大气光通信中大气闪烁时间平滑效应研究

利用大气闪烁的时间平滑效应,增加光电探测器曝光时间是克服大气闪烁对大气光通信的瞄准、捕获、跟踪链路影响的有效途径之一.基于科尔莫戈罗夫谱,导出了弱湍流起伏区无限平面波和球面波的大气闪烁时间平滑因子的一般表达式,并且用几何光学近似得到了在大孔径和小孔径接收情况下的时间平滑因子近似表达式.在孔径远大于菲涅耳区尺度时,平面波和球面波的时间平滑因子的近似表达式与精确表达式的误差分别小于6%和3%.分析结果表明,孔径越小,时间平滑效应越显著,并且菲涅耳区尺度对时间平滑效应影响的程度也随着孔径的增加而减弱.     

耦合微盘及带输出波导的单微盘腔的耦合模式特性

光学微腔具有很高的品质因子和很小的模式体积,在光电子器件研究方面具有重要的应用价值.运用时域有限差分(FDTD)法和Padé近似频谱分析法模拟研究了耦合微盘及带输出波导的单微盘微腔由于空间对称性破坏导致的模式耦合现象;特别计算了耦合模式的场分布和品质因子,并由场分布得出不同角量子数模式的能量比例.对耦合微盘,模式耦合引...     

基于EEMs及PARAFAC的洪湖、东湖与梁子湖CDOM组成特征分析

国内外关于长江中下游地区如洪湖、东湖及梁子湖等大中型浅水湖泊DOM组成特征的分析较少,本文基于2007年9月—10月洪湖、东湖与梁子湖34个站点野外实地采样数据,运用三维荧光图谱(EEMs)与平行因子分析(PARAFAC)模型,着重分析了三个湖泊CDOM吸收荧光特性及组成特征。结果表明,CDOM在350 nm处吸收系数a(350)在三个湖泊表现为洪湖极显著高于东湖与梁子湖(p<0.001);三个湖泊CDOM光谱斜率S_280～500与a(350)呈极显著负相关(R2=0.781, p<0.001)且洪湖S_280～500值极显著低于东湖与梁子湖(p<0.01);光谱斜率比值S_R值也表现为洪湖显著低于东湖与梁子湖(p<0.05)。PARAFAC模型解析得到两个类腐殖质组分(C1, C2),两个类蛋白质组分(C3,C4),其中组分C1与C2呈极显著正相关(R2=0.884,p<0.001),组分C3与C4亦为极显著正相关(R2=0.677,p<0.001),这表明三个湖泊CDOM组分C1与C2,C3与C4来源相似,然而统计结果并未发现四个荧光组分与DOC及Chl-a浓度之间存在任何显著性相关关系。三个湖泊荧光指数FI₂₅₅(HIX),FI₂₆₅,FI₃₁₀(BIX)与FI₃₇₀值均表现为东湖显著高于梁子湖(p<0.05),极显著高于洪湖(p<0.01),这意味着东湖富营养化程度高于洪湖与梁子湖。     

Gd2(WO4)3: Eu纳米发光材料中黄昆因子和能量传递速率的实验获得

采用共沉淀法制备了不同Eu³⁺掺杂浓度的Gd₂(WO₄)₃纳米发光材料. 测量了纳米材料样品的X射线衍射谱(XRD) 和场发射扫描电镜, 对样品的结构和形貌进行了表征. 测量了各样品的发射光谱和激发光谱(声子边带光谱), 绘制了浓度猝灭曲线, 确定了最佳的掺杂浓度为20 mol%. 通过声子边带光谱计算了不同掺杂浓度样品的黄昆因子. 测量了不同浓度样品的荧光寿命, 利用Auzel模型对Eu^{3+ 5}D₀能级荧光寿命数据进行了拟合, 确定了⁵D₀能级的固有寿命和猝灭过程中生成的声子数. 本文还根据荧光寿命数据计算了Eu³⁺之间的能量传递速率, 确定了能量传递速率与浓度的关系. 关键词： 钨酸盐 3+')" href="#">Eu³⁺ 黄昆因子 能量传递速率     

分形烟尘簇团粒子的消光特性研究

根据物质的电结构,将烟尘簇团粒子离散为一系列的偶极子,利用离散偶极子近似方法,获得了不同波长电磁波入射情况下分形烟尘簇团粒子不对称因子、吸收和散射效率因子的值.结合偶极子在电磁场中的力学性质,分析了烟尘簇团粒子在外加电磁场中所受的力和力矩,给出三种分形结构烟尘簇团粒子的电磁辐射压力及电磁辐射力矩效率因子随入射波波长变化的数值结果,分析了烟尘粒子对电磁能量吸收的宏观表现和微观机理.结果显示:入射波长、烟尘簇团粒子的分形维数及所含原始微粒数目都将影响烟尘粒子的消光特性.     

