增益竞争双波长放大单频光纤放大器理论研究

引入增益竞争是抑制单频光纤放大器中受激布里渊散射(SBS)的有效方式. 在单频光纤放大器的基础上, 推导了描述增益竞争双波长放大单频掺镱双包层光纤放大器的稳态速率方程组, 建立了增益竞争双波长放大单频光纤放大器的理论模型; 利用建立的理论模型模拟分析了信号光波长间隔、 信号光种子功率比、 抽运方式和增益光纤长度等因素对放大器的单频激光输出 效率以及SBS抑制效果的影响.     

飞秒激光成丝过程中由等离子体光栅引起的超连续谱增强与转移

在飞秒宽带激光脉冲成丝过程中, 由于双光束干涉效应而形成的空间等离子体光栅, 研究了空气中飞秒宽带激光脉冲成丝所产生的超连续谱增强效应, 并进一步观测到泵浦光脉冲成丝产生的超连续谱能量向较弱的未成丝的探测光脉冲转移, 有效拓展探测光脉冲带宽的新现象. 通过基于布拉格衍射特性的理论计算较好地解释了实验结果.     

Can we reach very high intensity in air with femtosecond PW laser pulses?

In the course of femtosecond pulse filamentation in atmospheric density gases, the peak intensity is always limited by optical-field-induced ionization. This intensity clamping phenomenon is universal in all the cases we studied, namely, single and multiple filament regimes with and without external focusing using pulses of up to subpetawatt level. Even in the tight focusing cases, the clamped intensity along the propagation direction does not exceed 30% of the global intensity maximum. The remarkable shot-to-shot stability of the clamped intensity (better than 1% of the maximum value) is revealed both experimentally and numerically in a single filament regime in air.     

Relation between chaos probability and zero-point number of the Melnikov function for a Bose-Einstein condensate

We investigate an attractive Bose-Einstein condensate perturbed by a weak traveling optical superlattice. It is demonstrated that under a stochastic initial set and in a given parameter region solitonic chaos appears with a certain probability that is tightly related to the zero-point number of the Melnikov function; the latter depends on the potential parameters. Effects of the lattice depths and wave vectors on the chaos probability are studied analytically and numerically, and different chaotic regions of the parameter space are found. The results suggest a feasible method for strengthening or weakening chaos by modulating the potential parameters experimentally.      

X波段高功率微波对介质窗材料的破坏现象

 在X波段微波源（频率9.4 GHz,功率1 GW）下,对4种典型介质窗材料（聚四氟乙烯、有机玻璃、低密度聚乙烯及高密度聚乙烯）在真空中进行了微波放电击穿实验,同时考虑了材料的不同表面处理工艺（表面刻槽和抛光）对其击穿特性的影响,对微波击穿后样品的表面形貌进行了宏观和微观分析,实验观测到:介质表面出现了沿微波电场方向的明显树枝状破坏现象,且材料表面处理工艺对其击穿破坏程度有显著影响,认为树枝状破坏通道与施加的微波场有着密切的关系。通过观察透明有机玻璃内部的树枝状破坏,发现树枝既沿介质表面生长,同时也向介质内部发展。提出了微波作用下介质窗击穿破坏的物理模型,认为微波电场导致树枝状破坏沿电场方向发展,而微波磁场导致树枝状向介质内部发展,并进一步给出了树枝状破坏起始和发展的可能原因。     

高精度有限差分法模拟Kelvin-Helmholtz不稳定性

 WENO有限差分格式有较高的分辨精度,适合复杂流场的计算,在国际上被广泛采用。本文利用WENO有限差分格式求解2维守恒型欧拉方程,实现了对无粘流体中Kelvin-Helmholtz不稳定性的数值模拟。速度剪切方向采用周期边界条件;扰动增长方向采用嵌边出流边界条件,一个不稳定波长分布64个网格。数值模拟给出的扰动幅值线性增长率与线性稳定性分析给出的结果很好符合,显示了该格式的有效性和精度。数值模拟给出了清晰的密度等值线,表明该方法还具有较好的界面变形捕捉能力。     

Fiber optic acoustic emission sensor and its applications in the structural health monitoring of CFRP materials

A fiber optic acoustic emission sensor based on fused-tapered coupler and its applications in structural health monitoring are proposed in this paper. The fiber optic acoustic emission sensor (FOAES) was tested using pencil lead break tests compared with the commercial acoustic emission sensor (R15 PZT). Besides, the sensor was embedded into the carbon fiber reinforced plastics (CFRP) materials and tested in the same way. It successfully detected the AE signals. FOAES was applied in the structural health monitoring (SHM) of CFRP materials. Damages of carbon fiber/epoxy composite laminates during three-point-bending test were monitored by surface-mounted and embedded FOAES, respectively. Results identified that the sensor embedded into composite structures could monitor damage of composite laminates on-line as the surface-mounted sensor did.     

凸体的宽度不等式及应用

该文建立了关于单形宽度的杨路、张景中不等式的一个逆不等式. 作为凸体宽度不等式的应用,得到了凸体的截面和投影的一些估计式.     

一个Mini Max定理和一类二阶Hamiltont系统的解的唯一性5

推广了Stepan A．Tersian的关于g（u）=2^-1（Au，u）-Ф（u）型泛函的一个Mini Max定理．利用这一推广了的MiniMax定理，研究了一类受迫振动下二阶Hamilton系统的边界值问题的解，获得了这类二阶Hamilton系统边界值问题的解的一个唯一性定理．     

1,3-Di­chloro-1,1-di­methyl-3,3-diiso­propyl­distannoxane

The title compound, [Sn₄(CH₃)₄(C₃H₇)₄Cl₄O₂] or {Cl[(CH₃)₂CH]₂SnOSn(CH₃)₂Cl}₂, obtained by the reaction of [(CH₃)₂CH]₂SnO and (CH₃)₂SnCl₂, exists as centrosymmetric dimers in the solid state. It contains a central planar four-membered Sn₂O₂ ring. The coordinate geometry about the Sn atoms is distorted trigonal pyramidal.