五元体系Li~ /Cl~-,CO_3~(2-),SO_4~(2-),B_4O_7~(2-)-H_2O298K相关系实验研究

青藏高原盐湖富含锂、钠、钾的氯化物、硫酸盐、碳酸盐和硼酸盐,尤以其高锂、硼而闻名于世[1]。这些盐湖卤水大多属于Li ,Na ,K ,Mg2 /Cl-,SO42-,CO32-,Borate-H2O体系。在卤水蒸发浓缩后期,由于绝大部分钠盐、钾盐均已结晶析出,所以卤水的化学组成实际变成Li ,Mg2 /Cl-,SO42-,     

分光棱镜干涉法测量涡旋光束拓扑荷

理论分析并实验研究了涡旋光束通过单分光棱镜后的自干涉现象.研究结果表明,不同于涡旋光束与平面波或者球面波干涉,涡旋光束自干涉条纹呈"扭曲"状,且在干涉条纹边缘处会出现"断裂"条纹,其数目随着涡旋拓扑荷数增大而增大,且"断裂"条纹的指向与拓扑荷符号相关.上述结论提供了一种原理和操作简单的测量涡旋光束拓扑荷数的方法.     

The interaction of in-band and in-gap lattice soliton trains in optically induced two-dimensional photonic lattices

We demonstrate the coherent interactions of lattice soliton trains,including in-band solitons (IBSs) and gap soliton trains (GSTs),in optically induced two-dimensional photonic lattices with self-defocusing nonlinearity.It is revealed that the π-staggered phase structures of the lattice soliton trains will lead to anomalous interactions.Solely by changing their initial separations,the transition between attractive and repulsive interaction forces or reversion of the energy transfer can be obtained.The 'negative refraction' effect of the soliton trains on the interaction is also discussed.Moreover,two interacting IBSs can merge into one GST when attraction or energy transfer happens.     

双零色散光子晶体光纤中超连续谱的产生及控制

 通过数值模拟飞秒脉冲在具有双零色散波长的光子晶体光纤中的传输过程,详细分析了超连续谱的产生和控制机制.结果表明：中心波长处于反常色散区的泵浦脉冲在高阶非线性和高阶色散等作用的调制下,将演化为基孤子和正常色散区的两个色散波|该色散波进而经与之相位匹配的基孤子相干加强而使频谱展宽形成超连续谱,同时两个色散波上出现了干涉引起的振荡现象.进一步对比三种结构的光子晶体光纤中超连续谱的特点,定量分析了两色散波对超连续谱的限制作用,阐述了结构参量对超连续谱的影响.基于上述结论,结合对色散波的中心波长与光子晶体光纤的色散曲线、结构参量之间关系的分析,提出了设计光子晶体光纤的结构来控制超连续谱的方法.作为例证,通过优化光子晶体光纤结构理论上实现了频谱分量覆盖可见光区的平坦超连续谱.     

水热沉淀法制备掺铁二氧化钛中空球及其光催化性能

 以碳球为模板剂, 采用水热沉淀法制备了不同配比掺 Fe 的 TiO2 (Fe-TiO2) 中空球, 并运用 X 射线粉末衍射、扫描电子显微镜、元素分析能谱、红外光谱和热重等方法对其进行了表征. 结果表明, 中空球为锐钛矿相, 大小为 0.5~3.20 ?m, 壳层厚度为 30~60 nm, 比表面积为 150~300 m2/g. 随着 Fe 掺杂量的增加, 中空球在可见光区的吸收强度逐渐增加. 光催化降解实验表明, 掺 Fe 后, TiO2 中空球的可见光催化活性升高, 其中 0.5% Fe-TiO2 在 80 min 内降解亚甲基蓝超过 75%. 同时还讨论了光催化机制.     

