晶格振动和热电子对疏松金属材料冲击压缩特性的贡献

 根据固体晶格的谐振子模型、热电子的自由电子气模型以及Grüneisen物态方程，仅通过简洁的代数运算分别导出晶格振动、热电子对疏松金属材料的冲击温度、冲击压强、乃至压缩体积贡献的计算公式。结果表明：晶格振动对冲击压缩体积的贡献分量计算公式与吴-经方程的推导结果在形式上具有很好的一致性，同时改进了热电子对体积贡献分量的计算公式。并论证了两个体积贡献分量表达式的合理性及其物理意义。     

球面角锥棱镜非稳腔钕玻璃激光器

为了将虚共焦非稳腔输出光束质量高和角锥棱镜谐振腔具有免调试的优点结合到一起,提出了用球面角锥棱镜构成虚共焦非稳腔的方案。利用已有虚共焦非稳腔钕玻璃激光器,设计加工了一球面角锥棱镜非稳腔钕玻璃激光器。模拟计算了两谐振腔输出光束的模式分布,然后对两钕玻璃激光器进行了实验对比研究。结果表明:实验得到的模式分布与模拟计算结果相吻合,球面角锥棱镜非稳腔钕玻璃激光器与虚共焦非稳腔钕玻璃激光器分别获得了最大2176.9J和2340.6J的能量输出,二者的电光效率与束散基本相同,分别为4.3%,0.30mrad和4.6%,0.26mrad。     

基于环形光束整形的衍射光学元件的精确设计

提出一种改进的Gerchberg-Saxton(G-S)算法,实现了基于环形光束的衍射光学元件的精确设计。所提算法可以确保输出平面上有小的采样间隔,起到了抑制散斑的作用;与未采用散斑抑制的常规的改进G-S算法相比,所提算法得到了更高性能的均匀光斑;仿真结果和实验结果一致。     

等离子体初始密度对激光支持爆轰波特性的影响

采用守恒元求解元方法,对描述激光支持爆轰波等离子体流场演化的二维轴对称流体动力学控制方程组进行了数值模拟计算,给出了不同时刻点的等离子体压强、密度、温度、速度及对激光吸收系数的空间分布,比较了初始密度不同的情况下等离子体演化的不同特点。计算结果表明,等离子体初始密度较大时,等离子体对激光的吸收系数较大,为了增强激光能量与靶面的耦合,应合理控制靶面等离子体密度、激光脉宽及脉冲间隔。     

A Direct Comparison between Static and Dynamic Melting Temperature Determinations below 100 GPa

A preliminary experiment of sound velocity measurements for porous iron with initial average density of 6.275 g/cm^3 has been performed at pressures below 100 CPa, in order to clarify a long-standing problem that the static melting temperature Tin, mostly below 100CPa due to its technical limitations, is notably lower than the extrapolated melting data inferred from the shock wave experiments made above 200 CPa, for the sake of making a direct comparison between the experimental static and dynamic melting temperatures in the same pressure region. With the lately proposed Hugoniot sound velocity data analysis technique [Chin. Phys. Left. 22 (2005) 863], the results deduced from this Hugoniot sound velocity measurement is Tm = 3200 K at 87 CPa and Tm = 3080 K at 80 GPa, which are in good agreement with the two latest static data of Tm = 3510 K at 105 GPa and Tm = 2750 K at 58 GPa, which utilized modern improved double-side laser heating and in situ accurate x-ray diffraction techniques in experiments. It can be concluded that consensus Tm data would be obtained from static and shock wave experiments in the case that the recently improved techniques are adopted in investigations.