非对称电极表面微观形貌对交流电渗流速的影响

经典交流电渗理论是利用电场进行非机械式微流体驱动的基础.传统理论交流电渗理论以双电层理论为基础,通过耦合电场方程以及流场方程得到微电极表面交流电渗流速表达式,通常与实验流速相差较大. 以电极表面微观形貌对交流电渗流速的影响为研究目标,定义微电极表面粗糙度为微观形貌特征参数,建立了等效双电层模型,并对传统交流电渗流速公式进行了修正.理论并仿真分析了表面粗糙度对于交流电渗流速的影响,利用非对称电极对交流电渗微流体驱动进行了实验研究,并进行对比分析.结果表明,理论分析与实验结果具有较好的一致性. 关键词： 交流电渗 电极表面粗糙度 等效双电层     

铁电相变中极化与介电性的随机场效应

基于随机场Ising模型描述的有序无序相变中偶极子在电场作用下的反转运动, 研究了有序无序相变过程中电场与极化强度的关系. 认为tanh(x) 的函数关系与位移型二阶铁电相变极化强度随电场变化的实验结果完全相同. 由此得出基本结论: 偶极子的集体转向造成了极化强度的增大并等同于内电场的增加. 通过区分光学模和偶极子对介电隔离率的贡献, 考虑偶极子极化对介电常数复数形式的频率色散关系, 发现从高斯分布的居里温度可以导出二阶铁电相变过程中介电常数与温度和频率的色散关系. 关键词： 铁电相变 极化强度 随机场     

微系统中转矩及电渗流作用下的微粒子电动旋转操控

微粒子的电动旋转操控是表征分散系中微粒子介电特性的有效方法.低雷诺数微系统中,以Maxwell-Wagner极化理论为基础,进行了转矩作用下的微粒子电动旋转机理研究,推导了此机理作用下微粒子电动旋转峰值速度所对应的特征频率,分析了弛豫时间对粒子旋转方向的影响,对转矩作用下的微粒子电动旋转速度进行仿真;以双电层理论为基础,对电渗流导致的微粒子电动旋转机理进行定性分析,提出具有金修饰的粒子表面更适合电渗流作用下的电动旋转研究.分别以羧基修饰的聚苯乙烯微球以及表面被金修饰的聚苯乙烯微球为操控对象,进行电动旋转实 关键词： 微系统 电动旋转 转矩 电渗流     

Dielectric Analysis of Dynamic Fouling Behavior on Surface of Polyethersulfone Composite Ultrafiltration Membrane

基于界面极化与静电场理论建立了聚醚砜复合超滤膜表面污染层与溶液体系的介电解析模型. 应用参数敏感性分析和介电测量研究了体系中浓差极化层与滤饼层的厚度与电导率对超滤体系介电弛豫的影响机制. 结果表明超滤过程中浓差极化层能快速建立,而滤饼层的形成是一个增长与剥蚀的动态过程;并且浓差极化层与滤饼层的电学性质是影响超滤体系介电谱的关键因素. 比较介电测量与模拟结果证实了建立的超滤体系介电解析模型能够有效可靠地描述与解释超滤体系产生介电驰豫的机制.     

直流电场作用下油中水滴的破裂时间特征

采用显微实验与理论分析相结合的方法,对直流电场作用下水滴破裂前的拉伸过程及其时间特征进行了系统研究。结果表明,电毛细数和表面活性剂浓度是影响水滴拉伸过程的关键因素,而油水黏度比和电导率比的影响并不显著。拉伸时间对低电毛细数和高表面活性剂浓度体系更为敏感。在实验范围内,直流电场作用下球形水滴经拉伸并破裂的最小时间为10 ms。基于此,提出了一种可有效提高水滴静电聚并效率并抑制电分散现象的脉冲电场设计方法。     

一种基于超材料的宽带、反射型90°极化旋转体设计

根据各向异性媒质理论, 设计了一种宽带、反射型超材料极化旋转体, 能够将线极化波极化方向旋转90°, 极化转化率大于90%的工作带宽为5.5–14.5 GHz. 该极化旋转体由两层介质板、金属双开口谐振环和金属底板周期排列构成, 具有各向异性的特点, 单元两对角线方向的电场分量反射系数相同, 反射相位相差180°, 导致其极化旋转特性. 利用表面电流分布图, 分析不同极化波入射时该极化旋转体的谐振状态, 实验和仿真结果符合较好. 该极化旋转体在新型天线设计和隐身技术等方面具有广阔的应用前景.     

