光学超材料的制备方法与参数提取

在光学超材料研究过程中,其微观结构的控制制备技术至关重要。综述了国内外在光学超材料制备方法方面的大致发展历程。重点介绍了二维光学超材料的制备技术,并分析对比了各种经典制备方法的优缺点。在二维光学超材料制备方法基础上,进一步叙述了三维光学超材料的传统制备和新的研究制备方法。简要介绍了均匀介质光学超材料的介电常数、磁导率、折射率和阻抗等有效电磁参数的提取过程。     

ZnO及其掺杂Mn纳米粒子的微乳液法合成

纳米材料的制备是纳米科学发展的基础,微乳液法与传统的制备方法相比具有明显的优势。本文用双微乳液混合法制备纳米ZnO粉末,通过实验从ZnSO4和NaCO3制备纳米粒子,同时采用在制备过程中掺杂Mn2+,讨论对其性质的改变的影响,并采用荧光发射分析和XRD表征。     

Mo-Fe催化下SWCNTs制备中温度窗口的研究

本文以Mo1-Fe10-MgO为催化剂, Ar为载气, CH4为碳源, 在不同的温度下制备SWCNTs。利用显微激光拉曼研究了不同的制备温度对生成SWCNTs的质量的影响, 得到制备SWCNTs的温度窗口, 给出最佳制备温度。     

催化裂解CH4制备碳纳米管的影响因素

以柠檬酸法制备的Fe MgO、Co MgO和Ni MgO为催化剂 ,CH4 为碳源气 ,H2 为还原气 ,在 873、973和 10 73K制备出碳纳米管 ,通过TEM和拉曼光谱表征 ,讨论了催化剂、制备温度、反应时间等因素对碳纳米管形貌、产率和内部结构的影响 .结果表明 :不同的催化剂在相同的温度下制备的碳纳米管的形态和内部结构有很大的差异 .其中Fe MgO催化剂制备的碳纳米管管径粗 ,且大小不均匀 ,而Ni MgO催化剂制备的碳纳米管管径较细、较均匀 .碳纳米管的产率随着裂解温度的变化而改变 .Fe MgO催化剂制备碳纳米管的产率随制备温度的升高而提高 ,而Ni MgO催化剂制备碳纳米管的产率随制备温度的升高而降低 .Fe MgO催化剂制备碳纳米管 ,在10 73K甚至更高的制备温度才能达到其最高产率 .Co MgO催化剂制备碳纳米管的产率在 973K左右产率较高 ,而用Ni MgO催化剂制备碳纳米管 ,则在 873K甚至更低的制备温度就能达到最高产率 .反应时间与碳纳米管的产率不成正比 ,有一最佳反应时间 ,如Ni MgO催化剂的最佳反应时间为 2h .     

SiO_2胶体晶体自组装技术

介绍了垂直沉降法和旋涂法制备SiO2胶体晶体,并对两种方法制备的胶体晶体在宏观形貌、微观结构及光子带隙性质进行了比较。采用改进的Stober法在乙醇介质中合成粒径不同、单分散性较好的SiO2微球,用垂直沉积法和旋涂法制备出有序性较好的密排结构的SiO2胶体晶体。宏观照片表明,用旋涂法制备的SiO2胶体晶体经白光照射出现的光柱呈6次对称,而垂直沉降法制备的胶体晶体表面出现条纹。SEM分析表明,选用不同溶剂在同等旋涂工艺下制备SiO2胶体晶体,用乙醇和乙二醇混合溶液作溶剂制备出的SiO2胶体晶体质量最好。透射光谱表明,垂直沉降法所制备的胶体晶体在(111)方向具有明显的光子带隙性质,而旋涂法制备的胶体晶体则不明显。     

化学水浴法和磁控溅射法制备硫化镉薄膜的性能研究

以氯化铵、氯化镉、氢氧化钾和硫脲为反应物采用化学水浴法制备了硫化镉薄膜,为了作对比研究,采用射频磁控溅射以硫化镉为靶材,氩气为溅射气体,制备了硫化镉薄膜。采用X射线衍射、扫描电子显微镜和紫外-可见光光谱仪分别表征了硫化镉薄膜的结构、形貌和光学吸收特性。结果表明,采用以上两种方法制备的硫化镉均具有(002)择优取向,溅射法制备的硫化镉薄膜较致密,薄膜表面较光滑,平均晶粒尺寸在20～30nm;水浴法制备的硫化镉薄膜颗粒尺寸较小,缺陷较多。除了在短波段溅射所得硫化镉薄膜的透过率略差于水浴法所得硫化镉薄膜之外,溅射法制备的硫化镉薄膜的性能整体上优于水浴法制备的薄膜。两种方法制备的硫化镉薄膜的能隙在2.3～2.5eV。     