Entropy resistance analyses of a two-stream parallel flow heat exchanger with viscous heating

Heat exchangers are widely used in industry, and analyses and optimizations of the performance of heat exchangers are important topics. In this paper, we define the concept of entropy resistance based on the entropy generation analyses of a one-dimensional heat transfer process. With this concept, a two-stream parallel flow heat exchanger with viscous heating is analyzed and discussed. It is found that the minimization of entropy resistance always leads to the maximum heat transfer rate for the discussed two-stream parallel flow heat exchanger, while the minimizations of entropy generation rate, entropy generation numbers, and revised entropy generation number do not always.     

A comparison of different entransy flow definitions and entropy generation in thermal radiation optimization

In thermal radiation, taking heat flow as an extensive quantity and defining the potential as temperature T or the black body emissive power U will lead to two different definitions of radiation entransy flow and the corresponding principles for thermal radiation optimization. The two definitions of radiation entransy flow and the corresponding optimization prin ciples are compared in this paper. When the total heat flow is given, the optimization objectives of the extremum entransy dissipation principles （EEDPs） developed based on potentials T and U correspond to the minimum equivalent temperature difference and the minimum equivalent blackbody emissive power difference respectively. The physical meaning of the definition based on potential U is clearer than that based on potential T, but the latter one can be used for the coupled heat transfer optimization problem while the former one cannot. The extremum entropy generation principle （EEGP） for thermal radiation is also derived, which includes the minimum entropy generation principle for thermal radiation. When the radiation heat flow is prescribed, the EEGP reveals that the minimum entropy generation leads to the minimum equivalent thermodynamic potential difference, which is not the expected objective in heat transfer. Therefore, the minimum entropy generation is not always appropriate for thermal radiation optimization. Finally, three thermal radiation optimization examples are discussed, and the results show that the difference in optimization objective between the EEDPs and the EEGP leads to the difference between the optimization results. The EEDP based on potential T is more useful in practical application since its optimization objective is usually consistent with the expected one.     

羟基磷灰石对氟离子的吸收作用

用基准NaF配置标准溶液,用氟离子选择性电极测定氟离子的标准曲线,将自制的羟基磷灰石(HAP)粉体放入三组不同配方的NaF溶液浸泡,测定HAP在吸收氟离子的过程中溶液的pH值和氟离子浓度的变化,并利用XRD、TEM、EDS等对吸附氟离子的HAP粉体进行检测.结果表明,HAP对氟离子的吸附动力学相对于Lagergren拟一级速率方程,更符合Lagergren拟二级速率方程,线性相关系数R2为1.降低pH值可以提高氟离子吸收率,HAP在吸收氟离子的同时释放出大量的氢氧根,提高了溶液的pH值.吸收氟离子后粉末晶体的XRD图谱的测试结果与FAP的图谱相一致,微观结构相近均为棒状结构,EDS结果表明粉体晶体结构中掺杂了大量的氟离子,得到的粉末晶体为FAP.     

拼接式光学窗口装配关键技术研究

对拼接式光学窗口组件的结构特点作了介绍,分析了影响拼接式光学窗口性能的主要装配因素,并从装配齐平性及微应力装调两个方面出发,开展了装配关键技术研究,通过计算分析及参数量化工艺措施解决装调技术难题,获得了装配后外形齐平性≤0.2 mm,装配后应力≤50 nm/cm的高精度、微应力装调效果,满足光学分辨率及高速飞行使用要求。     

Graphene integrated photodetectors and opto-electronic devices — a review

Graphene and other two-dimensional materials have recently emerged as promising candidates for next-generation,high-performance photonics. In this paper, the progress of research into photodetectors and other electro-optical devices based on graphene integrated silicon photonics is briefly reviewed. We discuss the performance metrics, photo-response mechanisms, and experimental results of the latest graphene photodetectors integrated with silicon photonics. We also lay out the unavoidable performance trade-offs in meeting the requirements of various applications. In addition, we describe other opto-electronic devices based on this idea. Integrating two-dimensional materials with a silicon platform provides new opportunities in advanced integrated photonics.