太赫兹波导滤波器的分析与设计

分析了不同宽边情况下对滤波器加工精度的影响,分析结果表明对于不同频段的滤波器,需要选择合适的谐振腔的宽边才能达到较好的性能,同时分析了不同谐振模式的滤波器对加工精度的影响,分析表明,对于太赫兹频段滤波器,选用TE101谐振模式时存在腔体长度会比波导的宽边小很多的情况,而选用高阶谐振模式不但可以提高滤波器的品质因数Q值,减少损耗,同时也能在一定程度上降低滤波器对加工精度的要求。最后以0.34 THz 4阶带通滤波器为例验证此方法的正确性,测试表明该滤波器最低损耗为-0.73 dB,在0.335~0.349 THz范围内损耗在-2 dB以内。     

水平微细圆管内膜状凝结换热特性的研究

实验研究了微细圆管内凝结换热特性,实验中采用四种不锈钢管,其内径范围为289-997μm。基于实验结果, 分析了换热温差、蒸汽进口雷诺数Rein和管径对管内膜状凝结换热系数的影响,发现温差对管内膜状凝结换热的影响很小, Nu随蒸汽进口雷诺数Rein增加而增大,随管径减小而降低,而对流换热系数随管径减小而显著增大。     

The use of the isotropic orientation factor in fluorescence resonance energy transfer (FRET) studies of the actin filament

A Dale-Eisinger style analysis (R. E. Daleet al., Biophys. J. 26, 161, 1979) is used to produce three-dimensional plots that display the limits on the average orientation factor k ² that is required to calculate molecular distances in F-actin from fluorescence resonance energy transfer measurements. Maxima and minima plots are generated for the transfer of energy from a donor to a single acceptor and for transfer to multiple acceptors that are related by F-actin helical symmetry. The analysis is performed in terms of dipole cone half-angles rather than depolarization factors, in order to facilitate the modeling of the multiple acceptor problem. Calculations are carried out under the restrictive condition of a single electric dipole moment per fluorophore. In addition, both surface and volume averaging of the donor and acceptor dipoles are considered. Comparisons between the plots show that for the multiple acceptor cases with F-actin symmetry, there is a great reduction in the range for maxima and minima limits on k ². The calculations also suggest guidelines for the choice of fluorescence label that will result in an average orientation factor occurring within acceptable limits, i.e., inside the limits for which k ²=2/3 may be employed. Thus, without having detailed knowledge of the mean donor or acceptor dipole relative orientations, the use of k ²=2/3 in radial coordinate studies of F-actin is more than reasonable and is fairly assured of being correct.     

Rescaled mean spherical approximation structure factor for an aqueous suspension of polystyrene spheres

Rescaled mean spherical approximation (RMSA) has been used to calculate the structure factor for the aqueous suspension of polystyrene macroions with the interaction potential taken according to Derjaguin and Landau (1941) and Verwey and Overbeek (1948) (DLVO) model. The effects of charge over the macroion and size on the surface potential and therefore, the structure factor have been studied. The breakdown of the DLVO potential with an excess charge over the macroion (⩾800e) has been reported. The oscillation in the first peak height of structure factor versus wave vector curve with size has been correlated with the Debye length.     

Nuclear spin–spin constants,rotational g factor and susceptibility of sulphur hexafluoride

Following our previous study on spin–rotation and shielding constants of the SF₆ molecule, the rotational g factor and the magnetic susceptibility are calculated here, using ab initio methods to evaluate the electronic contribution to the nuclear hyperfine constants, and compared with experimental results. It is shown, for the first time, that the electronic component of the rotational g factor is proportional to a constant, which is given by a sum over electronic states. We also evaluate for the SF₆ molecule the indirect, or electron-coupled spin–spin interaction, theoretically described by Ramsey, and show that it gives non-negligible corrections to direct coupling constants d ₁ and d ₂. The contributions of the terms included in this interaction (DSO, PSO, SD and FC) are also analysed.