LD抽运高重复频率四通放大MOPA系统中的光纤相位共轭研究

报道了利用多模光纤作为相位共轭镜应用于重复频率100Hz。脉宽20ns的电光调Q四通放大LD抽运激光器的实验研究。由于光纤受激布里渊散射(SBS)存在的阈值效应，可以抑止使用平面全反镜的四通放大系统中难以克服的放大级自振荡(SO)和放大自发辐射(ASE)效应．以获得高能量高光束质量的激光输出。实验中在20ns．100Hz和注入光纤能量4．6mJ的情况下获得了4．1mJ的1064nm的基模激光输出。激光光束模式接近TEMoo模．且脉宽被压缩至4．7ns。在使用了光纤相位共轭镜的四通放大技术后，很好地补偿了由板条放大器热效应造成的光斑畸变。输出光斑很好地复原了振荡级输出光斑的光强空间分布。     

A highly rigid diamine monomer derived from naturally occurring myo‐inositol and its use for polyamide synthesis

A rigid diamine was synthesized from myo‐inositol, a naturally occurring cyclic hexaol, and used as a monomer to synthesize polyamides. myo‐Inositol was treated with 1,1‐dimethoxycyclohexane to yield a bisketal bearing two hydroxyl groups, and from this bisketal, the target diamine was synthesized in three steps: (1) derivation of the diol into the corresponding bistriflate, (2) nucleophilic substitution of the bistriflate with sodium azide yielding a diazide, and (3) reduction of the diazide to the target diamine. The target diamine readily underwent polycondensation with dicarboxylic acid chloride in solution. The resulting polyamides, whose main chain inherited the rigid 5‐6‐5 system from the diamine monomers, have high glass transition temperatures. © 2016 Wiley Periodicals, Inc. J. Polym. Sci., Part A: Polym. Chem. 2016 , 54, 3436–3443     

Interpolation inequalities with weights

We use elementary methods to prove a sufficient and necessary condition for a Sobolev interpolation inequalities with weight [ILLM0001] where [ILLM0001] are real numbers, and [ILLM0001]     

基于QN旋转布局的10位500 MS/s分段电流舵DAC

针对分段电流舵数/模转换器（Digital-to-Analog Converter，DAC），通过理论分析和推导，研究电流源阵列系统失配误差和寄生效应对非线性的影响，采用电流源阵列Q^N旋转游走版图布局方案，能够减小电流源系统失配的一次误差，而且版图布线简单，由寄生效应引起的电流源失配较小，利于DAC非线性的优化.基于0.18μm CMOS，采用"6+4"的分段结构，设计了一种10位500MS/s分段电流舵DAC，流片测试结果表明，在输入频率为1.465MHz，采样速率为500MS/s的条件下，无杂散动态范围（Spurious Free Dynamic Range，SFDR）为64.9dB，有效位数（Effective Number of Bits，ENOB）为8.8 bit，微分非线性误差（Differential Non-linearity，DNL）和积分非线性误差（Integral Non-linearity，INL）分别为0.77LSB和1.12LSB.     

Kolmogorov Type Law of the Logarithm for Arrays

In this paper, we establish the analogue of Kolmogorov-type law of the logarithm for an array of independent random variables. The main methods are to develop the classic Bernstein’s and Kolmogorov’s inequality and replace the boundedness condition by conditions on the cumulant transform.     

多孔活性自燃金属的光谱辐射特性研究

多孔活性金属材料因为内部存在大量的孔隙，大大地增加了与空气的接触面积，使得其在空气中的燃烧较为猛烈，燃烧温度迅速上升。其燃烧过程属于固体燃烧的范畴，较为复杂。以镁为例，通过建立燃烧模型，来研究多孔活性金属的光谱辐射特性。首先，建立氧气总消耗量与活性金属剩余质量的关系，研究氧气在活性金属孔隙内的扩散浓度关系，通过求解活性金属热平衡方程得到活性金属燃烧过程中温度与时间的关系式，进而得到活性金属的峰值光谱辐射强度表达式；然后，将模型计算的仿真结果与红外热像仪测得的实验结果对比，结果表明，模型的计算结果与实验结果相一致，误差在了10%以内；最后，通过建立的燃烧模型来研究活性金属燃烧规律以及其光谱辐射特性，解决了高空、高速下的活性金属光谱辐射强度难以实验获得的问题，大大减小了实验成本与时间。分别对比不同时间活性金属箔片在1～3，3～5以及8～12 μm波段下的辐射强度，得出活性金属燃烧时的辐射强度主要集中在3～5 μm波段的结论。研究结果表明：自燃金属最大燃烧温度随高度的增加逐渐下降，随气流速度的增加先增加后减小，在速度为30 m·s-1时，温度达到最大；自燃金属的光谱辐射强度在2～6 μm波段达到最大。该模型也可以用来研究其他活性金属的燃烧特性。     

基于变异的紧凑遗传算法在农药检测中的应用

为了简化农药检测的预测模型,提高模型预测精度,采用红外光谱技术结合基于变异的紧凑遗传算法对波长变量进行筛选,一定程度上减少了无信息变量和干扰变量。通过不同算法选择的波长变量建立预测模型,mCGA得到的预测均方根偏差平均值是0.198,而与mCGA比较的紧凑遗传算法、简单遗传算法得到的预测均方根偏差平均值分别为0.241、0.289,mCGA具有最小误差。结果表明,采用mCGA进行变量选择,能有效提高模型收敛速度及模型准确度,实现农药含量快速高效的检测。     

Performance of CO-OFDM system with RS-Turbo concatenated code

In this paper, the RS-Turbo concatenated code is applied to coherent optical orthogonal frequency division multiplexing (CO-OFDM) system. RS(186,166,8) and Turbo code with code rate of 1/2 are employed for RS-Turbo concatenated code. Two decoding algorithms, which are Max-Log-MAP algorithm and Log-MAP algorithm, are adopted for Turbo decoding, and the iteration Berlekamp-Massey (BM) algorithm is adopted for RS decoding. The simulation results show that the bit error rate (BER) performance of CO-OFDM system with RS-Turbo concatenated code is significantly improved at high optical signal to noise ratio (OSNR), and the iteration number is reduced compared with that of the Turbo coded system. Furthermore, when the Max-Log-MAP algorithm is adopted for Turbo decoding, the transmission distance of CO-OFDM system with RS-Turbo concatenated code can reach about 400 km without error, while that of the Turbo coded system can only reach about 240 km when BER is lower than 10-4 order of magnitude.