电导率对电流变效应的影响

通过实验和理论分析，证明电导率对直流电场下电流变效应的产生及对其大小的决定作用．电流变机制不仅包括体极化和界面极化过程，而且包括离子的双电层极化过程．低频或直流电场下，显著电流变效应的体系要求σ_p＞σ_f，且ε_p＞ε_f．适当地增大σ_f，提高离子层的静电作用，有利于提高电流变液体的流变性能，但这种做法应以不引起电流过大、焦耳热过多、电功输入过大为前提 关键词：     

基于方形开口环的超宽带线性极化转换器

电磁波的极化调控在卫星通信、雷达探测以及立体显示成像等领域有重要的应用价值,探索易于加工、转换效率高、工作频带宽的高性能极化转换器具有重要的研究意义.本文提出了一种基于方形开口环超构表面的线性极化转换器,该转换器具有各向异性特点,反射电场沿两个对角线方向的分量振幅相等,相位相差180°,导致在反射模式下能够将入射波的极化方向旋转90°.实验测试结果表明,在7.12—18.82 GHz频带范围内极化转换率高于90%,相对带宽达到90%.频带的显著拓宽基于四个谐振频点,每个谐振频点的转换效率都接近100%.实验结果与模拟结果相符合,验证了提出的超构表面可以在较宽的频带范围内实现电磁波的90°极化旋转.     

指数掺杂GaAs光电阴极量子效率的理论计算

将GaAs光电阴极发射层掺杂浓度由体内到发射表面从高到低的进行指数掺杂，能在发射层形成一个恒定的内建电场，有利于光电子的逸出.在考虑内建电场的作用下，通过建立和求解少数载流子所遵循的一维连续性方程，得到了反射式和透射式指数掺杂阴极的量子效率公式，并利用这些公式对其量子效率进行了理论计算和仿真.计算结果显示发射层指数掺杂能较明显的提高阴极的量子效率，与均匀掺杂阴极相比，能使反射式阴极积分灵敏度提高约20%，透射式阴极提高30%以上.指数掺杂提高阴极量子效率的主要原因与内建电场有关，光电子在内建电场作用下以扩散加漂移的方式到达阴极表面，从而减小了后界面复合速率对阴极的影响，同时提高了阴极的等效电子扩散长度. 关键词： 指数掺杂 内建电场 能带结构 量子效率     

共轭高聚物中极化子散射引起的激子迁移(英文)

基于Su-Schrieffer-Heeger(SSH)模型并考虑到Brazovskii-Kirova对称破缺项,研究了共轭聚合物中注入极化子和激子在外电场下的散射过程.研究发现在外场作用下极化子总是能通过激子,而激子的运动行为则密切依赖于电场的强度.如果电场大于临界电场3.0×10~5V/cm,那么激子与极化子散射后并不发生任何运动;然而当电场小于此临界值时,激子将在极化子运动的相反方向上有一个明显的位移.激子在弱电场下所发生的这种迁移运动,是由于同极化子发生了慢散射作用.     

Automatic microcircuit formation based on gold-coated SU-8 microrods via dielectrophoresis

To explore the application of the characteristics of metallic microparticles, alternating current electric trapping of the SU-8 microrods coated with a thin gold layer by the chemical approach is investigated. Positive dielectrophoresis is used to absorb the gold-coated SU-8 microrods at the edge of the parallel electrodes, thereby forming chains to connect the electrodes. This is a fast automatic microcircuit formation process. Moreover, a non-charged molecule is modified on the surface of the gold-coated SU-8 microrod, and the modified microrods are controlled by the alternating electric field to form a number of chains. The different chains between the parallel electrodes consist of various parallel circuits. In order to compare these chains with different electric surfaces, the impedances of the metallic and modified microrods are measured and compared, and the results show that the gold-coated microrods act as pure resistors, while the microrods functionalized by a non-charged molecule behave as good capacitors.     

石墨烯对ZnO微米棒光学特性的影响

采用化学气相沉积(CVD)方法制备了具有良好结晶质量和(002)择优取向的ZnO微米棒。在此基础上,选取单根ZnO微米棒,将其部分搁置于单层石墨烯表面。光致发光(PL)谱结果表明,石墨烯不仅增强了ZnO微米棒的紫外发光强度,同时也对光场在ZnO微米棒中的分布有很大的限域作用。分析认为这是由于石墨烯的表面等离子效应引起了ZnO微米棒与石墨烯之间的光-物质相互作用导致的。在拉曼(Raman)光谱中,石墨烯对ZnO微米棒的E2(L)声子振动模和E2(H)声子振动模的强度具有明显的减弱效应,这进一步证明二者之间存在光子的传输和电荷的转移,从而导致其晶格振动受到抑制。     