静电纺丝法制备纳米纤维及其应用进展

静电纺丝技术是采用物理方法制备一维采用纳米纤维的有效方法,它在大规模制备有序的、复杂的一维纳米材料方面具有很强优势。除了制备一维纤维材料外,电纺丝技术还用于制备二维和三维多孔结构的材料。本文分为三部分,首先介绍了静电纺丝技术的原理和方法;然后综述了静电纺丝技术在制备一维材料方面的研究进展,最后列举了静电纺丝技术在生物工程领域的应用。     

黑腔芯轴超精密加工

黑腔制备是间接驱动惯性约束聚变靶制备的重要环节。一般的方法要把金电镀在芯轴上,具体制备工艺步骤包括：车削制作芯轴;用电镀法,在芯轴表面镀上适当厚度的金层;镀金芯轴二次装夹,按要求加工金层;溶掉芯轴,得到金空腔。由此可以看出,芯轴加工作为空腔制备工艺过程的首道加工工序,也是最重要的一道工序。芯轴加工质量决定了空腔制备所能达到的质量上限。因此,国内外都把其作为靶制备的重要环节加以研究。     

快速前处理TFA-MOD制备YBCO超导薄膜的研究

三氟乙酸盐金属有机物沉积(TFA-MOD)方法是制备YBa2Cu3O7(YBCO)超导薄膜最有应用前景的方法之一。采用快速前处理TFA-MOD的方法在LaAlO3单晶基片上生长YBCO薄膜并与常规的TFA-MOD方法进行对比研究。XRD分析表明用快速前处理TFA-MOD方法制备的YBCO薄膜的c轴取向一致性,没有常规的TFA-MOD制备的YBCO薄膜好。SEM的分析表明快速前处理TFA-MOD制备的YBCO超导薄膜表面有孔洞和YBCO(103)取向生长的晶粒,常规方法制备的YBCO薄膜表面比较光滑,孔洞较少。虽然较常规方法制备的薄膜的临界电流密度(JC)低,但超导电性能分析表明,快速前处理方法制备的YBCO薄膜JC达到1mA/cm2以上,且前处理时间大幅缩短,对于提高YBCO薄膜制备的效率非常有效。     

塑料微球表面制备聚乙烯醇涂层研究进展

在聚苯乙烯（PS）-聚乙烯醇（PVA）-碳氢聚合物（CH）三层球的设计中制备PVA涂层的方法主要包括乳液微封装法、炉内成球涂层法、浸(旋)涂法、界面缩聚法及喷涂法等,前三种方法目前最为常用。总结了前三种制备PVA涂层方法的优缺点及目前的研究和制备现状。乳液微封装法适合于500 m以下小尺寸双层球的制备,具有微球成活率高、产品质量较好等优点,但制备过程受人为因素影响较大,且不易制备大直径双层球。炉内成球涂层法也适用于小尺寸双层球的制备,其制备周期短,但液滴发生器的设计苛刻,PVA层的均匀性差,且不易制得较大尺寸的双层球。浸（旋）涂法可制备1000 m以上的大直径双层球,但该方法中影响PVA涂层铺展的因素较多,得到的PVA涂层均匀性较差,且涂层很薄。     

大气压低温氦等离子体射流的诊断研究

为了加快低温氦气等离子体射流的工程化进程,通过自主设计的同轴式介质阻挡放电等离子体射流发生器,在放电频率10 kHz,一个大气压条件下产生了稳定的氦气等离子体射流。通过分析不同工况下的电压电流波形可以发现单纯增加氦气体积流量只能小幅的增加电流脉冲幅值,而对放电时间、电流脉冲数的影响不大。增加放电峰值电压时电流脉冲幅值会得到较大幅度增加。通过发射光谱法对大气压氦气等离子射流的活性粒子种类、电子激发温度、电子密度进行了诊断。结果表明,大气压氦气等离子体射流中的主要活性粒子为He Ⅰ原子、N₂第二正带系、N+₂的第一负带系、羟基（OH）,H原子的巴尔末线系（H_α和H_β）与O原子,这表明虽然该试验中使用的氦气纯度已达99.99%,但其中仍残留有少量的空气,同时放电时大气中的空气会被卷吸到放电空间发生电离。还可以发现,主要活性粒子的相对光谱强度随氦气体积流量的增加及放电峰值电压的增大均呈现上涨的趋势。选用He Ⅰ原子的四条谱线对不同试验工况下的电子激发温度进行了计算,得到大气压氦气等离子体射流的电子激发温度在3 500~6 300 K之间,电子激发温度随放电峰值电压与氦气体积流量的增大总体上呈现上升的趋势。但由于反向电场的存在,某些峰值电压可能会出现电子激发温度下降的情况;根据Stark展宽原理对大气压氦气等离子体射流的电子密度进行了计算,发现电子密度的数量级可达1015 cm-3,同时增大峰值电压与氦气体积流量均可有效的提高射流中的电子密度。这些参数的研究对氦气等离子体射流在工程实际中的应用具有重要意义。     

