场干涉图样,结果表明远场中心主瓣具有随着占空比减小能量降低、旁瓣增多的分布规律.实验结果表明,相干源呈正三角形分布时能量集中度较好.对高功率激光相干合成具有一定的参考意义.     

活塞激光热负荷应力场数值模拟

活塞激光热负荷就是通过光学转光片改变激光在空间的能量分配比例.结合活塞激光热负荷试验工况,建立了活塞激光热负荷应力场模拟数学物理模型,模型中考虑了材料的热物性参数随温度的变化.结果表明:由于活塞顶凹坑位置靠近通油孔,导致其应力波动幅值比激光辐照区域大;活塞凹坑、通油孔和靠近活塞顶面的活塞内腔由于和冷却介质直接接触,是活...     

新的Schiff碱-双(2,3-二甲氧基苯甲醛)缩联苯胺的合成与光谱研究

以2,3-二甲氧基苯甲醛和联苯胺为原料,在无水甲醇溶剂中合成了一种新的Schiff碱,收率为86.0%.反应的最佳条件是2,3-二甲氧基苯甲醛与联苯胺的比例为3:1,反应时间为1h,反应温度为30℃.这种新的Schiff碱结构利用IR和UV光谱表征.     

Correlation between Al2O3 particles and interface of Al-Al2O3 coatings by cold spray

Al-Al₂O₃ composite coatings with different Al₂O₃ particle shapes were prepared on Si and Al substrate by cold spray. The powder compositions of metal (Al) and ceramic (Al₂O₃) having different sizes and agglomerations were varied into ratios of 10:1 wt% and 1:1 wt%. Al₂O₃ particles were successfully incorporated into the soft metal matrix of Al. It was found that crater formation between the coatings and substrate, which is typical characteristic signature of cold spray could be affected by initial starting Al₂O₃ particles. In addition, when the large hard particles of fused Al₂O₃ were employed, the deep and big craters were generated at the interface between coatings and hard substrates. In the case of pure soft metal coating such as Al on hard substrate, it is very hard to get proper adhesion due to lack of crater formation. Therefore, the composite coating would have certain advantages.     

基于BF3正比管的宽量程脉冲中子探测技术

介绍了一种基于BF3正比计数管的宽量程脉冲中子探测技术。该技术采用多通道、组合式的BF3管阵列中子探测器组,以适应产额变化范围较宽的脉冲中子测试场合,并同时兼顾测量下限。基于该技术研制了一套BF3阵列中子探测系统并应用于脉冲中子源的测试,实验结果表明,该系统的脉冲中子测量范围可达5个数量级(56~8106),测量下限低、输出信号清晰,证明了该技术的可行性和有效性。     

用于实时三维成像的双频结构光编解码方法

对三维重建中的实时性问题进行了研究,提出一种新的结构光双频测量方法。首先,投影光栅将基频正弦图案和高频正弦图案结合在一起,并保留一张图片作为直流分量,高频图案用于得出鲁棒性较好的高频相位信息,基频图案得出基频相位,并对高频相位进行展开,共5幅图片。其次,用相应的解码方法计算每一像素点的相位,滤除噪声干扰,得到照相机与投影仪的对应关系。最后,根据相位计算出每一采样点的三维坐标,实现三维重建。实验结果表明：计算得到的相位误差的方差为5.559 110-6 rad2,扫描时间为0.156 3 s,在保证实时性的同时有相对较高的精度。对表面深度变化复杂的物体进行三维测量,验证方法的可行性。相比较于传统的双频测量方法,本方法将投影图片数量减小到5幅的同时保持了较好的精度,可应用于扫描动态物体。     

Ultra-intense femtosecond super-heavy ion beams driven by a multi-PW laser

The paper reports the results of numerical studies on the laser-driven acceleration of super-heavy ions by a multi-PW laser pulse of ultra-relativistic intensity attainable with the Extreme Light Infrastructure lasers currently being built in Europe. Using a multi-dimensional (2D3V) particle-in-cell code, it is shown that multi-GeV super-heavy (thorium) ion beams with an intensity of $～{10}^{21}\text{–}{10}^{22}\text{W}/{\text{cm}}^2$, fluence $～{10}^{17}\text{–}{10}^{18}{\text{cm}}^{?2}$ and time duration $～20\text{–}100\text{fs}$ can be produced from a sub-μm thorium target irradiated by a 150-J, 20-fs laser pulse with an intensity of ${10}^{23}\text{W}/{\text{cm}}^2$. Such ion beams are impossible to obtain presently with the use of conventional RF-driven accelerators, so they can open the door to new areas of research in both nuclear and high energy-density physics.     

The Three Processes of Phase II – I Transformation of Isotactic Polybutene-1

The spontaneous transformation of the unstable tetragonal phase II to the stable twined hexagonal phase I of isotactic polybutene – 1 at room temperature and atmospheric pressure was shown to proceed by one of three different mechanisms with these mechanism being neutral (N), increasing (P) or decreasing (M) the phase transformation rate. The rate was shown to be influenced by environmental effects. The environment can increase or decrease the phase transformation rate and, to a smaller extent, influence the sample crystallinity and the amount of the residual, untransformed phase II. The transformation rate was principially affected by the segmental mobility, increased by solvents or decreased by some chemical compounds or groups (e.g.–CH₂-CH₂ – as a comonomer). The transformation rate of the M process starts after an induction period during which the transformation nuclei are blocked.