Electric-field-induced polarization of the layer of condensed ions on cylindrical colloids

In concentrated suspensions of charged colloids, interactions between colloids can be induced by an external electric field through the polarization of charge distributions (within the diffusive double layer and the layer of condensed ions) and/or electro-osmotic flow. In case of rod-like colloids, these field-induced inter-colloidal interactions have recently been shown to lead to anomalous orientation perpendicular to the external field, and to phase/state transitions and dynamical states, depending on the field amplitude and frequency of the external field. As a first step towards a (semi-) quantitative understanding of these phenomena, we present a linear-response analysis of the frequency-dependent polarization of the layer of condensed ions on a single, long and thin cylindrical colloid. The in-phase and out-phase response functions for the charge distribution and the electric potential are calculated for arbitrary orientation of the cylindrical colloid. The frequency-dependent degree of alignment, which is proportional to the electric-field-induced birefringence, is calculated as well, and compared to experiments on dilute fd virus suspensions.     

Metal particle polarization

The effect of electron collisions with lattice atoms in metals on metal particle polarization in an ac electric field was analyzed. It was shown that, in contrast to collisionless (free) electron gas, an increase in the negative electronic permittivity with decreasing electric field frequency in relaxation metal particles is limited by the conductivity relaxation time. It was shown that the plasma frequency appears in relaxation metal only if the dielectric relaxation time is less than the free path time in metal.     

Second-harmonic generation from a thin spherical layer and No-generation conditions

The dispersion of the electro-optical effect in polydisperse hydrosols of diamond is studied in the external field frequency ranging from 10 Hz to 2.5 MHz. The conservative dichroism, which is determined by the difference in the turbidity constants for light polarized along and perpendicular to the particle-orienting field, is chosen as the electro-optic effect. The dispersion dependences of the dichroism are determined and used to calculate the dispersion of the average values of the polarizability anisotropy of the diamond particles. The influence of the concentration of monovalent ions in an aqueous KCl solution on these dispersion dependences is studied. The experimental dependences of the dispersion are compared with the theoretical ones within the model of the polarizability of the colloidal particles which takes into account the polarizability of the diffuse part of their double electric layer.     

波导内场增强法测量微波气体击穿

 提出并研究了波导内场增强法测量微波气体击穿的实验方案,在密闭波导内加金属针实现电场增强,通过调节微波源辐射功率及两针距离,使微波传输达到气体击穿的条件。介绍了实验原理及诊断方法,进行了频率2.86 GHz、脉宽180 ns的微波在0.1 MPa空气中的击穿实验,分析了实验中得到的典型波形。结果表明实验现象与设计吻合,验证了该方案研究微波气体击穿的可行性。     

Electronic States and Schottky Barrier Height at Metal/MgO(100) Interfaces

Using an ab initio total energy approach, we study the electronic structure of metal/MgO(100) interfaces. By considering simple and transition metals, different adsorption sites and different interface separations, we analyze the influence of the character of metal and of the detailed interfacial atomic structure. We calculate the interface density of states, electron transfer, electric dipole, and the Schottky barrier height. We characterize three types of electronic states: states due to chemical bonding which appear at well defined energies, conventional metal-induced gap states associated to a smooth density of states in the MgO gap region, and metal band distortions due to polarization by the electrostatic field of the ionic substrate. We point out that, with respect to the extended Schottky limit, the interface formation yields an electric dipole mainly determined by the substrate characteristics. Indeed, the metal-dependent contributions (interfacial states and electron transfer) remain small with respect to the metal polarization induced by the substrate electrostatic field.     

Electric double layer of anisotropic dielectric colloids under electric fields

Anisotropic colloidal particles constitute an important class of building blocks for self-assembly directed by electrical fields. The aggregation of these building blocks is driven by induced dipole moments, which arise from an interplay between dielectric effects and the electric double layer. For particles that are anisotropic in shape, charge distribution, and dielectric properties, calculation of the electric double layer requires coupling of the ionic dynamics to a Poisson solver. We apply recently proposed methods to solve this problem for experimentally employed colloids in static and time-dependent electric fields. This allows us to predict the effects of field strength and frequency on the colloidal properties.     

Mechanism for far infrared absorption of small metallic particles

A mechanism for far infrared absorption of small particles of noble metals is described. The electric double layer formed at the particle surface allows excitation of the resonant low frequency mode in which the metal core oscillates rigidly with respect to the shellof adsorbed atoms. The model is capable of explaining the large magnitude and the anomalous frequency dependence recently reported for Pt particles.