Active and driven hydrodynamic crystals

Motivated by the experimental ability to produce monodisperse particles in microfluidic devices, we study theoretically the hydrodynamic stability of driven and active crystals. We first recall the theoretical tools allowing to quantify the dynamics of elongated particles in a confined fluid. In this regime hydrodynamic interactions between particles arise from a superposition of potential dipolar singularities. We exploit this feature to derive the equations of motion for the particle positions and orientations. After showing that all five planar Bravais lattices are stationary solutions of the equations of motion, we consider separately the case where the particles are passively driven by an external force, and the situation where they are self-propelling. We first demonstrate that phonon modes propagate in driven crystals, which are always marginally stable. The spatial structures of the eigenmodes depend solely on the symmetries of the lattices, and on the orientation of the driving force. For active crystals, the stability of the particle positions and orientations depends not only on the symmetry of the crystals but also on the perturbation wavelengths and on the crystal density. Unlike unconfined fluids, the stability of active crystals is independent of the nature of the propulsion mechanism at the single-particle level. The square and rectangular lattices are found to be linearly unstable at short wavelengths provided the volume fraction of the crystals is high enough. Differently, hexagonal, oblique, and face-centered crystals are always unstable. Our work provides a theoretical basis for future experimental work on flowing microfluidic crystals.     

电流变液中悬浮颗粒的体积与形状的变化

基于偶极近似 ,运用电极化方法 ,定量研究了电流变液中悬浮颗粒在外电场作用下其体积和形状的变化 ,并计算了其体积和形状的相对变化率 .研究结果表明 :悬浮颗粒的体积和形状的相对变化率均与电场强度的平方成正比 ,并与ER本身的性质有关 .一般情况下 ,颗粒的体积和形状的相对变化率分别为 8.4 %和 12 .5 % ,对总体积变化率的贡献为 1.6 8% .这种变化对于ER系统的电涨和电热都作出了贡献 ,仅当将颗粒当作刚性球时 ,其自由能才与电场强度的平方成正比 .     

Ar/CH4等离子体射流发射光谱诊断研究

为了更加深入的研究大气压条件下Ar/CH₄等离子体射流的放电机理和其内部电子的状态,通过自主设计的针-环式介质阻挡放电结构,在放电频率10 kHz、一个大气压条件下产生了稳定的Ar/CH₄等离子体射流,并利用发射光谱法对其进行了诊断研究。对大气条件下Ar/CH₄等离子体射流的放电现象及内部活性粒子种类进行诊断分析,重点研究了不同氩气甲烷体积流量比、不同峰值电压对大气压Ar/CH₄等离子体射流电子激发温度、电子密度以及CH基团活性粒子浓度的影响规律。结果表明,大气压条件下Ar/CH₄等离子体射流呈淡蓝色,在射流边缘可观察到丝状毛刺并伴有刺耳的电离声同时发现射流尖端的形态波动较大;通过发射光谱可以发现Ar/CH₄等离子体射流中的主要活性粒子为CH基团,C,CⅡ,CⅢ,CⅣ,ArⅠ和ArⅡ,其中含碳粒子的谱线主要集中在400~600 nm之间,ArⅠ和ArⅡ的谱线分布在680~800 nm之间;可以发现CH基团的浓度随峰值电压的增大而增大,但CH基团浓度随Ar/CH₄体积流量比的增大而减小,同时Ar/CH₄等离子体射流中C原子的浓度随之增加,这表明氩气甲烷体积流量比的增大加速了Ar/CH₄等离子体射流中C-H的断裂,因此可以发现增大峰值电压与氩气甲烷体积流量比均可明显的加快甲烷分子的脱氢效率,但增大氩气甲烷体积流量比的脱氢效果更加明显。通过多谱线斜率法选取4条ArⅠ谱线计算了不同工况下的电子激发温度,求得大气压Ar/CH₄等离子体射流的电子激发温度在6 000~12 000 K之间,且随峰值电压与氩气甲烷体积流量比的增大均呈现上升的趋势;依据Stark展宽机理对Ar/CH₄等离子体射流的电子密度进行了计算,电子密度的数量级可达1017 cm-3,且增大峰值电压与氩气甲烷体积流量比均可有效的提高射流中的电子密度。这些参数的探索对大气压等离子体射流的研讨具有重大意义。     

Phase separation and super diffusion of binary mixtures of active and passive particles

Computer simulations were performed to study the dense mixtures of passive particles and active particles in two dimensions. Two systems with different kinds of passive particles(e.g., spherical particles and rod-like particles) were considered. At small active forces, the high-density and low-density regions emerge in both systems, indicating a phase separation. At higher active forces, the systems return to a homogeneous state with large fluctuation of particle area in contrast with the thermo-equilibrium state. Structurally, the rod-like particles accumulate loosely due to the shape anisotropy compared with the spherical particles at the high-density region. Moreover, there exists a positive correlation between Voronoi area and velocity of the particles. Additionally, a small number of active particles capably give rise to super-diffusion of passive particles in both systems when the self-propelled force is turned on.     

Some formulations of light scattering in laser flowmeters employing differential Doppler heterodyning

The theory for the Doppler shifted light is developed by diffraction theory combined with galilean transformation. The theory developed is applied to a differential Doppler heterodyning technique in which two beams are brought simultaneously, but at different angles, into the same area, and the cross region made by the two beams becomes a probing volume. When the concentration of scattering particles is so low that only one particle is found in the probing volume, the theory can be classified into two cases of a single particle and many particles depending on the analysing time for the Fourier transform, i.e. whether the time, during which one particle passes through the probing volume, is longer than the observing time or not. When the concentration of particles in the probing volume becomes dense, the light scattered by the different particles interferes and the theory shows great complexity. The cases of two particles and many particles showing a very high density are studied. Comparisons are made for the difference between differential Doppler heterodyning and normal heterodyning techniques.     

Effective interactions between colloidal particles suspended in a bath of swimming cells

The dynamics of passive colloidal tracers in a bath of self-propelled particles is receiving a lot of attention in the context of nonequilibrium statistical mechanics. Here we demonstrate that active baths are also capable of mediating effective interactions between suspended bodies. In particular we observe that a bath of swimming bacteria gives rise to a short range attraction similar to depletion forces in equilibrium colloidal suspensions. Using numerical simulations and experiments we show how the features of this interaction arise from the combination of nonequilibrium dynamics (peculiar of bacterial baths) and excluded volume effects.     

Mixing and segregation of granular materials in chute flows

Mixing of granular solids is invariably accompanied by segregation, however, the fundamentals of the process are not well understood. We analyze density and size segregation in a chute flow of cohesionless spherical particles by means of computations and theory based on the transport equations for a mixture of nearly elastic particles. Computations for elastic particles (Monte Carlo simulations), nearly elastic particles, and inelastic, frictional particles (particle dynamics simulations) are carried out. General expressions for the segregation fluxes due to pressure gradients and temperature gradients are derived. Simplified equations are obtained for the limiting cases of low volume fractions (ideal gas limit) and equal sized particles. Theoretical predictions of equilibrium number density profiles are in good agreement with computations for mixtures of equal sized particles with different density for all solids volume fractions, and for mixtures of different sized particles at low volume fractions (nu<0.2), when the particles are elastic or nearly elastic. In the case of inelastic, frictional particles the theory gives reasonable predictions if an appropriate effective granular temperature is assumed. The relative importance of pressure diffusion and temperature diffusion for the cases considered is discussed. (c) 1999 American Institute of Physics.     

浓悬浮液中渗透性颗粒的扩散特性研究

本文利用浓悬浮液中渗透性颗粒的短时扩散动力学数值模拟的结论,并结合Cohen-de Schepper近似和Percus-Yevick近似,研究了不同粒径渗透性颗粒的有效扩散系数随体积分数和渗透率的变化关系. 结果表明:对于浓悬浮液中一定粒径的渗透性颗粒,其扩散系数随渗透率的增加而增加,随体积分数的增加而减少;具有相同粒径与流体动力学屏蔽深度比值且波数较大的渗透性颗粒,其粒径对扩散的影响可以忽略. 关键词： 渗透性颗粒 有效扩散系数 体积分数 布朗运动短时区域     

Formation mechanisms of colloidal silica via sodium silicate

Colloidal silica is formed by titrating active silicic acid into a heated KOH with seed solution. The colloidal silica formation mechanisms are investigated by sampling the heated solution during titration. In the initial stage, the added seeds were dissolved. This might due to the dilution of seed concentration, the addition of potassium hydroxide (KOH) and the heating at 100°C. Homogenous nucleation and surface growth occur simultaneously in the second stage of colloidal silica formation. Homogenous nucleation is more important when the seed concentration is relatively low. On the other hand, surface growth plays an important role when the seed concentration is increased. In the middle seed concentration, the seed particles grow up and some new small particles are born by the homogenous nucleation process to form a bimodal size distribution product. As the titrating volume of active silicic acid exceeds a specific value in the last stage the particle size increases rapidly and the particle number decreases, which may be caused by the aggregation of particles. The intervals between each stage were varied with the seed concentration. Increasing the seed concentration led to the formation of uniform particle size colloidal silica.